[CP2K-user] [CP2K:18582] large fluctuations of the dipole moment

Wei Chen chenweiitp at gmail.com
Tue Mar 28 03:06:00 UTC 2023


Dear CP2K users,

I am trying to calculate the dipole moment of BCC iron. But I got large 
fluctuations of the dipole moment based on the periodic (Berry phase) 
operator CP2K_INPUT/FORCE_EVAL/DFT/PRINT/MOMENTS.   I tried different 
reference points, but it does not help.

The full input file, atomic coordinates and output file are all attached. 

Thank you very much for your help!

Best wishes,

Wei

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  Reference Point [Bohr]              1.35258825      1.35258825      1.35258825
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.65734552 Y=  -15.96809240 Z=   13.00941301     Total=    22.74838729
  Reference Point [Bohr]              0.16907491     -0.00000011     -0.16907361
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.97645478 Y=   -2.42971024 Z=    6.36052015     Total=     6.87845712
  Reference Point [Bohr]              0.16908217      0.00000091     -0.16907778
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.07686806 Y=   27.43087861 Z=  -17.99064285     Total=    34.62388391
  Reference Point [Bohr]              0.16909178      0.16906679     -0.00001651
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.13150262 Y=  -15.20157414 Z=  -26.55829930     Total=    32.91814810
  Reference Point [Bohr]              0.33817322      0.16903796     -0.00004762
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.42620252 Y=   22.94592470 Z=  -19.63340082     Total=    30.87526465
  Reference Point [Bohr]              0.33817795      0.33805675     -0.00010380
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.24390582 Y=    7.83653571 Z=    4.17235624     Total=    16.78418009
  Reference Point [Bohr]              0.33818893      0.33798037     -0.16925815
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.88140619 Y=   16.83336939 Z=   17.21165368     Total=    24.09108185
  Reference Point [Bohr]              0.33821474     -0.00025230     -0.33843260
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.08851855 Y=  -13.17772913 Z=   -5.51395402     Total=    30.62423993
  Reference Point [Bohr]              0.33824854      0.16873489     -0.33853982
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.64993674 Y=   -8.75538683 Z=   -2.79151324     Total=    23.51954731
  Reference Point [Bohr]              0.16919606      0.16864888     -0.00049394
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.61772343 Y=   17.16787474 Z=  -12.57854777     Total=    34.08018467
  Reference Point [Bohr]              0.16919241      0.16856134     -0.16964880
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.35720829 Y=   -5.06915335 Z=   13.90618665     Total=    16.10876904
  Reference Point [Bohr]              0.16917167      0.16847212     -0.00062959
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.40482519 Y=  -23.59526559 Z=   -7.46688037     Total=    24.86511703
  Reference Point [Bohr]              0.00007137      0.16837595     -0.00067133
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.59586953 Y=  -12.29259590 Z=   -2.64983295     Total=    26.73751273
  Reference Point [Bohr]              0.00004101     -0.00080871     -0.00072892
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.98115659 Y=   19.34211808 Z=    5.72836334     Total=    24.54392833
  Reference Point [Bohr]              0.00000010     -0.00093276     -0.00081862
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.27585844 Y=   -3.67975898 Z=    7.29960265     Total=     8.80659262
  Reference Point [Bohr]             -0.33820792     -0.00105628      0.16815452
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.20958329 Y=  -21.09151908 Z=   10.06313491     Total=    23.58856262
  Reference Point [Bohr]             -0.33829680     -0.17023752      0.16806713
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.58860872 Y=    7.40201499 Z=    8.31778059     Total=    11.69843632
  Reference Point [Bohr]             -0.33841863     -0.17032984      0.16798320
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.69282339 Y=  -19.30269105 Z=    3.35089587     Total=    19.66438496
  Reference Point [Bohr]             -0.33856820     -0.17041592      0.16787011
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.50305498 Y=  -16.65733585 Z=  -25.63815526     Total=    30.77423008
  Reference Point [Bohr]             -0.50779662     -0.17047864     -0.17044052
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.82445763 Y=   21.42025209 Z=   -3.35690947     Total=    24.23354955
  Reference Point [Bohr]             -0.50793257     -0.33956474     -0.17064356
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.35770457 Y=   17.98105106 Z=    9.54315766     Total=    30.98342166
  Reference Point [Bohr]             -0.50805673     -0.17045760     -0.17086299
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.99151314 Y=   -8.79349330 Z=    9.74731521     Total=    23.91644363
  Reference Point [Bohr]             -0.33912236     -0.17041059     -0.17108987
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.06375468 Y=    7.49696478 Z=  -17.20316473     Total=    31.31046401
  Reference Point [Bohr]             -0.33927656     -0.17038139     -0.00225053
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.96216707 Y=   23.64447467 Z=   -4.41644578     Total=    26.43360139
  Reference Point [Bohr]             -0.33942192     -0.17037603     -0.00249738
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.96228252 Y=  -19.36786297 Z=   26.18073217     Total=    35.43289695
  Reference Point [Bohr]             -0.17047804     -0.17037909     -0.00275385
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.70668828 Y=    4.74632255 Z=   -0.63408944     Total=    24.18546498
  Reference Point [Bohr]             -0.17059982     -0.33945531     -0.17207034
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.56829418 Y=   -3.50278236 Z=   -0.87866381     Total=     6.63682412
  Reference Point [Bohr]             -0.00165181     -0.33946780     -0.00320146
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.93812704 Y=  -23.20190343 Z=   23.55584771     Total=    33.78378148
  Reference Point [Bohr]             -0.00180089     -0.17043127     -0.00337051
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.20273967 Y=  -16.57831375 Z=   21.42250981     Total=    28.60864958
  Reference Point [Bohr]             -0.00198801     -0.17050174     -0.00352623
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.72874681 Y=   16.17406797 Z=   -9.06636213     Total=    24.31445811
  Reference Point [Bohr]             -0.00220251     -0.17060516     -0.00368956
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.99491396 Y=   20.69726629 Z=  -15.80270579     Total=    26.21205547
  Reference Point [Bohr]             -0.34057702     -0.17072674     -0.00386729
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.87222043 Y=   25.16624880 Z=   20.77298061     Total=    35.45836011
  Reference Point [Bohr]             -0.34079954     -0.17084888     -0.00404364
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.33575347 Y=    1.77332281 Z=    8.95318180     Total=    22.29006521
  Reference Point [Bohr]             -0.34100926     -0.17096035     -0.00420071
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.42932325 Y=  -22.62355306 Z=  -25.62132497     Total=    34.46587226
  Reference Point [Bohr]             -0.34121171     -0.17105003     -0.00434251
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.07692325 Y=    9.05246051 Z=   27.08297996     Total=    28.84538348
  Reference Point [Bohr]             -0.34141362     -0.17110536     -0.00448483
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.19900310 Y=   15.23104418 Z=  -27.00363443     Total=    31.43581735
  Reference Point [Bohr]             -0.34163265     -0.17111982      0.16444642
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.18992650 Y=   -9.29051126 Z=  -27.17731602     Total=    34.54234191
  Reference Point [Bohr]             -0.34188386     -0.17109554      0.16431790
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.79973902 Y=   18.94231614 Z=   -1.44876060     Total=    22.90728196
  Reference Point [Bohr]             -0.17307632     -0.17102867      0.16420123
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.33756357 Y=   17.01677941 Z=   -3.88213358     Total=    23.23537387
  Reference Point [Bohr]             -0.17333719     -0.17092566      0.16408328
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.93592561 Y=   12.33344749 Z=   -6.23906913     Total=    21.86013464
  Reference Point [Bohr]             -0.00451870     -0.17080360      0.16395581
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.05077135 Y=   18.14086290 Z=  -13.02457614     Total=    24.48976307
  Reference Point [Bohr]             -0.00474969     -0.17066285      0.16382349
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.19445851 Y=   19.01561026 Z=  -14.06661445     Total=    27.08425393
  Reference Point [Bohr]             -0.00492678     -0.17048503      0.16370008
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.45262817 Y=   22.97735058 Z=    9.64756452     Total=    28.80820373
  Reference Point [Bohr]             -0.00504685     -0.17026166      0.16359522
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.03594094 Y=   27.33374233 Z=    5.82136488     Total=    31.27346154
  Reference Point [Bohr]             -0.00513638     -0.17002342      0.16351293
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.95647484 Y=    3.50776049 Z=    2.97733279     Total=    11.88331751
  Reference Point [Bohr]             -0.00522468     -0.16979466      0.16345714
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.55694655 Y=    6.98263681 Z=    1.80587841     Total=    10.44633212
  Reference Point [Bohr]             -0.00532256     -0.16957246      0.16342884
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.15810623 Y=  -17.09786953 Z=    2.19370675     Total=    30.49720972
  Reference Point [Bohr]             -0.00542943     -0.16934566      0.16342110
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.58698206 Y=  -15.99148903 Z=  -27.16374258     Total=    37.11127186
  Reference Point [Bohr]             -0.00555474     -0.16911218      0.16341405
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.27285293 Y=  -16.90539634 Z=   20.19352124     Total=    28.64695339
  Reference Point [Bohr]              0.16336302     -0.16889039      0.16339091
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.59080136 Y=   10.03834186 Z=   15.35011788     Total=    22.82770921
  Reference Point [Bohr]              0.16318887     -0.16868886      0.16335458
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.67332890 Y=   10.71087107 Z=   13.54145022     Total=    21.41744379
  Reference Point [Bohr]              0.16302338      0.00057108      0.16331982
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.36809694 Y=  -16.96554496 Z=  -14.28523635     Total=    25.89601725
  Reference Point [Bohr]              0.16288246      0.00073389     -0.00576920
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.99729618 Y=  -19.06907070 Z=    7.88600016     Total=    22.92955270
  Reference Point [Bohr]              0.16277042      0.00087983     -0.00575840
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.62356499 Y=    4.05056428 Z=  -10.41625180     Total=    27.04117833
  Reference Point [Bohr]              0.33175475     -0.16805294     -0.17481284
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.70485237 Y=   -0.32331433 Z=   20.08783677     Total=    26.77848980
  Reference Point [Bohr]              0.33166755     -0.16791323     -0.17479820
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.33901547 Y=   -2.52367278 Z=   -4.46387366     Total=    14.29071119
  Reference Point [Bohr]              0.33156967     -0.16776847     -0.17477545
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.54872489 Y=   25.24937932 Z=   -6.55899590     Total=    26.67095670
  Reference Point [Bohr]              0.33146647     -0.16761969     -0.17474521
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.95547937 Y=    0.44404279 Z=   -9.17074523     Total=    15.07425717
  Reference Point [Bohr]              0.33135541     -0.16747954     -0.17472495
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.07583042 Y=  -23.58336742 Z=   -8.13741707     Total=    33.98362437
  Reference Point [Bohr]              0.33122486     -0.16736637     -0.17471298
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.14608126 Y=  -21.54100657 Z=  -26.87973072     Total=    42.06623501
  Reference Point [Bohr]              0.33107515     -0.16727742     -0.17468641
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.94995454 Y=  -19.80170941 Z=  -16.01963214     Total=    32.35331506
  Reference Point [Bohr]              0.33093346     -0.16717725     -0.00556002
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.85151391 Y=  -13.52553346 Z=   16.86382661     Total=    28.03578521
  Reference Point [Bohr]              0.33081969     -0.16704480     -0.00547905
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.71861802 Y=   -2.75094685 Z=   20.16733514     Total=    26.34010827
  Reference Point [Bohr]              0.16164684     -0.16688263     -0.00537053
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.87333969 Y=  -23.97327141 Z=   -5.15645497     Total=    29.76602698
  Reference Point [Bohr]              0.16153967     -0.33577385     -0.00524226
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.83231806 Y=  -20.02609481 Z=   -2.72281917     Total=    27.62452572
  Reference Point [Bohr]              0.16141497     -0.33557890      0.16397540
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.18592544 Y=   10.59390103 Z=  -27.45887194     Total=    40.06613195
  Reference Point [Bohr]             -0.00779915     -0.33536981      0.16413959
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.03640044 Y=  -13.36992280 Z=    1.48495000     Total=    23.30975019
  Reference Point [Bohr]             -0.17702583     -0.33514412      0.16431461
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.91273874 Y=   -6.71601011 Z=  -24.83602682     Total=    27.94675091
  Reference Point [Bohr]             -0.17718930     -0.33490158      0.16447339
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.78939243 Y=   27.32273750 Z=  -23.20697907     Total=    38.40889487
  Reference Point [Bohr]             -0.17736256     -0.33464380      0.16461433
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.41568804 Y=   14.82145947 Z=    5.33843713     Total=    18.88547403
  Reference Point [Bohr]             -0.17754576     -0.33437733      0.16475369
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.28553177 Y=    3.93416171 Z=  -24.48582955     Total=    30.22950687
  Reference Point [Bohr]             -0.00867083     -0.33410517      0.16488141
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.06178645 Y=   -0.38583357 Z=    3.00923722     Total=    10.50923036
  Reference Point [Bohr]             -0.00888042     -0.33381424      0.16497495
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.20687482 Y=   -3.36454269 Z=    2.92313210     Total=    18.74446957
  Reference Point [Bohr]             -0.00908927     -0.33349097      0.16503414
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.26247681 Y=    9.09581407 Z=    0.47733745     Total=    10.51928452
  Reference Point [Bohr]             -0.17835924     -0.33315462      0.16507402
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.42951850 Y=   -3.44677226 Z=   -2.69460207     Total=     9.49725757
  Reference Point [Bohr]             -0.17850881     -0.33282561      0.16511667
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.14310333 Y=   -9.46512788 Z=   18.07664422     Total=    21.61891851
  Reference Point [Bohr]             -0.00951094     -0.33249986      0.16517624
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.10309193 Y=  -12.69965077 Z=   -5.26585695     Total=    24.35456188
  Reference Point [Bohr]              0.15953864     -0.16310719      0.16524156
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.94638676 Y=   14.01770353 Z=   19.21733788     Total=    25.07881875
  Reference Point [Bohr]              0.15952293     -0.16279971      0.33436649
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.98265106 Y=  -11.64317855 Z=   -9.18578407     Total=    16.39206063
  Reference Point [Bohr]              0.15949547     -0.16251033      0.16532501
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.38944704 Y=   20.40951444 Z=   -8.13279235     Total=    22.62159876
  Reference Point [Bohr]              0.15945138      0.00682314      0.16535811
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.40413034 Y=   25.68992815 Z=   22.71143101     Total=    42.08732689
  Reference Point [Bohr]              0.15939034      0.00706469      0.16542076
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.21216694 Y=   24.52619736 Z=   26.33174178     Total=    36.36016592
  Reference Point [Bohr]              0.32840510      0.17639014      0.16551353
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.70897748 Y=    8.21737724 Z=  -13.12293243     Total=    22.77995990
  Reference Point [Bohr]              0.15928263      0.17666805      0.16562448
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.92979993 Y=  -20.12963560 Z=  -10.84896466     Total=    34.57248600
  Reference Point [Bohr]              0.15923413      0.17697005      0.16576237
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.53431424 Y=    3.18853312 Z=   -5.94701366     Total=    10.11432677
  Reference Point [Bohr]              0.15918710      0.17729214      0.16593434
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.92889570 Y=   -4.01728792 Z=    2.51889724     Total=    22.43568390
  Reference Point [Bohr]              0.15912026      0.00856096      0.16612544
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.13557711 Y=  -16.12108123 Z=   -0.69695198     Total=    26.59111923
  Reference Point [Bohr]              0.15900147      0.00891547     -0.00275139
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.47412312 Y=    2.29697847 Z=  -26.20934819     Total=    37.32405709
  Reference Point [Bohr]              0.32790919     -0.15980874     -0.00255268
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.39002151 Y=   25.86082268 Z=   27.13924247     Total=    39.48206257
  Reference Point [Bohr]              0.15864743     -0.15946862     -0.00234581
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.31714830 Y=   25.32629038 Z=  -20.39006962     Total=    41.83023091
  Reference Point [Bohr]              0.15844743     -0.15911836     -0.00212999
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.39933390 Y=   -0.85525603 Z=   11.39846828     Total=    23.38352766
  Reference Point [Bohr]              0.15824598     -0.32781647     -0.00192227
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.48166757 Y=    0.61800417 Z=  -13.68470122     Total=    18.53226921
  Reference Point [Bohr]              0.15805200     -0.15835609      0.16734750
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.47875014 Y=  -25.51743596 Z=   16.16309216     Total=    32.31326029
  Reference Point [Bohr]             -0.01120878     -0.15798716      0.16754822
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.00830295 Y=    2.59505000 Z=   -9.12157535     Total=    13.08002078
  Reference Point [Bohr]             -0.01139296     -0.15764967      0.16774511
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.01835357 Y=    3.28758145 Z=   -7.66090854     Total=    10.89747670
  Reference Point [Bohr]             -0.18067141     -0.15732513      0.33697440
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.55842638 Y=    5.09837542 Z=   -7.56685869     Total=    24.33379098
  Reference Point [Bohr]             -0.18092053     -0.15699455      0.33707562
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.62802071 Y=  -20.11465229 Z=   -8.83462122     Total=    30.13577620
  Reference Point [Bohr]             -0.18121016     -0.15665709      0.33714341
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.40197439 Y=   14.64260619 Z=   -9.46065993     Total=    21.39436774
  Reference Point [Bohr]             -0.18152164     -0.15630451      0.33718557
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.94918393 Y=   20.17580533 Z=   -3.21826067     Total=    28.55503917
  Reference Point [Bohr]             -0.18183856     -0.15591945      0.33719281
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.94299604 Y=   18.95193085 Z=   25.96022789     Total=    32.51987584
  Reference Point [Bohr]             -0.18214693     -0.32455742      0.33716676
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.61421246 Y=    8.89455844 Z=   23.20654237     Total=    25.11412572
  Reference Point [Bohr]             -0.01335814     -0.32406489      0.16804815
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.84457088 Y=   22.99317570 Z=   -7.45292362     Total=    31.91752394
  Reference Point [Bohr]             -0.18268692     -0.15447326      0.16799378
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.26498300 Y=   21.92043286 Z=   17.76599551     Total=    34.16541443
  Reference Point [Bohr]              0.15522123      0.01511971     -0.17021299
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.44092374 Y=   20.33303147 Z=   15.48840537     Total=    30.94363732
  Reference Point [Bohr]              0.15498102      0.01564287     -0.17026132
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.81323970 Y=   -8.48001142 Z=  -15.90525152     Total=    22.70887955
  Reference Point [Bohr]             -0.01433867      0.01615699     -0.17028722
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.11527060 Y=  -22.50161834 Z=  -25.63964189     Total=    38.62482483
  Reference Point [Bohr]             -0.01459511      0.01664973     -0.17030770
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.36182917 Y=   -2.67357007 Z=   15.58159521     Total=    25.77863792
  Reference Point [Bohr]             -0.01486951      0.01712425     -0.17034848
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.20616735 Y=  -11.32478318 Z=   -9.99031605     Total=    23.65421017
  Reference Point [Bohr]              0.15392191      0.01759235     -0.17040842
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.23298348 Y=    8.86513883 Z=  -16.65451021     Total=    26.94199418
  Reference Point [Bohr]             -0.01543494      0.01807134     -0.33953123
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.08431244 Y=  -27.27241678 Z=  -21.94917096     Total=    35.71747900
  Reference Point [Bohr]             -0.01572087      0.01857038     -0.17047770
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.27728701 Y=   -6.24833692 Z=    8.91841780     Total=    20.42264765
  Reference Point [Bohr]             -0.01600824      0.01907176     -0.17046243
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.72698224 Y=  -16.90458918 Z=   -3.36418678     Total=    19.31950069
  Reference Point [Bohr]             -0.01629923      0.01954154     -0.17040801
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.67903607 Y=  -20.71350757 Z=   -5.34142320     Total=    25.94329004
  Reference Point [Bohr]             -0.01660623      0.01996371     -0.17033323
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.32351024 Y=    4.38988000 Z=   -6.91903687     Total=    19.16371897
  Reference Point [Bohr]              0.15212721      0.02035969     -0.17024480
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.50020818 Y=  -27.03934586 Z=  -26.24541895     Total=    39.70142875
  Reference Point [Bohr]              0.15175174      0.02075292     -0.17011532
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.95727876 Y=   -3.61545803 Z=  -24.61814093     Total=    31.89698066
  Reference Point [Bohr]              0.15134962      0.02114921     -0.16993375
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.19134344 Y=   16.70407218 Z=  -25.53591532     Total=    31.59441574
  Reference Point [Bohr]              0.15092954      0.02155453     -0.16970664
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.09420719 Y=  -21.02907940 Z=  -24.80900936     Total=    34.05293151
  Reference Point [Bohr]              0.15050410      0.02197343     -0.00036052
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.18751763 Y=    2.97832231 Z=  -21.87603397     Total=    26.24341675
  Reference Point [Bohr]              0.15008273      0.02238877     -0.00005055
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.82252042 Y=  -22.13190078 Z=    6.81457527     Total=    24.14138051
  Reference Point [Bohr]              0.31873617      0.02277848      0.16934515
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.13796884 Y=  -15.46961674 Z=    1.52468511     Total=    16.37169602
  Reference Point [Bohr]              0.31831086      0.02314569      0.16966682
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.31144216 Y=   27.31410743 Z=   -9.07823802     Total=    29.69734090
  Reference Point [Bohr]              0.31787517      0.02351314      0.16999270
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.47203659 Y=  -20.77746962 Z=   21.70277703     Total=    40.04350753
  Reference Point [Bohr]              0.31741648      0.02390421      0.17032215
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.36915133 Y=    2.14374610 Z=   -6.98526401     Total=    12.68498561
  Reference Point [Bohr]              0.14786223      0.02432581      0.17064348
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.56003962 Y=   10.06675403 Z=   16.99528362     Total=    29.24063116
  Reference Point [Bohr]             -0.02170932      0.02477476      0.17094623
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.60392072 Y=   17.19900828 Z=   17.22116970     Total=    25.21876961
  Reference Point [Bohr]             -0.02221389      0.19430270      0.17124391
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.03870734 Y=   -1.97672238 Z=   18.18740117     Total=    27.13372043
  Reference Point [Bohr]              0.14636740      0.19473792      0.17154881
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.26804882 Y=   -6.56240368 Z=   -8.46742306     Total=    20.32111969
  Reference Point [Bohr]              0.14588597      0.02607997      0.17184230
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.48294892 Y=   -5.58104873 Z=  -10.96664038     Total=    18.25390966
  Reference Point [Bohr]              0.14540410      0.02648687      0.34118577
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.11808392 Y=   -9.65976659 Z=   -5.25616007     Total=    19.51232787
  Reference Point [Bohr]              0.14493428     -0.14217603      0.17236383
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.34348291 Y=  -11.96623782 Z=   10.93898258     Total=    23.74128444
  Reference Point [Bohr]              0.14447415     -0.31084299      0.17260958
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.61679760 Y=  -16.13121958 Z=    6.30219426     Total=    20.31379554
  Reference Point [Bohr]              0.31308623     -0.31046225      0.17286606
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.96670850 Y=    8.78642389 Z=  -23.67324980     Total=    28.38590372
  Reference Point [Bohr]              0.31262403     -0.47917790      0.17314202
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.69553668 Y=  -14.74658114 Z=    6.51058750     Total=    19.91569690
  Reference Point [Bohr]              0.14308345     -0.30975258      0.17342880
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.97889041 Y=   17.44435098 Z=  -12.67744662     Total=    27.44641604
  Reference Point [Bohr]              0.14260560     -0.30940974      0.17370981
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.70275149 Y=   22.01962210 Z=    1.29467821     Total=    30.94429465
  Reference Point [Bohr]              0.14211553     -0.30908579      0.17398697
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.78789754 Y=   24.84119479 Z=    9.93040055     Total=    36.47105260
  Reference Point [Bohr]              0.14162671     -0.30877188      0.17427005
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.90668254 Y=   -1.40914743 Z=  -11.27844050     Total=    29.20887676
  Reference Point [Bohr]              0.14114875     -0.30844619      0.34363623
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.95801966 Y=    1.21846641 Z=   -6.39176124     Total=     8.18053978
  Reference Point [Bohr]              0.14068555     -0.30809421      0.34394313
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.03181962 Y=   26.01162310 Z=   -2.44075930     Total=    33.53951817
  Reference Point [Bohr]              0.14024807     -0.30772697      0.34425785
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.04770872 Y=   26.29590145 Z=  -26.48415344     Total=    38.40241984
  Reference Point [Bohr]              0.13984333     -0.30736652      0.34456364
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.34655172 Y=  -25.55157286 Z=  -22.26703305     Total=    38.53958480
  Reference Point [Bohr]              0.13945665     -0.47608435      0.34485703
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.90009488 Y=   -6.30304250 Z=   14.95718598     Total=    18.05151673
  Reference Point [Bohr]              0.30814352     -0.47571574      0.34514875
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.00804278 Y=    0.98388628 Z=   21.64523353     Total=    22.23880976
  Reference Point [Bohr]              0.30776300     -0.47533797      0.34544930
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.72720779 Y=  -24.98671040 Z=   24.54449860     Total=    42.30541925
  Reference Point [Bohr]              0.47647031     -0.47497115      0.34576389
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.00527058 Y=  -26.68316713 Z=   26.32159946     Total=    38.54754084
  Reference Point [Bohr]              0.47610414     -0.47461395      0.34609291
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.06541314 Y=  -24.05343181 Z=  -27.30020031     Total=    43.62353297
  Reference Point [Bohr]              0.47573172     -0.47424426      0.34641688
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.31804593 Y=  -13.19917032 Z=    2.03818292     Total=    29.51290952
  Reference Point [Bohr]              0.30628667     -0.47385101      0.17764578
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.46309679 Y=  -19.02540222 Z=    3.49490730     Total=    27.44070778
  Reference Point [Bohr]              0.30589918     -0.47344734      0.17793606
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.07349521 Y=  -20.40319416 Z=    4.05770595     Total=    26.91207068
  Reference Point [Bohr]              0.30548255     -0.47304911      0.17823347
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.71476254 Y=    7.05175514 Z=    2.39769294     Total=    25.81270365
  Reference Point [Bohr]              0.30506328     -0.47265251      0.17853698
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.24288465 Y=    7.79681035 Z=   -1.97936058     Total=     8.13958734
  Reference Point [Bohr]              0.30467082     -0.47223883      0.17883302
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.44874832 Y=  -16.93919135 Z=   21.29591092     Total=    35.92068795
  Reference Point [Bohr]              0.30430559     -0.30272794      0.17911832
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.71981526 Y=   16.35929302 Z=   -9.83148396     Total=    21.89061407
  Reference Point [Bohr]              0.30395199     -0.30227905      0.17938955
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.90195108 Y=   -1.70766743 Z=  -14.85271843     Total=    21.82639276
  Reference Point [Bohr]              0.30360387     -0.30182188      0.17965980
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.39845842 Y=    4.67053239 Z=  -19.24770327     Total=    20.81413520
  Reference Point [Bohr]              0.13419823     -0.30135396      0.17994584
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.10707004 Y=  -19.04254071 Z=  -21.82390932     Total=    28.98494400
  Reference Point [Bohr]              0.13389988     -0.30088726      0.18024796
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.53876816 Y=   -0.13268640 Z=    5.57112796     Total=    24.18943320
  Reference Point [Bohr]              0.13362896     -0.30043381      0.01146614
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.07881054 Y=   27.47513798 Z=  -18.41578819     Total=    39.76805673
  Reference Point [Bohr]              0.13335775     -0.29999464      0.01172290
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.28115342 Y=   -1.29698723 Z=   15.05365954     Total=    30.31491162
  Reference Point [Bohr]             -0.03599905     -0.29956192      0.01196207
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.76161486 Y=    0.36359255 Z=   -7.59865502     Total=    27.82185809
  Reference Point [Bohr]              0.13278378     -0.29912672      0.01221153
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.24579287 Y=    4.78637311 Z=   -4.02723864     Total=     6.26006651
  Reference Point [Bohr]              0.13248201     -0.29868735      0.01247289
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.84541564 Y=    8.51811001 Z=   -1.52116402     Total=    26.30906339
  Reference Point [Bohr]              0.13215889     -0.29824351      0.01274111
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.14190714 Y=   10.13414945 Z=    0.53191845     Total=    10.96080823
  Reference Point [Bohr]              0.13182269     -0.29778773     -0.15605571
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.64259600 Y=  -16.43156458 Z=  -23.45388066     Total=    28.86779067
  Reference Point [Bohr]              0.13148643     -0.12825491     -0.15577900
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.58822538 Y=  -14.86033348 Z=    2.85148890     Total=    27.18801990
  Reference Point [Bohr]              0.13114640     -0.12780703     -0.15550755
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.66175058 Y=   13.89851506 Z=   21.60578997     Total=    32.35063086
  Reference Point [Bohr]              0.13081393      0.04172164     -0.15525249
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.59980823 Y=   16.19441680 Z=   24.73711759     Total=    32.97481649
  Reference Point [Bohr]              0.29959571      0.04220457     -0.15502205
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.25894200 Y=   16.32769544 Z=  -12.96787697     Total=    24.70949240
  Reference Point [Bohr]              0.29935329      0.04270073     -0.15480523
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.31931307 Y=   10.39026265 Z=  -18.02373754     Total=    24.70256614
  Reference Point [Bohr]              0.29914517      0.04319061     -0.15458656
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.49782187 Y=   13.30967662 Z=    5.73648255     Total=    17.32810850
  Reference Point [Bohr]              0.29896514      0.04368038     -0.15435797
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.16797296 Y=   11.24284097 Z=    0.98138021     Total=    18.90587168
  Reference Point [Bohr]              0.29881283      0.04418266     -0.15412344
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.97437159 Y=    8.92496963 Z=   23.32311117     Total=    25.05036408
  Reference Point [Bohr]              0.29868915      0.04469618     -0.15389013
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.30256368 Y=    6.42250805 Z=   -9.16030735     Total=    11.26305964
  Reference Point [Bohr]              0.29858623      0.04522469     -0.15365838
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.09841402 Y=  -23.19703646 Z=  -14.69242476     Total=    27.48047232
  Reference Point [Bohr]              0.46757485     -0.12328582     -0.15342549
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.20676601 Y=  -27.48770071 Z=   10.53325821     Total=    39.41215299
  Reference Point [Bohr]              0.46752116     -0.12266924     -0.15319916
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.76577564 Y=   -6.05540727 Z=   12.14356587     Total=    14.38216836
  Reference Point [Bohr]              0.46750698      0.04706203     -0.15298328
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.01412539 Y=   -6.53557706 Z=    5.50089330     Total=    11.05312397
  Reference Point [Bohr]              0.46752612      0.04773703     -0.15277801
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.45321128 Y=  -25.78276265 Z=  -22.06288254     Total=    34.22503070
  Reference Point [Bohr]              0.46757193      0.04843300     -0.15259145
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.91507478 Y=  -25.17568552 Z=  -25.15762755     Total=    44.02627018
  Reference Point [Bohr]              0.46763620      0.04914907     -0.15241781
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.56088366 Y=  -26.47909782 Z=  -23.02663372     Total=    35.18418121
  Reference Point [Bohr]              0.46769665      0.04986650     -0.15223743
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.73912113 Y=   -0.38661173 Z=  -21.91097345     Total=    28.83391904
  Reference Point [Bohr]              0.46773364     -0.28758436      0.18610030
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.64011191 Y=   -1.18836060 Z=  -18.98361386     Total=    25.27218076
  Reference Point [Bohr]              0.46774736     -0.28692120      0.18630074
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.93573346 Y=   -1.64552677 Z=  -10.48666747     Total=    11.70638364
  Reference Point [Bohr]              0.29867727     -0.28626533      0.18651613
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.05240287 Y=   25.66186882 Z=  -13.74987733     Total=    29.18566421
  Reference Point [Bohr]              0.29867529     -0.28558625      0.18672633
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.05700731 Y=   26.26770817 Z=   -6.40843606     Total=    38.25104168
  Reference Point [Bohr]              0.29867243     -0.28489072      0.18691548
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.40088505 Y=  -27.13209398 Z=   20.49019563     Total=    43.04654890
  Reference Point [Bohr]              0.29866938     -0.28419472      0.18711075
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.22622851 Y=  -25.22901459 Z=   18.26997747     Total=    31.22901451
  Reference Point [Bohr]              0.29864801     -0.28350378      0.18732635
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.54793709 Y=  -22.78925642 Z=   13.97760955     Total=    26.85546053
  Reference Point [Bohr]              0.12951319     -0.28281835      0.18753488
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.18712193 Y=  -22.72612827 Z=  -24.01515517     Total=    41.56435606
  Reference Point [Bohr]              0.12941129     -0.28212529      0.18771441
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.12942627 Y=   23.93797797 Z=   -0.88117839     Total=    26.85006976
  Reference Point [Bohr]              0.12929314     -0.28140080      0.18786783
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.54162548 Y=   23.50193527 Z=  -27.18804631     Total=    38.40451073
  Reference Point [Bohr]              0.12918553     -0.28063579      0.18800091
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.79457914 Y=  -21.91626558 Z=  -22.57223790     Total=    33.96365522
  Reference Point [Bohr]              0.12909148     -0.27983497      0.18810152
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.94243287 Y=   11.22208627 Z=   13.78098541     Total=    19.89517240
  Reference Point [Bohr]              0.12902012     -0.27899861      0.18814567
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.52681821 Y=  -14.20241334 Z=   18.07741912     Total=    29.52532167
  Reference Point [Bohr]              0.12899257     -0.27813575      0.18814518
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.67479292 Y=   13.73803714 Z=   -9.39331268     Total=    20.32901319
  Reference Point [Bohr]              0.12900010     -0.27727309      0.18814153
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.98166709 Y=  -15.08348003 Z=   23.08756328     Total=    29.68406913
  Reference Point [Bohr]              0.12902294     -0.10735948      0.18816608
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.15117380 Y=  -17.24879902 Z=    0.02135460     Total=    20.01419130
  Reference Point [Bohr]              0.29812789     -0.10654768      0.18823380
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.94104617 Y=    8.57997537 Z=  -23.26454420     Total=    28.94978160
  Reference Point [Bohr]              0.29815861      0.06330668      0.18834806
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.42980922 Y=  -19.65834330 Z=  -18.85294257     Total=    29.53852474
  Reference Point [Bohr]              0.29817314      0.06405783      0.18850856
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.17942373 Y=   11.45510281 Z=  -15.87269013     Total=    27.40459755
  Reference Point [Bohr]              0.29814899      0.06479225      0.18870195
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.22616132 Y=   -2.96337599 Z=   11.08888896     Total=    16.76973692
  Reference Point [Bohr]              0.29809579     -0.10354807      0.18890125
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.73982229 Y=  -12.19207448 Z=  -22.08579211     Total=    26.38813639
  Reference Point [Bohr]              0.29803766     -0.10280426      0.18910272
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.33957735 Y=  -20.76502571 Z=    9.66911037     Total=    23.02502139
  Reference Point [Bohr]              0.29796689     -0.10204966      0.18933681
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.70981480 Y=  -22.06848187 Z=    9.16209932     Total=    23.95590580
  Reference Point [Bohr]              0.29786711     -0.10129771      0.18960438
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.42388413 Y=  -23.43932018 Z=   10.07252163     Total=    25.55161186
  Reference Point [Bohr]              0.29773289     -0.26962786      0.18989594
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.59917485 Y=    3.14708165 Z=   15.20859752     Total=    15.94238442
  Reference Point [Bohr]              0.29757523     -0.26888066     -0.14792974
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.61491624 Y=    2.72899123 Z=    3.70991739     Total=     8.89931624
  Reference Point [Bohr]              0.29741087     -0.26810816     -0.14757875
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.64575069 Y=  -24.42445317 Z=  -24.61579159     Total=    38.46520667
  Reference Point [Bohr]              0.29724419     -0.26730391     -0.14721494
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.86804876 Y=  -23.19345357 Z=    1.18502280     Total=    27.04927622
  Reference Point [Bohr]              0.29707497     -0.26648240     -0.14686500
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.20600175 Y=    6.30770756 Z=   -0.35118477     Total=    12.00304033
  Reference Point [Bohr]              0.29691894     -0.26565695     -0.14654507
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.38621317 Y=   12.94626909 Z=   -1.34274549     Total=    25.03555397
  Reference Point [Bohr]              0.29679187     -0.26483720     -0.14626252
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.78172216 Y=   -7.15938752 Z=  -25.96825743     Total=    27.20126185
  Reference Point [Bohr]              0.29668997     -0.26403236     -0.14601119
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.09099546 Y=   20.56202212 Z=  -16.58031064     Total=    29.48012240
  Reference Point [Bohr]              0.29661119     -0.26322436     -0.14577334
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.42735206 Y=   24.62246373 Z=    7.31588480     Total=    29.46075997
  Reference Point [Bohr]              0.12749706     -0.26238319     -0.14553137
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.45312863 Y=   27.14688234 Z=   15.14591393     Total=    34.28184442
  Reference Point [Bohr]              0.12751272     -0.26150745     -0.14527762
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.67171730 Y=    4.49084556 Z=    8.75090907     Total=    10.19235875
  Reference Point [Bohr]              0.12758885     -0.26062078     -0.14500690
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.87620987 Y=   25.63117856 Z=   13.73367125     Total=    36.38872901
  Reference Point [Bohr]              0.12772061     -0.25973843     -0.14470386
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.26635079 Y=   18.37743483 Z=    9.21306604     Total=    29.57817393
  Reference Point [Bohr]              0.12790049     -0.25887029     -0.14435991
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.32783253 Y=  -19.61106627 Z=  -24.65748728     Total=    40.42381353
  Reference Point [Bohr]              0.12811884     -0.42709737     -0.14398398
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.45785624 Y=   -1.45125299 Z=   25.13014135     Total=    34.40786478
  Reference Point [Bohr]              0.12835730     -0.42626567     -0.14358946
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.30159520 Y=   -9.32979541 Z=   19.35283817     Total=    28.88129161
  Reference Point [Bohr]              0.12859576     -0.25636109     -0.14318339
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.35168163 Y=   13.60944228 Z=   -9.85064292     Total=    26.39020709
  Reference Point [Bohr]              0.12883451     -0.25552433     -0.14276615
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.91712130 Y=  -16.90262986 Z=   19.90296810     Total=    36.09279664
  Reference Point [Bohr]              0.12907537     -0.25468216     -0.14232684
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.76841969 Y=  -19.13808063 Z=   -1.42275028     Total=    26.84294928
  Reference Point [Bohr]             -0.03975713     -0.42291416     -0.14185214
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.91817579 Y=    6.82316572 Z=    2.83050029     Total=    10.82888869
  Reference Point [Bohr]             -0.20859291     -0.42208174     -0.14133955
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.32437832 Y=    5.88186544 Z=  -22.19932728     Total=    32.02786818
  Reference Point [Bohr]             -0.20837266     -0.42126415     -0.14078935
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.97912159 Y=    5.83396434 Z=    8.48691427     Total=    24.27230190
  Reference Point [Bohr]             -0.20818215     -0.42045465      0.02887308
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.32935234 Y=    7.82978121 Z=   12.27105389     Total=    25.82296475
  Reference Point [Bohr]             -0.03895289     -0.41964033      0.02948058
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.00511288 Y=   16.10878027 Z=  -11.51767174     Total=    20.69325844
  Reference Point [Bohr]             -0.03882528     -0.41883432      0.03005868
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.07901426 Y=   11.22850197 Z=   19.06486605     Total=    23.55459287
  Reference Point [Bohr]             -0.03870241     -0.24899090      0.03055982
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.76591797 Y=   -0.12449278 Z=   -6.31793908     Total=    17.91725029
  Reference Point [Bohr]             -0.03856591     -0.24825702      0.03097929
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.15458860 Y=    1.15378635 Z=   22.01790324     Total=    32.70418072
  Reference Point [Bohr]             -0.03842689     -0.24754163      0.03135047
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.66158483 Y=   27.21893374 Z=   -6.30810664     Total=    36.61329212
  Reference Point [Bohr]              0.13076727     -0.41590657      0.03169250
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.35791294 Y=   24.43630592 Z=  -12.05710478     Total=    34.01398892
  Reference Point [Bohr]              0.13087050     -0.41519440      0.03200691
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.62723418 Y=   22.02638511 Z=    1.19068504     Total=    30.20036692
  Reference Point [Bohr]              0.13097517     -0.41447214      0.03229788
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.18078095 Y=   -6.71762665 Z=  -21.39040560     Total=    28.24633062
  Reference Point [Bohr]              0.13109924     -0.41375608      0.03256926
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.43499197 Y=   -7.36923586 Z=  -24.76914032     Total=    27.18391140
  Reference Point [Bohr]              0.13125028     -0.41307504      0.03282968
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.31334615 Y=   -2.82970797 Z=  -26.90041908     Total=    35.70926915
  Reference Point [Bohr]              0.46956451     -0.24334774      0.03308887
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.47043722 Y=   24.69760760 Z=   -2.25592702     Total=    25.04206386
  Reference Point [Bohr]              0.30064587     -0.24271286      0.03334466
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.65167765 Y=  -26.74261546 Z=   -6.11659875     Total=    28.00931491
  Reference Point [Bohr]              0.30077030     -0.24212627      0.20267601
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.59366420 Y=  -18.97368304 Z=   16.21921399     Total=    30.53850964
  Reference Point [Bohr]              0.30087106     -0.24159535      0.20294578
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.70706797 Y=   -3.64119756 Z=   11.90364007     Total=    17.78832603
  Reference Point [Bohr]              0.30097685     -0.24109048      0.20321937
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.70263616 Y=  -25.71038019 Z=  -18.23587753     Total=    32.70025620
  Reference Point [Bohr]              0.30111672     -0.24059302      0.03441874
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.78376058 Y=    5.88705991 Z=    7.59050769     Total=    22.89624391
  Reference Point [Bohr]              0.30128868     -0.24009458      0.03470377
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.15347693 Y=  -18.17104626 Z=    5.90825502     Total=    20.40261335
  Reference Point [Bohr]              0.30146926     -0.23958632      0.03500610
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.78931651 Y=   12.75999694 Z=    3.33350285     Total=    15.84871755
  Reference Point [Bohr]              0.30164049     -0.23907676      0.03530396
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.66908007 Y=   26.21927512 Z=  -22.34211290     Total=    36.37015021
  Reference Point [Bohr]              0.30179821     -0.23858428      0.03557570
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.27599052 Y=  -17.03780978 Z=  -24.20914322     Total=    30.26148765
  Reference Point [Bohr]              0.47101610     -0.06904519      0.03581194
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.04759586 Y=   17.99162257 Z=   27.21146677     Total=    35.92481799
  Reference Point [Bohr]              0.47115009     -0.06859952      0.03599558
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.83676526 Y=  -11.05412448 Z=   -9.60362443     Total=    14.66708718
  Reference Point [Bohr]              0.30221191     -0.23723534      0.03611773
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.48817650 Y=   15.88681463 Z=    6.13512572     Total=    17.09518400
  Reference Point [Bohr]              0.30235948     -0.23680895      0.03620624
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.77708836 Y=   18.88195975 Z=   16.90735142     Total=    36.87003386
  Reference Point [Bohr]              0.30251505     -0.23638471      0.03629883
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.82281580 Y=   -1.08128630 Z=  -20.18342305     Total=    30.48640135
  Reference Point [Bohr]              0.30267816     -0.23593953      0.03640078
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.26209557 Y=   -3.79892442 Z=   -2.42256097     Total=    12.12993921
  Reference Point [Bohr]              0.30284813     -0.23546575      0.03649241
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.54685611 Y=   -5.41472283 Z=  -16.61028807     Total=    24.76111977
  Reference Point [Bohr]              0.30300912     -0.23497564      0.03655663
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.60471971 Y=    9.96393402 Z=  -18.97207301     Total=    26.50899494
  Reference Point [Bohr]              0.30315420     -0.23448635      0.03658993
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.71151616 Y=   24.03886576 Z=    7.84587248     Total=    26.16236287
  Reference Point [Bohr]              0.30328875     -0.23399443      0.03660573
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.00025309 Y=  -14.90588029 Z=  -20.92937419     Total=    35.85019701
  Reference Point [Bohr]              0.30341186     -0.23347633      0.03660871
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.44013998 Y=    2.81312136 Z=    4.56153303     Total=     5.88859223
  Reference Point [Bohr]              0.30351927     -0.23292075      0.03659288
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.54666413 Y=   22.20698036 Z=  -24.13583001     Total=    33.89297471
  Reference Point [Bohr]              0.30362560     -0.40142114      0.03656485
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.96768671 Y=   -1.46923330 Z=    3.49738182     Total=    17.38656719
  Reference Point [Bohr]              0.30373245     -0.40085888      0.03653862
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.87285852 Y=  -15.59930134 Z=    4.01278122     Total=    25.58067867
  Reference Point [Bohr]              0.13476604     -0.40032642      0.20560129
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.75404816 Y=   19.80264352 Z=  -18.41124760     Total=    35.33929026
  Reference Point [Bohr]              0.13488370     -0.39982508      0.20560480
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.68796481 Y=   19.75895671 Z=  -10.38869637     Total=    34.03252736
  Reference Point [Bohr]              0.13501302     -0.39935606      0.20561126
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.14551724 Y=   23.31311589 Z=   21.64338957     Total=    38.19778245
  Reference Point [Bohr]              0.13513900     -0.39892177      0.20560798
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.21097593 Y=    1.77093003 Z=   18.66939276     Total=    21.35290258
  Reference Point [Bohr]              0.13524705     -0.39851507      0.20559360
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.05628823 Y=  -18.65003849 Z=    9.56562152     Total=    25.23696276
  Reference Point [Bohr]              0.13534448     -0.39813698      0.20558064
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.21170511 Y=   13.49979673 Z=  -22.32634308     Total=    28.80687155
  Reference Point [Bohr]              0.13545610     -0.39779376      0.20557001
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.46646054 Y=  -14.05266496 Z=  -26.21764767     Total=    36.10704154
  Reference Point [Bohr]              0.13559861     -0.39749440      0.37461841
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.52467939 Y=  -16.91093293 Z=   -1.50184459     Total=    17.33950849
  Reference Point [Bohr]              0.13578253     -0.39725435      0.20548279
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.89831847 Y=    8.81091869 Z=   21.81353627     Total=    23.70364746
  Reference Point [Bohr]              0.13600352     -0.39706893      0.20537381
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.37691593 Y=    7.90166941 Z=  -10.63880065     Total=    16.23413105
  Reference Point [Bohr]              0.13623957     -0.39690513      0.20523147
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.21246928 Y=  -20.80611581 Z=   18.52944944     Total=    29.34458283
  Reference Point [Bohr]              0.30554856     -0.22767168      0.20508633
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.21563446 Y=  -23.78042545 Z=   21.06992760     Total=    32.37413466
  Reference Point [Bohr]              0.30576890     -0.22752206      0.20495419
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.24125623 Y=   24.60374088 Z=   20.86318699     Total=    32.68160650
  Reference Point [Bohr]              0.30597346     -0.22738598      0.03575665
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.75464771 Y=   -9.16164517 Z=   -5.49264400     Total=    11.69237167
  Reference Point [Bohr]              0.30617986     -0.39633431      0.03562843
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.05311841 Y=   17.30827744 Z=   -1.32378768     Total=    17.62527769
  Reference Point [Bohr]              0.30639916     -0.39621610      0.03548206
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.25303254 Y=   20.01388634 Z=    5.65302450     Total=    20.83464478
  Reference Point [Bohr]              0.30663042     -0.22702158      0.03529666
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.24613601 Y=   -2.12251322 Z=   -4.21817847     Total=    25.68395366
  Reference Point [Bohr]              0.30686778     -0.22689567      0.03506963
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.97489433 Y=   24.09067427 Z=  -15.43743018     Total=    30.64511614
  Reference Point [Bohr]              0.30711762     -0.22677378     -0.13424429
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.94609114 Y=   24.11878713 Z=   -3.90599003     Total=    32.84210053
  Reference Point [Bohr]              0.30738254     -0.22665524     -0.13447521
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.42642513 Y=   20.78808618 Z=   -6.50867809     Total=    23.73530932
  Reference Point [Bohr]              0.13857331     -0.22652653     -0.13469539
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.15963230 Y=  -12.99973255 Z=   -7.81093038     Total=    19.43863004
  Reference Point [Bohr]              0.13882625     -0.39545466     -0.13491593
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.64507852 Y=  -23.66872013 Z=    2.44207398     Total=    26.06702389
  Reference Point [Bohr]              0.13906559     -0.39530295     -0.13514959
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.10593491 Y=  -26.63944911 Z=    8.71512286     Total=    29.17738501
  Reference Point [Bohr]              0.13929980     -0.39515522     -0.13539861
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.30428802 Y=   -0.55564710 Z=  -13.87423056     Total=    24.59811231
  Reference Point [Bohr]              0.13953784     -0.39501935     -0.13565367
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.50386952 Y=  -27.23662002 Z=  -10.24860764     Total=    35.59882153
  Reference Point [Bohr]              0.13978879     -0.39489633     -0.13589812
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.18453779 Y=    1.41339313 Z=   -8.30165931     Total=    20.03977650
  Reference Point [Bohr]              0.14006837     -0.22571491     -0.13611127
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.49938357 Y=    6.22336241 Z=   16.71966894     Total=    24.30035447
  Reference Point [Bohr]              0.14036733     -0.22562821     -0.13628692
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.16053683 Y=   -1.97761846 Z=   12.72046508     Total=    25.62831636
  Reference Point [Bohr]              0.14065320     -0.22554922      0.03261474
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.24001618 Y=    4.01144169 Z=   13.68293532     Total=    28.98918419
  Reference Point [Bohr]             -0.02815945     -0.22546575      0.03241289
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.78706359 Y=  -18.97357201 Z=  -15.62176627     Total=    33.51546335
  Reference Point [Bohr]             -0.02791782     -0.22539503      0.03217574
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.87555144 Y=  -19.33044970 Z=   11.23729305     Total=    24.44319040
  Reference Point [Bohr]              0.14138441     -0.22534711      0.03192398
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.64527991 Y=    7.50803545 Z=  -16.69868887     Total=    24.74433571
  Reference Point [Bohr]              0.14160837     -0.22530205      0.03167511
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.08513438 Y=    5.81620918 Z=   10.55883033     Total=    24.28785867
  Reference Point [Bohr]              0.14183051     -0.22523095      0.03143359
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.93971216 Y=    2.55097250 Z=  -16.85261360     Total=    17.74595171
  Reference Point [Bohr]              0.14203680     -0.22512963      0.03121260
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.43488185 Y=   24.17711581 Z=   13.42613887     Total=    27.86741012
  Reference Point [Bohr]             -0.02687589     -0.22502523      0.03101440
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.11251861 Y=   15.98579544 Z=   16.47544313     Total=    35.52568856
  Reference Point [Bohr]             -0.02678054     -0.22494257      0.03082633
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.28464307 Y=    4.19601151 Z=   -4.68672629     Total=     8.89205569
  Reference Point [Bohr]             -0.02673724     -0.22487709      0.03064931
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.82157484 Y=   14.43800374 Z=  -22.52158614     Total=    29.24769095
  Reference Point [Bohr]              0.14235272     -0.22481757      0.03048973
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.07484003 Y=    0.86053406 Z=  -11.02272950     Total=    19.51003759
  Reference Point [Bohr]              0.14236669     -0.22477227      0.03034944
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.49686256 Y=    1.41902026 Z=  -13.12185912     Total=    22.72291200
  Reference Point [Bohr]              0.14240973     -0.22474719      0.03024212
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.37780725 Y=  -26.46672679 Z=   22.49151701     Total=    40.78439171
  Reference Point [Bohr]              0.14248917     -0.22474591      0.03017355
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.99126537 Y=   -1.27360989 Z=    1.39190154     Total=    24.06533371
  Reference Point [Bohr]              0.14258947     -0.22476577      0.03012711
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.26209132 Y=   23.89076673 Z=  -12.45159102     Total=    36.93215553
  Reference Point [Bohr]              0.14271922     -0.22479064      0.03008827
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.10534925 Y=   -6.32360601 Z=  -20.35872085     Total=    28.62655895
  Reference Point [Bohr]             -0.02619082     -0.22481780      0.03007451
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.78080371 Y=  -10.13434466 Z=  -16.27293457     Total=    21.08591603
  Reference Point [Bohr]             -0.02603014     -0.22485679      0.03010018
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.93776570 Y=    9.81034478 Z=  -16.25996101     Total=    27.53440934
  Reference Point [Bohr]             -0.02590005     -0.22491056      0.03014864
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.58151644 Y=   19.50594945 Z=    8.39497984     Total=    28.21755666
  Reference Point [Bohr]             -0.02578916     -0.22497546      0.03020780
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.55020898 Y=  -10.24934296 Z=  -21.75499252     Total=    28.10760239
  Reference Point [Bohr]             -0.02567822     -0.05596475      0.03027491
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.50749833 Y=   -6.78479847 Z=    3.28771467     Total=     9.95942230
  Reference Point [Bohr]              0.14350310     -0.05601104      0.03033736
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.08470172 Y=   -6.26245491 Z=   25.40391773     Total=    27.38502838
  Reference Point [Bohr]              0.14359585     -0.05604731      0.03038067
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.63190287 Y=  -10.26661608 Z=   16.03866840     Total=    19.22418275
  Reference Point [Bohr]              0.14367428     -0.22513745      0.03041012
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.64804214 Y=   -7.91095783 Z=   -9.57974930     Total=    19.98039222
  Reference Point [Bohr]              0.14375165     -0.22510691      0.03044633
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.32023992 Y=   -7.32428076 Z=  -19.86269353     Total=    21.17248773
  Reference Point [Bohr]              0.14384510     -0.22503601      0.03050467
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.67189954 Y=   20.65544200 Z=   14.10853736     Total=    25.02298063
  Reference Point [Bohr]              0.31303627     -0.22496550     -0.13847713
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.71450847 Y=   -3.82859979 Z=  -14.20486622     Total=    30.49756323
  Reference Point [Bohr]              0.31317878     -0.22492952     -0.13834475
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.53103842 Y=    1.66315818 Z=   13.80688508     Total=    13.91683055
  Reference Point [Bohr]              0.14426149     -0.22492872     -0.13818498
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.27450464 Y=    7.62426312 Z=   15.86658248     Total=    17.90531230
  Reference Point [Bohr]              0.14439720     -0.22494401     -0.13803461
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.06534863 Y=   15.33065280 Z=  -16.65026854     Total=    22.83980560
  Reference Point [Bohr]              0.14448438     -0.22496715      0.03114870
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.65242385 Y=  -10.16111302 Z=    4.77263075     Total=    14.80525273
  Reference Point [Bohr]              0.14453126     -0.22498963      0.03120841
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.23931734 Y=  -10.96171933 Z=  -24.60803988     Total=    34.30486144
  Reference Point [Bohr]              0.14456597     -0.05592306      0.03122867
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.75740620 Y=  -20.81932811 Z=    2.84067422     Total=    28.16654292
  Reference Point [Bohr]             -0.02447601     -0.05590858      0.03123404
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.29791693 Y=  -18.30586040 Z=    4.06007293     Total=    18.75306566
  Reference Point [Bohr]             -0.02446983     -0.05587237      0.03124712
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.71281580 Y=  -19.76039558 Z=   12.46549813     Total=    31.89526998
  Reference Point [Bohr]             -0.02450391     -0.05582133      0.03128270
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.88237259 Y=   11.81285031 Z=   20.76329310     Total=    35.96275474
  Reference Point [Bohr]             -0.02455568     -0.05576154      0.03133643
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.18585090 Y=    4.45279710 Z=   25.02940052     Total=    25.42307678
  Reference Point [Bohr]             -0.02459609     -0.05569121      0.03139586
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.18585451 Y=  -27.20373550 Z=   26.60768197     Total=    45.63265533
  Reference Point [Bohr]             -0.02460959     -0.05561858      0.03145471
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.25427366 Y=    4.71169757 Z=  -20.45685007     Total=    33.61502185
  Reference Point [Bohr]             -0.02458244     -0.05555688      0.03151018
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.74535686 Y=    9.49679296 Z=    1.25943043     Total=    11.71644489
  Reference Point [Bohr]              0.14455982     -0.05549835      0.03157162
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.46696263 Y=    9.18836822 Z=    6.88007740     Total=    11.99088844
  Reference Point [Bohr]              0.14464467     -0.05542999      0.03165242
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.41005123 Y=   10.33570890 Z=  -25.08452751     Total=    38.56645313
  Reference Point [Bohr]              0.31378904     -0.05535460      0.03175229
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.63815740 Y=   10.79323890 Z=   26.65629219     Total=    29.30598468
  Reference Point [Bohr]              0.31383178     -0.22435257      0.03186657
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.30723585 Y=   -6.90626732 Z=    5.46628850     Total=     9.40822232
  Reference Point [Bohr]              0.31384528     -0.22428454     -0.13707900
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.31265784 Y=    0.29112844 Z=   -8.95880957     Total=     8.96898989
  Reference Point [Bohr]              0.14477182     -0.39329709     -0.13694519
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.22995864 Y=  -20.72618399 Z=  -16.06603743     Total=    26.56284646
  Reference Point [Bohr]              0.31385066     -0.39322214     -0.13681653
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.02509330 Y=  -14.96372995 Z=  -21.22155072     Total=    29.51221223
  Reference Point [Bohr]              0.31386659     -0.39312351     -0.13670404
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.25278971 Y=  -19.22047125 Z=   20.63919801     Total=    28.88772038
  Reference Point [Bohr]              0.31388595     -0.39301349     -0.13661312
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.85644606 Y=   12.07702995 Z=  -20.50477854     Total=    23.81247773
  Reference Point [Bohr]              0.14481792     -0.39290862     -0.13651574
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.75759871 Y=   17.64111782 Z=    1.15603682     Total=    18.92645237
  Reference Point [Bohr]              0.14482163     -0.39281979     -0.13638456
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.40953787 Y=  -21.09731589 Z=  -14.14373360     Total=    31.36961942
  Reference Point [Bohr]              0.14484543     -0.22367601     -0.13622830
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.23493767 Y=   22.34734809 Z=   18.68289289     Total=    30.87407331
  Reference Point [Bohr]              0.14490359     -0.22363009     -0.13607090
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.64570203 Y=  -19.46471141 Z=   -4.86640497     Total=    22.26199576
  Reference Point [Bohr]              0.14498896     -0.22359983     -0.13592109
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.19528099 Y=  -27.13842854 Z=   -0.99386848     Total=    35.07296076
  Reference Point [Bohr]              0.14509181     -0.22355643      0.03329827
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.29164133 Y=    6.74304930 Z=   23.40119480     Total=    24.57477435
  Reference Point [Bohr]              0.14522466     -0.22348691      0.03344892
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.61207451 Y=   14.42492710 Z=  -18.59554450     Total=    27.18752231
  Reference Point [Bohr]              0.14541511     -0.22341108      0.03360977
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.68202255 Y=  -21.50100351 Z=    4.27300027     Total=    25.84084798
  Reference Point [Bohr]              0.14567510     -0.22334437      0.03377346
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.99160913 Y=   -1.07686796 Z=  -24.98562560     Total=    27.73517299
  Reference Point [Bohr]              0.14599277     -0.22327023      0.03394207
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.67304317 Y=   17.13524117 Z=    3.65142794     Total=    25.60531111
  Reference Point [Bohr]              0.14634819     -0.22317542      0.03412383
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.24293333 Y=  -25.89628570 Z=  -20.12881485     Total=    40.19976057
  Reference Point [Bohr]              0.31579662     -0.22306681      0.03432462
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.28392267 Y=   21.40366806 Z=   10.31721080     Total=    36.17974960
  Reference Point [Bohr]              0.31618300     -0.22296483      0.03453437
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.57534535 Y=   20.83430205 Z=    8.68486183     Total=    33.36828683
  Reference Point [Bohr]              0.31655777     -0.39196350      0.03473719
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.02403280 Y=   23.72424391 Z=  -23.20779654     Total=    40.97066904
  Reference Point [Bohr]              0.31689108     -0.39192839      0.03493851
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.58114761 Y=    1.15884449 Z=   27.44091694     Total=    36.85891563
  Reference Point [Bohr]              0.31718266     -0.39193955      0.03515259
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.64192495 Y=    7.47231347 Z=   23.42973125     Total=    24.86063942
  Reference Point [Bohr]              0.14837053     -0.39198842      0.03538096
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.78324196 Y=  -10.78883767 Z=   -6.79752584     Total=    19.52305352
  Reference Point [Bohr]              0.14861664     -0.39206288      0.03562077
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.77784704 Y=    9.05745314 Z=   19.17206861     Total=    21.73553529
  Reference Point [Bohr]              0.14887015     -0.39215713      0.03587092
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.09807518 Y=    8.31418249 Z=  -11.82468013     Total=    29.83384352
  Reference Point [Bohr]              0.14915688     -0.39225593     -0.13294942
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.18098658 Y=  -24.09007935 Z=  -17.97635118     Total=    30.05850763
  Reference Point [Bohr]              0.14948664     -0.39233125      0.03638302
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.73287595 Y=    3.31927310 Z=   11.66059749     Total=    12.24703910
  Reference Point [Bohr]              0.14985736     -0.39237632      0.03666247
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.15158902 Y=   21.89357850 Z=   15.85213604     Total=    27.11546296
  Reference Point [Bohr]              0.15025663     -0.39240830      0.03696109
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.66128256 Y=   26.00028978 Z=   -8.74647621     Total=    36.88759645
  Reference Point [Bohr]              0.15066448     -0.22334880      0.03727626
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.07289682 Y=   26.38894334 Z=   12.40545425     Total=    30.85020058
  Reference Point [Bohr]              0.15105387     -0.22334160      0.20667209
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.00937321 Y=   26.00556350 Z=    4.63812588     Total=    29.01769442
  Reference Point [Bohr]              0.15140130     -0.22333000      0.20697956
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.31681008 Y=   24.69408380 Z=  -21.03263903     Total=    34.69688012
  Reference Point [Bohr]              0.15172331     -0.39239081      0.20725785
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.73343758 Y=   25.47342785 Z=  -13.82228670     Total=    31.65582993
  Reference Point [Bohr]              0.15205842     -0.39235823      0.20751984
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.36256404 Y=  -21.43598047 Z=    6.91615123     Total=    26.71362297
  Reference Point [Bohr]              0.15244166     -0.39230356      0.20779335
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.90320710 Y=  -11.34232070 Z=    7.12130972     Total=    13.70364559
  Reference Point [Bohr]              0.15288393     -0.22317683      0.20809036
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.39063986 Y=   -7.54115834 Z=   -5.07450404     Total=     9.70134522
  Reference Point [Bohr]             -0.01569537     -0.39221313      0.20840815
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.98021202 Y=   20.36714534 Z=   -8.98572435     Total=    22.45986454
  Reference Point [Bohr]             -0.01517175     -0.39218685      0.20874064
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.43604249 Y=   19.98640724 Z=   15.65455120     Total=    33.88063534
  Reference Point [Bohr]              0.15442455     -0.56123911      0.20908730
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.84625072 Y=   -6.86238050 Z=    9.64989960     Total=    22.25744807
  Reference Point [Bohr]             -0.01413460     -0.56121871      0.20944375
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.93897241 Y=   -5.86032312 Z=  -16.94904217     Total=    22.71361639
  Reference Point [Bohr]             -0.01361897     -0.56119243      0.20979925
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.52294908 Y=   23.09793415 Z=   26.64730597     Total=    41.31380901
  Reference Point [Bohr]              0.15596321     -0.56115826      0.21015626
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.66234086 Y=    5.36975126 Z=   -5.61552489     Total=     7.94554753
  Reference Point [Bohr]              0.15644191     -0.56111845      0.21052153
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.76180813 Y=   12.82542672 Z=   18.38369955     Total=    30.55330844
  Reference Point [Bohr]              0.32597436     -0.56107353      0.21090102
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.32572497 Y=  -11.74196557 Z=   -9.63544303     Total=    18.36671212
  Reference Point [Bohr]              0.15737813     -0.56102843      0.21130063
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.18319847 Y=    9.58097824 Z=   22.41903790     Total=    25.41666274
  Reference Point [Bohr]              0.15789373     -0.56099424      0.21171315
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.33338173 Y=   -6.58794783 Z=    2.69061333     Total=    10.21855882
  Reference Point [Bohr]              0.15844616     -0.56098108      0.21210880
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.01987225 Y=   -0.47011778 Z=  -16.33670730     Total=    16.34348222
  Reference Point [Bohr]              0.32809661     -0.56098478      0.21246375
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.19289909 Y=    4.54044230 Z=  -15.85464370     Total=    25.30519153
  Reference Point [Bohr]              0.32868498     -0.56098052      0.21277918
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.07710320 Y=    8.71592662 Z=  -22.43437643     Total=    26.92814595
  Reference Point [Bohr]              0.32927103     -0.56094866      0.04399443
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.50050125 Y=  -15.38532319 Z=    8.60682622     Total=    31.82863795
  Reference Point [Bohr]              0.32984383     -0.56088894      0.04427698
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.62178196 Y=  -12.37924497 Z=    1.03423639     Total=    19.95884322
  Reference Point [Bohr]              0.33040708     -0.39173629      0.04456551
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.54758933 Y=   -7.14608035 Z=  -26.59686542     Total=    31.14630107
  Reference Point [Bohr]              0.33097012     -0.39165027      0.04484997
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.18987952 Y=    3.43770971 Z=  -23.28112857     Total=    31.66764579
  Reference Point [Bohr]              0.33153335     -0.22249696      0.04512305
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.64878801 Y=  -13.07011485 Z=  -19.82110684     Total=    23.75131795
  Reference Point [Bohr]              0.33208797     -0.05334867      0.21446725
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.99330826 Y=   -6.28468527 Z=   11.71837323     Total=    13.44584761
  Reference Point [Bohr]              0.16355017     -0.05326339      0.04567019
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.97670797 Y=   -2.41036563 Z=  -13.32164484     Total=    27.53468011
  Reference Point [Bohr]              0.33313121     -0.05318162     -0.12311347
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.88018789 Y=    0.01472422 Z=   14.91750111     Total=    16.03460838
  Reference Point [Bohr]              0.33360861     -0.05314398     -0.12279970
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.93091195 Y=  -26.12490002 Z=  -12.09727004     Total=    30.45451289
  Reference Point [Bohr]              0.33406328     -0.05316777     -0.12246860
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.07273911 Y=    2.34463203 Z=  -11.89629622     Total=    20.13335803
  Reference Point [Bohr]              0.33450034     -0.05323707     -0.12214249
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.78602627 Y=  -23.64813386 Z=    1.58839336     Total=    34.29437748
  Reference Point [Bohr]              0.16585217     -0.05332368      0.04722695
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.90560208 Y=  -20.94076307 Z=    1.19974754     Total=    30.32837541
  Reference Point [Bohr]              0.16627592     -0.05341473      0.04748188
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.99982479 Y=  -17.02613072 Z=   25.09705186     Total=    32.99616014
  Reference Point [Bohr]              0.16670677     -0.05352071      0.04770691
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.52688316 Y=   12.99546333 Z=   22.16146567     Total=    34.83571240
  Reference Point [Bohr]              0.16715658     -0.05365066      0.04791811
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.76673922 Y=  -14.96348087 Z=   -8.52510227     Total=    30.99206316
  Reference Point [Bohr]              0.16763303     -0.05379196      0.04813298
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.80645799 Y=  -16.61627345 Z=  -12.61711046     Total=    26.17510523
  Reference Point [Bohr]              0.16813161     -0.05392066      0.04835206
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.09857789 Y=  -14.12290187 Z=  -14.50741008     Total=    31.47479564
  Reference Point [Bohr]             -0.00043222     -0.05402448      0.04856309
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.35583674 Y=   22.92792202 Z=  -24.82668608     Total=    34.21606256
  Reference Point [Bohr]              0.00007941     -0.05410312      0.04877457
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.40941287 Y=  -22.22774876 Z=    0.98922077     Total=    22.29434496
  Reference Point [Bohr]              0.00060661     -0.05415995      0.04902228
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.84154874 Y=   11.76696788 Z=   -1.15184933     Total=    16.73351626
  Reference Point [Bohr]              0.17023822     -0.05419934     -0.11973815
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.98519949 Y=  -10.74238708 Z=   24.87814038     Total=    28.87949026
  Reference Point [Bohr]              0.17082946     -0.05422999     -0.11935717
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.96782228 Y=   20.55610895 Z=   -4.10759855     Total=    26.96911148
  Reference Point [Bohr]              0.17146150     -0.05427563     -0.11892479
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.35690312 Y=   18.66492308 Z=   22.72337601     Total=    31.52317274
  Reference Point [Bohr]              0.17214162     -0.05434907      0.05060721
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.43330626 Y=   15.62261123 Z=   -5.25042974     Total=    23.99068905
  Reference Point [Bohr]              0.17287290     -0.05443595      0.05106704
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.77597073 Y=  -21.62053699 Z=   17.46405466     Total=    30.58866216
  Reference Point [Bohr]              0.17364550     -0.05451009      0.05150390
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.63173176 Y=  -21.76646213 Z=  -12.82193123     Total=    31.99352569
  Reference Point [Bohr]              0.17444806     -0.05456014      0.05190248
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.24600428 Y=   12.10921781 Z=  -13.90414156     Total=    29.67044023
  Reference Point [Bohr]              0.17526977     -0.05459417     -0.11681050
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.51853891 Y=  -10.82653287 Z=   -9.16199575     Total=    14.26400857
  Reference Point [Bohr]              0.17610552     -0.05462169     -0.11648639
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.74881794 Y=   -8.53032195 Z=   -6.34620558     Total=    10.98165369
  Reference Point [Bohr]              0.00788484     -0.22371890     -0.11620065
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.61768958 Y=   20.13958448 Z=   -5.72590767     Total=    32.31748013
  Reference Point [Bohr]              0.00875093     -0.22373810     -0.11594517
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.48370945 Y=   -6.29501769 Z=   -3.77820328     Total=     7.75054065
  Reference Point [Bohr]              0.00961635     -0.22376021     -0.11570501
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.41634033 Y=   22.42796245 Z=  -25.82698190     Total=    39.83558015
  Reference Point [Bohr]              0.01046948     -0.22379203     -0.11547810
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.40724077 Y=   22.88000719 Z=   -2.51150576     Total=    26.63750167
  Reference Point [Bohr]              0.01131491     -0.22382506     -0.11527328
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.26764871 Y=   -5.89816102 Z=   19.07938765     Total=    26.40043614
  Reference Point [Bohr]              0.01217287     -0.22384209     -0.11510408
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.31662114 Y=   -8.72192729 Z=   16.08385593     Total=    21.51344582
  Reference Point [Bohr]              0.01304990     -0.22383194     -0.11497776
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.04973185 Y=   15.00738463 Z=  -11.11015713     Total=    20.74981522
  Reference Point [Bohr]              0.01393148     -0.05471679     -0.11488994
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.20412221 Y=   10.33788600 Z=   -8.34766047     Total=    18.04150551
  Reference Point [Bohr]              0.01480207     -0.05465928     -0.11482917
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.50155939 Y=  -22.96308030 Z=   -5.03262620     Total=    25.74709950
  Reference Point [Bohr]              0.01566753      0.11444173     -0.11477477
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.85936618 Y=   -0.94012546 Z=   26.01866702     Total=    28.20958531
  Reference Point [Bohr]              0.01655353      0.11441891     -0.11470389
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.53867326 Y=   -5.85169611 Z=  -24.44093041     Total=    29.54744986
  Reference Point [Bohr]              0.01747282      0.11437840     -0.28367852
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.36327573 Y=   16.51612785 Z=  -18.90113664     Total=    25.66710291
  Reference Point [Bohr]              0.01842231     -0.05473096      0.05459633
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.18587584 Y=   11.34289814 Z=   -8.90224417     Total=    30.77309108
  Reference Point [Bohr]              0.01938911     -0.05476337      0.05474543
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.18478430 Y=  -20.48058529 Z=  -26.46638900     Total=    33.72590310
  Reference Point [Bohr]              0.02035609     -0.05479058      0.22398603
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.20929275 Y=    0.84525841 Z=  -26.56326143     Total=    35.95012066
  Reference Point [Bohr]              0.02131636     -0.05481011      0.22416595
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.12305416 Y=   16.54565916 Z=  -24.32742795     Total=    29.42104230
  Reference Point [Bohr]              0.02228124     -0.05481515      0.22434885
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.56449928 Y=   11.42907936 Z=  -26.51978774     Total=    38.56768881
  Reference Point [Bohr]              0.02326932     -0.05479743      0.22452820
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.87509374 Y=  -22.16904937 Z=   26.77236049     Total=    39.55370020
  Reference Point [Bohr]              0.02429543     -0.05476204      0.22469171
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.66704697 Y=   -0.68851966 Z=   20.81918445     Total=    32.28584375
  Reference Point [Bohr]              0.02535467     -0.05473187      0.22483624
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.08034665 Y=   22.45418300 Z=   21.14054983     Total=    41.04215340
  Reference Point [Bohr]              0.02641899     -0.05473491      0.22496530
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.39120854 Y=  -10.13455694 Z=   -9.70597562     Total=    25.58317826
  Reference Point [Bohr]              0.02746998     -0.05476908      0.05600015
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.44924216 Y=   -8.12657667 Z=   12.15786578     Total=    22.00982772
  Reference Point [Bohr]              0.02850592     -0.05480773      0.05608976
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.78696951 Y=   20.15835621 Z=  -20.91069165     Total=    32.15115672
  Reference Point [Bohr]              0.02952678     -0.05484738      0.05617399
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.82264563 Y=   17.25989474 Z=    0.82842276     Total=    22.76622662
  Reference Point [Bohr]              0.03052516     -0.05489240      0.05626731
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.80775554 Y=  -14.84921708 Z=   -2.36035251     Total=    21.81640775
  Reference Point [Bohr]              0.03149829     -0.05491702      0.05636638
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.64373510 Y=    8.50538839 Z=   23.83076185     Total=    32.65594343
  Reference Point [Bohr]             -0.13661259     -0.05490257      0.05645034
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.05169883 Y=    3.81727068 Z=   19.87135844     Total=    32.20295104
  Reference Point [Bohr]             -0.13563773     -0.05487602      0.05652434
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.88166129 Y=   10.02895914 Z=   11.55849524     Total=    15.32827976
  Reference Point [Bohr]             -0.13465644     -0.05486284      0.05662629
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.76665079 Y=    3.97280409 Z=  -25.04128852     Total=    25.50497324
  Reference Point [Bohr]             -0.13368592     -0.22394095      0.05677202
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.09980034 Y=  -25.83294293 Z=   22.39186555     Total=    34.32703519
  Reference Point [Bohr]             -0.13272385     -0.22395390      0.05694476
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.36383835 Y=   -0.43951849 Z=   18.96140296     Total=    19.01546827
  Reference Point [Bohr]             -0.13175930     -0.22394326      0.05711914
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.41031315 Y=   23.72647487 Z=   -4.31263825     Total=    24.11872334
  Reference Point [Bohr]             -0.29985697     -0.22388355      0.05727887
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.79199665 Y=   -9.22633562 Z=    3.40137012     Total=     9.86518354
  Reference Point [Bohr]             -0.29886640     -0.22379369      0.05743933
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.85338901 Y=  -13.29611719 Z=   11.01266302     Total=    17.36377061
  Reference Point [Bohr]             -0.29786356     -0.22372586      0.05761251
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.17573125 Y=  -11.54658271 Z=    0.80921387     Total=    12.67937669
  Reference Point [Bohr]             -0.29685242     -0.22370236      0.05778814
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.45871361 Y=   -5.13075262 Z=  -15.30086089     Total=    24.51866788
  Reference Point [Bohr]             -0.29583073     -0.22369982      0.05797618
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.52060871 Y=  -24.18992069 Z=   14.80508668     Total=    31.00174991
  Reference Point [Bohr]             -0.29479776     -0.22369952      0.05818791
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.27018383 Y=   11.05746757 Z=  -14.82134401     Total=    18.53518800
  Reference Point [Bohr]             -0.12468857     -0.22369951      0.05840926
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.56743854 Y=   21.30335484 Z=    8.40815252     Total=    22.90964737
  Reference Point [Bohr]              0.04541374     -0.22370400      0.05861849
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.25531058 Y=  -10.18616983 Z=    5.50914867     Total=    26.87803688
  Reference Point [Bohr]              0.04643190     -0.22371702      0.05880233
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.98020551 Y=   -8.79009405 Z=  -21.59035627     Total=    25.35771557
  Reference Point [Bohr]              0.04743775     -0.22373841      0.05896983
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.00419421 Y=   -8.58886533 Z=    8.82248682     Total=    16.51354509
  Reference Point [Bohr]              0.04842608     -0.22375914      0.05914309
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.19423489 Y=  -15.04718076 Z=   12.85201495     Total=    32.82879648
  Reference Point [Bohr]              0.04940267     -0.22376078      0.05932604
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.02010238 Y=   -1.89778030 Z=   16.41859765     Total=    28.33896668
  Reference Point [Bohr]              0.05038874     -0.22373917      0.05950168
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.14336762 Y=   -9.09573649 Z=  -12.88610646     Total=    21.86562931
  Reference Point [Bohr]              0.05139311     -0.22370034      0.05966576
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.22280863 Y=  -14.38056610 Z=   -9.91408436     Total=    22.52505351
  Reference Point [Bohr]              0.05240528     -0.22364376      0.22888333
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.74014000 Y=   12.66143115 Z=   -8.35133193     Total=    18.58513360
  Reference Point [Bohr]              0.05342098     -0.22357086      0.22900599
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.13350785 Y=  -15.69338668 Z=   -5.44654280     Total=    18.07855492
  Reference Point [Bohr]              0.22350819     -0.22349128      0.22913127
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.15883369 Y=  -19.77032135 Z=   25.13032443     Total=    33.26083353
  Reference Point [Bohr]              0.22449689     -0.22341267      0.22927351
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.71512660 Y=   21.54438906 Z=   25.66554965     Total=    35.84069730
  Reference Point [Bohr]              0.22544374     -0.22333976      0.22941757
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.04631376 Y=   14.73085823 Z=   -3.98692725     Total=    17.74061909
  Reference Point [Bohr]              0.22635663     -0.22325811      0.22954364
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.82509822 Y=   12.65927440 Z=   21.59783842     Total=    25.49520397
  Reference Point [Bohr]              0.22725399     -0.22315271      0.22964302
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.25407944 Y=  -16.48443731 Z=   -5.53762601     Total=    30.66219991
  Reference Point [Bohr]              0.22814979     -0.05394870      0.22971512
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.76703941 Y=  -16.82648531 Z=   -2.75363417     Total=    22.55612028
  Reference Point [Bohr]              0.05997414     -0.05380126      0.22976159
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.69939028 Y=  -15.98503315 Z=    2.88137127     Total=    24.76874607
  Reference Point [Bohr]              0.06087842     -0.05364926      0.22978409
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.10755737 Y=   11.82751658 Z=    9.86599500     Total=    26.12961890
  Reference Point [Bohr]              0.06179134     -0.05349213      0.22977848
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.27271482 Y=  -16.24153885 Z=  -11.12108061     Total=    31.25109123
  Reference Point [Bohr]              0.06271869     -0.05332859      0.22973409
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.86055496 Y=  -16.59708535 Z=   21.72393633     Total=    37.63191404
  Reference Point [Bohr]              0.06366886     -0.05316800      0.22965584
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.44554639 Y=   11.71224082 Z=   -2.90704490     Total=    24.60770113
  Reference Point [Bohr]              0.06463214     -0.05300813      0.22955994
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.63659608 Y=  -14.59515431 Z=   -2.34260824     Total=    16.63802700
  Reference Point [Bohr]              0.06560035     -0.22189747      0.22945404
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.92604847 Y=   16.97709831 Z=   -2.75977275     Total=    18.93833301
  Reference Point [Bohr]              0.06655960     -0.22166925      0.22936341
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.21066498 Y=   22.95974608 Z=   -3.32536086     Total=    30.76814820
  Reference Point [Bohr]              0.06748575     -0.22139970      0.22931837
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.56964848 Y=   25.84445544 Z=   22.80656059     Total=    41.20029266
  Reference Point [Bohr]              0.06837024     -0.22110064      0.22932408
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.09473435 Y=   25.59187625 Z=   18.79096098     Total=    41.73929772
  Reference Point [Bohr]              0.06922945     -0.22078545      0.22937865
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.87900367 Y=   23.44190787 Z=  -16.00111743     Total=    28.79867150
  Reference Point [Bohr]              0.07008583     -0.22046438      0.22947350
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.30771380 Y=   -7.05285600 Z=    4.18541815     Total=    21.90122696
  Reference Point [Bohr]              0.07095322     -0.22014663      0.22957193
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.50573783 Y=  -11.97769688 Z=   27.03241156     Total=    29.90849663
  Reference Point [Bohr]              0.07184344     -0.21983347      0.22963034
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.39261311 Y=  -21.22943037 Z=   23.65248118     Total=    41.95811998
  Reference Point [Bohr]              0.07275213     -0.21950978      0.22964683
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.96313179 Y=   24.12539322 Z=   -1.21744770     Total=    35.46267036
  Reference Point [Bohr]              0.07366364     -0.21916388      0.06058222
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.79088399 Y=   14.71687758 Z=    1.70494043     Total=    15.07588608
  Reference Point [Bohr]              0.07458225     -0.21879751      0.06060871
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.66863873 Y=  -19.88964437 Z=   -7.76259805     Total=    21.85525267
  Reference Point [Bohr]              0.07553109     -0.21842180      0.06065957
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.33725550 Y=    1.89096244 Z=   15.74105158     Total=    24.24069683
  Reference Point [Bohr]              0.07652282     -0.21805059     -0.10833771
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.23926986 Y=   25.25451502 Z=   12.17514307     Total=    30.59124653
  Reference Point [Bohr]              0.07754025     -0.21768312     -0.10823439
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.81047829 Y=   -7.89617013 Z=  -16.99020315     Total=    26.54902257
  Reference Point [Bohr]              0.07855726     -0.21731298     -0.10810692
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.40269325 Y=   -6.02668723 Z=  -12.84513101     Total=    22.45377656
  Reference Point [Bohr]              0.07955361     -0.21695007     -0.10797401
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.70055054 Y=   -5.54651635 Z=   21.15685626     Total=    26.92366427
  Reference Point [Bohr]              0.08052203     -0.21660898     -0.10785367
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.82522654 Y=  -17.23089586 Z=   25.70568388     Total=    31.69021416
  Reference Point [Bohr]              0.08146459     -0.21629657      0.06132551
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.03531982 Y=  -19.82771950 Z=    1.81703125     Total=    20.14083488
  Reference Point [Bohr]             -0.08669134     -0.21600192      0.06140731
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.95842538 Y=  -13.27780164 Z=    6.79108945     Total=    30.80869376
  Reference Point [Bohr]             -0.25486021     -0.21570960      0.06145886
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.00311255 Y=   23.53914704 Z=  -13.59908132     Total=    27.20354188
  Reference Point [Bohr]             -0.25396699     -0.21541233      0.06149000
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.62243058 Y=   -1.38236312 Z=  -10.63057950     Total=    18.13106793
  Reference Point [Bohr]             -0.25309879     -0.21509919      0.06150774
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.55608503 Y=    0.61397377 Z=   -9.71137669     Total=    27.34595552
  Reference Point [Bohr]             -0.25226037     -0.21476547      0.06151178
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.83966658 Y=    3.52505338 Z=   18.59625478     Total=    18.94602157
  Reference Point [Bohr]             -0.25145153     -0.21441534      0.06150311
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.14888603 Y=  -21.10280663 Z=   -4.87827853     Total=    21.76565552
  Reference Point [Bohr]             -0.25067580     -0.21404796      0.06147831
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.77745969 Y=  -19.83359466 Z=    4.10246438     Total=    32.00194056
  Reference Point [Bohr]             -0.24991915     -0.21365647      0.06142647
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.10535254 Y=  -20.31324986 Z=  -17.81801995     Total=    27.33063984
  Reference Point [Bohr]             -0.24914800     -0.21324311      0.06136189
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.20836818 Y=    5.23542857 Z=   14.86417543     Total=    16.93804177
  Reference Point [Bohr]             -0.07928043     -0.21282019      0.06131548
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.17647143 Y=  -25.63311411 Z=   18.88261426     Total=    33.13332594
  Reference Point [Bohr]             -0.07847871     -0.21238728      0.06128154
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.81985879 Y=   24.67448969 Z=   21.72977882     Total=    35.28969409
  Reference Point [Bohr]             -0.07768349     -0.21193193      0.06123182
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.08481764 Y=   -8.34591140 Z=   15.52691578     Total=    29.04562198
  Reference Point [Bohr]             -0.07688744     -0.21143740      0.06115097
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.64473280 Y=   15.60276424 Z=  -18.60366595     Total=    33.89123821
  Reference Point [Bohr]             -0.07606932     -0.21088824      0.06103832
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.97833614 Y=   16.73175537 Z=   20.34274214     Total=    27.24841226
  Reference Point [Bohr]             -0.07521222     -0.21029174      0.22997576
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.90274010 Y=   -8.55700848 Z=   20.37155225     Total=    30.41623052
  Reference Point [Bohr]             -0.07432773     -0.20967352      0.22981954
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.95449820 Y=   -7.73774793 Z=   -3.47231226     Total=    10.96789591
  Reference Point [Bohr]             -0.07345168     -0.20905485      0.22963651
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.37322865 Y=   -7.95900473 Z=    0.02725448     Total=    23.74674418
  Reference Point [Bohr]             -0.07259335     -0.20844101      0.22943282
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.24972463 Y=   19.55566398 Z=  -24.49213169     Total=    39.62748608
  Reference Point [Bohr]             -0.07173375     -0.03876558      0.22922627
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.10709350 Y=   20.23119777 Z=    5.36763611     Total=    21.33028592
  Reference Point [Bohr]             -0.07086680     -0.03818316      0.22903014
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.62174566 Y=   21.25919830 Z=  -21.70260120     Total=    30.49311335
  Reference Point [Bohr]             -0.06999943     -0.03760451      0.22884413
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.91250936 Y=   -4.89442395 Z=   -4.23879349     Total=     6.53876360
  Reference Point [Bohr]             -0.06914752     -0.03701743      0.22865229
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.97216827 Y=   -6.22107213 Z=   -2.61603586     Total=    27.80365522
  Reference Point [Bohr]             -0.06831721     -0.03641717      0.22844457
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.36520517 Y=  -19.47223724 Z=    4.06798680     Total=    33.02787585
  Reference Point [Bohr]             -0.06750407     -0.03582022      0.22822962
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.22733071 Y=   10.16155091 Z=  -22.78674710     Total=    36.92994039
  Reference Point [Bohr]             -0.06671737     -0.03524712      0.22802215
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.40177986 Y=  -14.51304285 Z=  -23.10725636     Total=    37.28034509
  Reference Point [Bohr]             -0.06596313     -0.03468634      0.22782324
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.28020711 Y=  -13.10428032 Z=    4.26638496     Total=    14.43067484
  Reference Point [Bohr]             -0.06524201     -0.03412268      0.22761707
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.45889082 Y=  -14.14895377 Z=  -22.82128891     Total=    37.69717527
  Reference Point [Bohr]             -0.06455222     -0.03354656      0.22739635
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.91576166 Y=  -17.45443062 Z=    6.17669590     Total=    19.43720547
  Reference Point [Bohr]             -0.06389227     -0.20201898      0.22718275
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.79599290 Y=    4.90385460 Z=    8.95029779     Total=    14.14627503
  Reference Point [Bohr]             -0.06326345     -0.20138977      0.22700712
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.39405174 Y=    7.93106303 Z=  -15.78671839     Total=    25.50418353
  Reference Point [Bohr]             -0.06265241     -0.20075381      0.05781117
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.19825438 Y=   19.50516780 Z=  -12.92224016     Total=    32.94836670
  Reference Point [Bohr]              0.10702337     -0.20013643      0.05774180
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.14820904 Y=   -6.90724595 Z=  -14.76965679     Total=    16.30566693
  Reference Point [Bohr]              0.10761607     -0.19953004      0.05771357
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.78385317 Y=   -7.87123640 Z=   13.17491612     Total=    27.47068879
  Reference Point [Bohr]             -0.06086253     -0.19891140      0.05771144
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.04118994 Y=   -1.12303155 Z=    8.57963551     Total=    10.01423693
  Reference Point [Bohr]             -0.06025670     -0.19826810      0.05773287
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.07096289 Y=  -26.36179614 Z=    7.11487222     Total=    29.85420988
  Reference Point [Bohr]             -0.05964062     -0.19760584      0.05778276
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.04250316 Y=    7.56380050 Z=    6.70813844     Total=    15.72361542
  Reference Point [Bohr]             -0.05902458     -0.19693931      0.05785299
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.18441678 Y=   17.81406650 Z=    8.05101667     Total=    22.04273530
  Reference Point [Bohr]             -0.05841694     -0.19628336      0.05792537
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.96913549 Y=   -1.25503812 Z=  -11.46840302     Total=    22.20197040
  Reference Point [Bohr]             -0.05781335     -0.19563159      0.22706730
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.66668221 Y=  -20.01576672 Z=  -24.08737422     Total=    38.66019913
  Reference Point [Bohr]             -0.05721014     -0.19495915      0.22713744
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.06811479 Y=  -15.00320097 Z=  -21.94139244     Total=    35.19458285
  Reference Point [Bohr]             -0.05660472     -0.19426238      0.22721153
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.13069992 Y=  -14.91685385 Z=    4.50699265     Total=    21.03573606
  Reference Point [Bohr]             -0.22505847     -0.19356019      0.22727978
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.25125048 Y=  -13.06743873 Z=  -26.12844918     Total=    31.30566161
  Reference Point [Bohr]             -0.22441095     -0.19287070      0.22733094
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.98816060 Y=   -6.40664343 Z=    1.32785667     Total=    16.35399773
  Reference Point [Bohr]             -0.22374346     -0.19219946      0.22737071
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.56354336 Y=    0.05897643 Z=    3.06254893     Total=    12.93156239
  Reference Point [Bohr]             -0.05399786     -0.19153025      0.22740750
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.85737987 Y=  -24.24998265 Z=  -23.47394003     Total=    35.16042458
  Reference Point [Bohr]             -0.05332545     -0.19084288      0.05836663
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.53469737 Y=    4.73592647 Z=    4.30575631     Total=    21.50912209
  Reference Point [Bohr]             -0.05267146     -0.19013446      0.05840981
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.57365746 Y=  -23.83265157 Z=  -22.89127053     Total=    33.36051394
  Reference Point [Bohr]             -0.05206526     -0.18940709      0.05847496
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.13160188 Y=    0.00991776 Z=    4.97307380     Total=     8.69432613
  Reference Point [Bohr]             -0.05150855     -0.18864949      0.05855210
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.72448535 Y=  -11.09890030 Z=  -20.80913139     Total=    26.79772499
  Reference Point [Bohr]             -0.05097577     -0.18785951      0.05863576
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.66888239 Y=   -5.45673792 Z=    8.59063686     Total=    15.48347011
  Reference Point [Bohr]             -0.05044923     -0.18705775      0.05873552
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.94912787 Y=   -0.53319637 Z=    9.01915470     Total=    15.78953332
  Reference Point [Bohr]             -0.04992110     -0.18626330      0.05885589
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.50116031 Y=    1.25311259 Z=   10.94518233     Total=    18.21128655
  Reference Point [Bohr]             -0.04938964     -0.18547744      0.05898526
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.57675174 Y=    0.65796993 Z=   -8.13335186     Total=    11.13514723
  Reference Point [Bohr]             -0.04885108     -0.18469430      0.05912134
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.87247182 Y=    1.12188482 Z=    1.53879084     Total=    17.97364047
  Reference Point [Bohr]             -0.04828844     -0.18391898      0.05927804
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.41663173 Y=  -21.24802180 Z=    5.43941898     Total=    35.11036036
  Reference Point [Bohr]             -0.04769718     -0.18316272      0.05945247
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.92945973 Y=  -12.69217489 Z=  -20.23206315     Total=    24.20471724
  Reference Point [Bohr]             -0.04709040     -0.18242940      0.05963435
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.94158763 Y=   17.68125701 Z=  -19.52416674     Total=    33.03765812
  Reference Point [Bohr]             -0.04648034     -0.18171163      0.05981616
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.27546277 Y=   17.23908402 Z=  -19.58577343     Total=    30.23455476
  Reference Point [Bohr]             -0.04587962     -0.18099329      0.05997822
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.60617282 Y=  -11.61363138 Z=    7.60118598     Total=    25.68036538
  Reference Point [Bohr]             -0.04530233     -0.18026859      0.06011168
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.01172256 Y=   14.88896423 Z=  -20.58620265     Total=    25.48568271
  Reference Point [Bohr]             -0.04476455     -0.17953186      0.06021694
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.32486712 Y=  -12.73836417 Z=  -22.45703293     Total=    34.79416152
  Reference Point [Bohr]             -0.04425810     -0.17875974      0.06029477
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.03337937 Y=  -11.81957427 Z=  -26.42973965     Total=    29.57423102
  Reference Point [Bohr]             -0.04374823     -0.17794534      0.06035076
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.01321605 Y=  -10.02436402 Z=   -4.97945953     Total=    21.20751857
  Reference Point [Bohr]             -0.04322555     -0.17712089      0.06038412
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.11981912 Y=   19.76099601 Z=   -9.85269811     Total=    25.18854182
  Reference Point [Bohr]             -0.04269662     -0.17632706      0.06039237
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.38145233 Y=   -5.30459289 Z=  -12.08079547     Total=    25.98102641
  Reference Point [Bohr]             -0.21124321     -0.17557958      0.06038219
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.26064210 Y=   -3.70967227 Z=  -14.01892636     Total=    16.21754877
  Reference Point [Bohr]             -0.21073127     -0.17487672      0.06036237
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.90192658 Y=   22.79793376 Z=  -15.74921435     Total=    32.98882405
  Reference Point [Bohr]             -0.04115006     -0.17421205      0.06034049
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.07593409 Y=   18.90898000 Z=   12.34110299     Total=    25.15012253
  Reference Point [Bohr]              0.12845031     -0.17357066      0.06032303
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.14221807 Y=  -13.42616058 Z=   16.26741087     Total=    25.96492273
  Reference Point [Bohr]              0.12899942     -0.17293417      0.06031508
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.24629987 Y=   10.73211942 Z=   21.94955301     Total=    27.33007730
  Reference Point [Bohr]              0.12954945     -0.17230237      0.22939375
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.24380017 Y=  -17.95867328 Z=   26.88336281     Total=    33.91407649
  Reference Point [Bohr]              0.13007825     -0.17169119      0.22940812
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.86208709 Y=    9.97823470 Z=    2.96945714     Total=    14.34027912
  Reference Point [Bohr]              0.13058319     -0.17110363      0.22943578
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.89017668 Y=   10.99761985 Z=    4.26946476     Total=    16.05527701
  Reference Point [Bohr]              0.13106817     -0.17053176      0.22949037
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.36804486 Y=  -16.40599665 Z=    3.33153382     Total=    22.06120025
  Reference Point [Bohr]              0.13153418     -0.33905253      0.22957237
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.81388455 Y=  -18.56463272 Z=    3.06404697     Total=    25.23372120
  Reference Point [Bohr]              0.13199423     -0.33852215      0.22967843
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.37107859 Y=    5.20541460 Z=    5.84013600     Total=     8.96157674
  Reference Point [Bohr]              0.13245911     -0.33799902      0.22980751
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.98769192 Y=  -27.01147374 Z=  -19.32076975     Total=    40.96731893
  Reference Point [Bohr]              0.13291066     -0.33746640      0.22994416
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.10186776 Y=   -6.29529477 Z=  -18.89114530     Total=    26.91066189
  Reference Point [Bohr]              0.13332687     -0.33692580      0.23006336
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.31561140 Y=   14.47839724 Z=    7.35861166     Total=    21.00187276
  Reference Point [Bohr]              0.13370669     -0.33638128      0.23015815
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.22616101 Y=   14.33654630 Z=   19.05091627     Total=    27.26545994
  Reference Point [Bohr]              0.13407589     -0.50489591      0.23023540
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.67113410 Y=  -10.60164487 Z=  -18.84722350     Total=    29.91502118
  Reference Point [Bohr]              0.13446078     -0.50431608      0.23030029
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.18087987 Y=    1.45240202 Z=  -18.28805297     Total=    18.38360221
  Reference Point [Bohr]              0.13485951     -0.50372748      0.23035551
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.15245103 Y=    0.80402295 Z=  -15.31745289     Total=    30.31866605
  Reference Point [Bohr]              0.13527038     -0.50314488      0.23040548
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.57866346 Y=   27.39375763 Z=   11.77368281     Total=    29.92803150
  Reference Point [Bohr]              0.13569022     -0.33349305      0.23044911
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.08946619 Y=   16.87773350 Z=    7.91651572     Total=    19.08540917
  Reference Point [Bohr]              0.13611852     -0.33291649      0.23048668
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.41811612 Y=  -14.93556895 Z=    0.32138462     Total=    15.89120795
  Reference Point [Bohr]              0.13656558     -0.33234046      0.23052392
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.25093099 Y=    8.70368791 Z=   25.62847466     Total=    27.06724705
  Reference Point [Bohr]              0.13702735     -0.33176257      0.23056546
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.86047704 Y=    9.84921373 Z=   -0.77403883     Total=    10.05323440
  Reference Point [Bohr]              0.13749533     -0.33118645      0.23060749
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.30979738 Y=   12.45420532 Z=  -22.93737751     Total=    36.35679249
  Reference Point [Bohr]              0.13797401     -0.33060792      0.23064413
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.52554837 Y=   14.90071150 Z=   10.90288970     Total=    29.12566800
  Reference Point [Bohr]              0.13845981     -0.33001655      0.23067557
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.97305141 Y=  -17.90290332 Z=  -11.85719292     Total=    22.90581848
  Reference Point [Bohr]              0.13892749     -0.16033735      0.23069957
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.22348317 Y=    7.27990745 Z=  -11.24031336     Total=    20.27550583
  Reference Point [Bohr]             -0.02971752     -0.15972244      0.23071611
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.59371029 Y=   24.57398291 Z=  -14.83848457     Total=    30.59882282
  Reference Point [Bohr]             -0.02932367     -0.15910494      0.23073836
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.99339882 Y=  -11.35709294 Z=    6.68238961     Total=    15.41208343
  Reference Point [Bohr]             -0.02894961     -0.15849637      0.39985186
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.23670355 Y=    8.54173944 Z=   26.17556913     Total=    32.48423742
  Reference Point [Bohr]             -0.02858681     -0.15790006      0.39990905
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.84956483 Y=  -22.32104439 Z=  -14.80940190     Total=    26.85085283
  Reference Point [Bohr]             -0.02823143     -0.15730486      0.39997095
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.07326011 Y=   22.01070985 Z=   26.88145769     Total=    44.04594792
  Reference Point [Bohr]             -0.02788274     -0.15670773      0.23095251
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.45748972 Y=   19.82640153 Z=   19.34751491     Total=    27.70598902
  Reference Point [Bohr]             -0.02754625     -0.15611943      0.23101004
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.13660071 Y=  -10.11850507 Z=  -14.48495965     Total=    22.01745851
  Reference Point [Bohr]             -0.02722787     -0.15553721      0.23109040
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.42953904 Y=  -11.59786936 Z=  -20.38590612     Total=    33.15175775
  Reference Point [Bohr]             -0.02693485     -0.15495497      0.23119929
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.55592301 Y=   16.28061445 Z=  -24.07239309     Total=    30.02716251
  Reference Point [Bohr]             -0.02667605     -0.15438933      0.23133293
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.02311164 Y=   -7.58541110 Z=  -21.74580309     Total=    25.11734820
  Reference Point [Bohr]             -0.02644342     -0.15385092      0.06241818
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.24733879 Y=  -24.59668448 Z=  -12.46218481     Total=    38.76493788
  Reference Point [Bohr]              0.14285344     -0.15331448      0.06260436
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.75039423 Y=   14.35210312 Z=  -11.00104435     Total=    19.67420777
  Reference Point [Bohr]             -0.02598693     -0.15274095      0.06280928
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.24252194 Y=   -4.29465214 Z=  -10.59632850     Total=    19.86317532
  Reference Point [Bohr]             -0.02572413     -0.15212200      0.06301509
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.94741143 Y=    5.49654562 Z=   17.19632642     Total=    22.21623548
  Reference Point [Bohr]             -0.02542945     -0.15148528      0.06321476
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.02747293 Y=    7.97999777 Z=  -10.10360344     Total=    16.95194166
  Reference Point [Bohr]             -0.02511317     -0.15085053      0.06341942
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.02771567 Y=  -21.04068067 Z=   16.67256285     Total=    38.09438291
  Reference Point [Bohr]             -0.02479048     -0.15021607      0.06364626
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.76816792 Y=  -25.48631065 Z=  -14.15226840     Total=    29.39452025
  Reference Point [Bohr]             -0.02446209     -0.14958522      0.06390157
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.60231232 Y=   25.38396820 Z=  -20.82667381     Total=    37.73780872
  Reference Point [Bohr]             -0.19317493     -0.14895918      0.06417714
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.84810158 Y=   -0.27058295 Z=    1.16140413     Total=    13.89935222
  Reference Point [Bohr]             -0.19277364     -0.14832326      0.06446657
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.31881868 Y=  -25.55994426 Z=    3.29064048     Total=    28.56382956
  Reference Point [Bohr]             -0.19235710     -0.14765524      0.06476094
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.32600828 Y=   25.91912187 Z=    6.84424896     Total=    31.91919776
  Reference Point [Bohr]             -0.02286624     -0.14693772      0.06504205
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.31936769 Y=   -3.20339520 Z=  -20.16896290     Total=    27.43443161
  Reference Point [Bohr]             -0.02245782     -0.14617433      0.06531191
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.76422255 Y=   -9.78989369 Z=    5.77423406     Total=    13.22643202
  Reference Point [Bohr]             -0.02206086     -0.14538369      0.06560624
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.95897055 Y=   22.20483158 Z=  -20.04608099     Total=    32.21671747
  Reference Point [Bohr]             -0.02165662     -0.14457587      0.06595660
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.61726955 Y=   -1.15238046 Z=  -23.88498981     Total=    25.41806549
  Reference Point [Bohr]             -0.02122706     -0.14374943      0.06634974
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.06863373 Y=    3.48750660 Z=   23.81333111     Total=    31.98632158
  Reference Point [Bohr]             -0.02076744     -0.14290642      0.06675555
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.88554439 Y=    9.22779278 Z=  -10.60302005     Total=    26.01063719
  Reference Point [Bohr]             -0.02029828     -0.48021116      0.06716568
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.01548741 Y=  -12.85116142 Z=   11.99061334     Total=    27.39667624
  Reference Point [Bohr]             -0.01984380     -0.47938991      0.06757611
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.29400552 Y=   -8.10569888 Z=    0.42298516     Total=    22.78850460
  Reference Point [Bohr]             -0.01940501     -0.47859654      0.06798826
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.62136746 Y=   -1.93580830 Z=   21.70683357     Total=    21.85321051
  Reference Point [Bohr]             -0.01897180     -0.47783315      0.06841342
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.30585553 Y=  -21.18244816 Z=   -3.19667189     Total=    33.92510658
  Reference Point [Bohr]             -0.01854128     -0.47710449      0.06886460
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.59569751 Y=   10.41926546 Z=    1.51526390     Total=    25.83822862
  Reference Point [Bohr]             -0.01810999     -0.47639306      0.06934671
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.78025094 Y=   11.52239713 Z=    5.90420854     Total=    13.80130839
  Reference Point [Bohr]             -0.01766695     -0.30658951      0.06984420
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.85459943 Y=  -16.06217401 Z=  -18.74730677     Total=    24.85163341
  Reference Point [Bohr]             -0.01720847     -0.13674853      0.07034915
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.11351454 Y=  -16.84227414 Z=   10.74398333     Total=    19.97769410
  Reference Point [Bohr]             -0.01674266     -0.13594278      0.07086970
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.98716384 Y=    9.19765181 Z=  -15.12529977     Total=    17.81348680
  Reference Point [Bohr]             -0.18535195     -0.13510487      0.07139873
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.66020098 Y=  -20.14391308 Z=   13.48171524     Total=    35.29843898
  Reference Point [Bohr]             -0.18489307     -0.13425515      0.07192314
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.26496897 Y=    5.15495505 Z=  -11.73138383     Total=    13.50514304
  Reference Point [Bohr]             -0.18443830     -0.13341614     -0.09663022
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.39319678 Y=  -25.39959885 Z=  -10.22644618     Total=    31.41130896
  Reference Point [Bohr]             -0.18397845     -0.13258572     -0.09609957
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.56074826 Y=   26.15640100 Z=  -10.88055141     Total=    29.59442723
  Reference Point [Bohr]             -0.01443522     -0.13175167     -0.09555212
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.48360094 Y=   23.89469446 Z=  -12.91594166     Total=    27.92516882
  Reference Point [Bohr]             -0.01397169     -0.13091113     -0.26406495
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.80675489 Y=   23.90020182 Z=   13.01729175     Total=    32.52306953
  Reference Point [Bohr]             -0.18260853     -0.13007186     -0.26348592
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.57603576 Y=   21.01264659 Z=   15.04334274     Total=    30.17360382
  Reference Point [Bohr]             -0.18219476     -0.12924072     -0.09380846
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.23873090 Y=  -16.04056885 Z=   14.78532088     Total=    25.01383811
  Reference Point [Bohr]             -0.18177558     -0.12841369     -0.09317977
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.64486779 Y=   11.30137458 Z=   12.36061624     Total=    20.98567566
  Reference Point [Bohr]             -0.18132527     -0.12758804      0.07654662
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.50816767 Y=  -15.74069817 Z=  -18.37213979     Total=    28.73688160
  Reference Point [Bohr]             -0.18084826     -0.12677103      0.07720673
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.08010223 Y=  -16.47876594 Z=  -23.36490940     Total=    33.30463347
  Reference Point [Bohr]             -0.18037111     -0.12597348      0.24692132
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.34362007 Y=    4.76105112 Z=  -27.44842443     Total=    30.88908882
  Reference Point [Bohr]             -0.01083247     -0.12519088      0.24753265
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.82075248 Y=    4.37881533 Z=   10.71866781     Total=    27.38856726
  Reference Point [Bohr]             -0.01037180     -0.12441243      0.24811791
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.45180367 Y=  -23.82285208 Z=    6.87525706     Total=    25.89067050
  Reference Point [Bohr]             -0.00992062     -0.29272038      0.07960989
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.99079420 Y=  -23.99066552 Z=    5.39507583     Total=    29.88889363
  Reference Point [Bohr]             -0.00949201     -0.29198866      0.08016306
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.16149216 Y=    3.68726034 Z=  -18.52196927     Total=    23.01921177
  Reference Point [Bohr]             -0.00908812     -0.29130285      0.08070831
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.92411335 Y=    3.22199238 Z=   17.88866826     Total=    26.23943126
  Reference Point [Bohr]             -0.00870745     -0.29066055      0.08124771
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.75967503 Y=    1.15143019 Z=   26.64639193     Total=    26.93494293
  Reference Point [Bohr]             -0.00834202     -0.29005570      0.08177312
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.35045539 Y=   25.71835373 Z=  -18.99790569     Total=    32.00277908
  Reference Point [Bohr]             -0.00798228     -0.28947854      0.08229269
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.43311584 Y=   25.34657876 Z=   -8.42347476     Total=    27.72463152
  Reference Point [Bohr]             -0.00762183     -0.28890413      0.08281519
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.65826378 Y=  -27.15878627 Z=  -26.04870789     Total=    40.03352375
  Reference Point [Bohr]             -0.00725176     -0.28832647      0.08333772
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.99540449 Y=    4.25356248 Z=    8.62743982     Total=    13.16976893
  Reference Point [Bohr]             -0.00687188     -0.11868927      0.08386049
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.96386046 Y=    8.02266358 Z=  -15.15222592     Total=    27.08203328
  Reference Point [Bohr]             -0.00649450     -0.11813840      0.08438798
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.28183707 Y=  -17.24234378 Z=  -14.70637955     Total=    30.41264430
  Reference Point [Bohr]             -0.00612770     -0.11757912      0.08491924
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.51997125 Y=  -16.80747339 Z=  -16.44230410     Total=    27.63458143
  Reference Point [Bohr]             -0.00576694     -0.11699158      0.08545081
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.69937982 Y=    7.94507619 Z=    5.80009337     Total=    24.73918274
  Reference Point [Bohr]             -0.00540622     -0.11637723      0.08598826
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.48817100 Y=  -24.76739894 Z=    7.50356335     Total=    34.94884390
  Reference Point [Bohr]             -0.00504697     -0.11575762      0.25560659
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.26999842 Y=   -1.87542301 Z=   12.09269964     Total=    22.82725203
  Reference Point [Bohr]             -0.00469668     -0.11515260      0.25614495
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.70172869 Y=   20.89073664 Z=    9.68062941     Total=    29.04287627
  Reference Point [Bohr]             -0.00436496     -0.28362242      0.25665593
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.35225706 Y=   -2.38030497 Z=    7.76048622     Total=     8.12496666
  Reference Point [Bohr]             -0.00405168     -0.28298550      0.25712198
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.07540845 Y=    1.94025873 Z=  -19.83697372     Total=    20.03939746
  Reference Point [Bohr]             -0.00374168     -0.28230689      0.25753805
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.54598970 Y=   25.98970601 Z=  -18.81511268     Total=    32.12263015
  Reference Point [Bohr]             -0.00342445     -0.28160350      0.25790619
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.67708101 Y=   -5.60299570 Z=   10.71339863     Total=    12.96323870
  Reference Point [Bohr]              0.16595978     -0.28088825      0.08918230
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.21785601 Y=   17.49010362 Z=   13.67264672     Total=    30.02676630
  Reference Point [Bohr]              0.16623441     -0.28015767      0.08955796
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.66202454 Y=  -14.42666875 Z=  -10.60397774     Total=    25.14995480
  Reference Point [Bohr]              0.16645815     -0.27941465     -0.07910189
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.11229937 Y=    9.19452821 Z=   18.93120375     Total=    23.79943322
  Reference Point [Bohr]              0.16664837     -0.27868143     -0.24773897
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.40007225 Y=  -21.07711087 Z=   -8.40117073     Total=    28.59347454
  Reference Point [Bohr]              0.16683377     -0.27797502     -0.24729799
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.19012143 Y=  -21.58783490 Z=   17.68360678     Total=    28.81739771
  Reference Point [Bohr]              0.16702863     -0.10821691     -0.24686817
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.19668338 Y=    3.80884517 Z=   15.11685654     Total=    15.91368712
  Reference Point [Bohr]              0.16722859     -0.10753939     -0.24645824
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.70615538 Y=   21.83167074 Z=   11.45090383     Total=    36.34506543
  Reference Point [Bohr]              0.16741481     -0.10685987     -0.24605145
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.03948173 Y=   11.58760151 Z=    6.38958961     Total=    13.83534520
  Reference Point [Bohr]              0.16757431     -0.10617730     -0.24563947
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.24525278 Y=  -21.31084538 Z=  -24.11296194     Total=    32.78094334
  Reference Point [Bohr]              0.16770793     -0.10549917     -0.24522257
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.76406493 Y=  -23.26990961 Z=  -14.53244603     Total=    35.01935469
  Reference Point [Bohr]              0.16782062     -0.27390843     -0.24480057
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.16553608 Y=  -22.53836838 Z=  -16.81265391     Total=    28.14252752
  Reference Point [Bohr]              0.16791383     -0.27325190      0.09376631
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.80201693 Y=  -21.08480751 Z=  -21.06811852     Total=    38.77595608
  Reference Point [Bohr]              0.16797694     -0.44165612      0.09417582
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.91290290 Y=    7.82086701 Z=    3.03688967     Total=    26.28766613
  Reference Point [Bohr]             -0.00106236     -0.27189659      0.09458924
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.47786214 Y=  -18.35156560 Z=  -27.37255546     Total=    42.27427038
  Reference Point [Bohr]             -0.17010913     -0.27121854      0.09501790
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.60264066 Y=  -17.39439353 Z=   -1.18304120     Total=    17.80290798
  Reference Point [Bohr]             -0.17006358     -0.27057208      0.09545816
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.02811587 Y=   10.95390612 Z=   -0.28656013     Total=    13.58384410
  Reference Point [Bohr]             -0.33906130     -0.26995447      0.09589759
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.29948092 Y=   13.22321865 Z=    0.39323343     Total=    14.25105758
  Reference Point [Bohr]             -0.33896440     -0.26936111      0.09631636
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.01652860 Y=  -19.84130076 Z=  -17.66801423     Total=    30.51773376
  Reference Point [Bohr]             -0.33885636     -0.26879817      0.09670051
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.45805253 Y=   27.45120823 Z=  -19.52917338     Total=    33.77868364
  Reference Point [Bohr]             -0.33873847     -0.26826259      0.09705119
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.05841656 Y=   26.19361769 Z=  -22.50517374     Total=    35.70214787
  Reference Point [Bohr]             -0.33860757     -0.26774575      0.09737637
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.40149969 Y=    4.18572055 Z=  -23.57912933     Total=    25.37874689
  Reference Point [Bohr]             -0.33846091     -0.26723152      0.09768457
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.57118573 Y=   -1.26936845 Z=    0.83531777     Total=    18.63324962
  Reference Point [Bohr]             -0.33829355     -0.26670210     -0.07109195
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.34431358 Y=   -7.40742136 Z=   -7.84522343     Total=    23.91646178
  Reference Point [Bohr]             -0.33809870     -0.26615762     -0.07080760
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.24814524 Y=   18.06014512 Z=   22.99616257     Total=    39.96815925
  Reference Point [Bohr]             -0.33787173     -0.26561233     -0.07053241
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.29824925 Y=  -10.38968021 Z=   -6.10521829     Total=    12.79429919
  Reference Point [Bohr]             -0.33761057     -0.09599940     -0.07026988
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.19524113 Y=  -11.40220259 Z=   19.35214701     Total=    32.28831103
  Reference Point [Bohr]             -0.33732405     -0.09546428     -0.07003445
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.27302987 Y=  -12.89630813 Z=   -7.84624816     Total=    30.30099787
  Reference Point [Bohr]             -0.33702509     -0.09493611     -0.06982516
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.52085655 Y=   12.12223436 Z=   19.95194379     Total=    23.60985086
  Reference Point [Bohr]             -0.33671268     -0.09441716     -0.06962139
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.14507421 Y=    9.10444789 Z=   -9.15574111     Total=    23.09225916
  Reference Point [Bohr]             -0.16730133     -0.09390743      0.09965873
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.02994224 Y=  -21.06908764 Z=    5.92976176     Total=    25.47249347
  Reference Point [Bohr]             -0.16692693     -0.09341559      0.09985995
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.80864071 Y=  -14.37567202 Z=    1.57330774     Total=    26.16776744
  Reference Point [Bohr]             -0.16651073     -0.09295225      0.10004903
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.94960463 Y=   11.53650592 Z=    4.09253553     Total=    17.10651534
  Reference Point [Bohr]              0.00301828     -0.09250809      0.10022574
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.03865039 Y=  -18.73922533 Z=    7.15926260     Total=    22.89684278
  Reference Point [Bohr]              0.00350121     -0.09205338      0.10038957
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.51306632 Y=   26.76687690 Z=  -20.33435397     Total=    33.91635915
  Reference Point [Bohr]              0.00399888     -0.09157621      0.10054247
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.08943610 Y=   -7.74522029 Z=   19.29485144     Total=    20.79153021
  Reference Point [Bohr]              0.00450743     -0.09110409      0.10070218
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.31612154 Y=  -13.59104896 Z=   18.94782756     Total=    35.91527916
  Reference Point [Bohr]              0.00503179     -0.09066684      0.10088226
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.98877445 Y=    7.56991177 Z=   15.09113891     Total=    26.16480731
  Reference Point [Bohr]              0.00558208     -0.09026337      0.10107762
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.83288581 Y=    0.99991551 Z=   18.54964144     Total=    28.66642516
  Reference Point [Bohr]              0.00616576     -0.08987395      0.10127512
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.82297772 Y=   16.51801780 Z=   -6.62755403     Total=    30.54422379
  Reference Point [Bohr]              0.00678444     -0.08947503      0.10147465
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.18633779 Y=   11.73744158 Z=   -4.57091990     Total=    29.96260680
  Reference Point [Bohr]              0.00743113     -0.08905835      0.10168863
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.59031260 Y=   12.09086739 Z=   -3.22620733     Total=    13.32923320
  Reference Point [Bohr]              0.00808478     -0.08863558      0.10191767
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.45428162 Y=   12.33234867 Z=   -3.84139509     Total=    21.71393762
  Reference Point [Bohr]              0.00872337     -0.08822216      0.10216870
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.94507354 Y=   10.17472259 Z=   21.41012997     Total=    26.54436714
  Reference Point [Bohr]              0.00933662     -0.08784674      0.10245536
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.98665907 Y=  -21.22845008 Z=   18.81797603     Total=    34.70201515
  Reference Point [Bohr]              0.00992003     -0.08752755      0.27184254
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.63894654 Y=  -25.51755133 Z=   17.60339527     Total=    31.34557028
  Reference Point [Bohr]              0.01046984     -0.08724099      0.27216042
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.09678884 Y=   -3.06658738 Z=   -9.56261947     Total=    10.50893670
  Reference Point [Bohr]              0.01098847     -0.08695105      0.27247147
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.64286654 Y=   -8.60446771 Z=   -9.65403947     Total=    12.94799676
  Reference Point [Bohr]              0.01149128     -0.08664251      0.10371149
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.17853458 Y=  -11.00347760 Z=   16.90731978     Total=    23.56375789
  Reference Point [Bohr]              0.01199653     -0.08632167      0.10403595
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.69295403 Y=   17.97373752 Z=   14.64108249     Total=    27.44630093
  Reference Point [Bohr]              0.01250043     -0.08600472      0.10436294
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.28848469 Y=   -5.36892073 Z=   11.61997489     Total=    19.18358467
  Reference Point [Bohr]              0.18206165     -0.08570483      0.10468706
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.15926005 Y=  -26.40650666 Z=  -18.00036428     Total=    34.95427518
  Reference Point [Bohr]              0.18253110     -0.08542077      0.10501496
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.88124611 Y=    5.41741084 Z=  -20.41797276     Total=    24.74203818
  Reference Point [Bohr]              0.18297942     -0.08514525      0.10534863
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.59501766 Y=  -20.03729015 Z=    0.50299862     Total=    23.67235675
  Reference Point [Bohr]              0.18339057     -0.08487684      0.10567711
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.99449344 Y=    8.75908282 Z=   21.95155057     Total=    28.53797338
  Reference Point [Bohr]              0.18375839     -0.08461305      0.10599458
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.36338535 Y=    6.49077297 Z=   -5.76188280     Total=    14.29880952
  Reference Point [Bohr]              0.18410200     -0.08434059      0.10630972
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.71161972 Y=   13.18362625 Z=   18.62390665     Total=    31.49686224
  Reference Point [Bohr]              0.18444508     -0.08404881      0.10663802
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.47158080 Y=  -17.01337712 Z=   17.74940480     Total=    36.12811871
  Reference Point [Bohr]              0.18479750     -0.08374893      0.10699840
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.13541736 Y=    8.53060510 Z=   -9.67097014     Total=    13.27138760
  Reference Point [Bohr]              0.18516790     -0.08344874      0.10739175
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.95730755 Y=  -20.58646388 Z=   18.73386265     Total=    31.13786343
  Reference Point [Bohr]              0.18555564     -0.08314769      0.10779149
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.03093097 Y=  -22.67915087 Z=   20.26371458     Total=    30.41320387
  Reference Point [Bohr]              0.01687217     -0.25192729      0.10817551
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.05496366 Y=  -25.26803753 Z=  -23.33645665     Total=    34.76516342
  Reference Point [Bohr]              0.01726164     -0.25164699      0.10854834
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.59042294 Y=    0.87158965 Z=  -11.85075317     Total=    23.77321047
  Reference Point [Bohr]              0.01765144     -0.42045405      0.10893280
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.12347370 Y=  -25.48962957 Z=  -10.89523432     Total=    33.67691483
  Reference Point [Bohr]              0.01802532     -0.42018704      0.10934389
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.93033597 Y=    5.35722603 Z=  -11.26037456     Total=    15.94074899
  Reference Point [Bohr]              0.01837779     -0.41991032      0.10978537
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.42635069 Y=    8.25503145 Z=  -13.84396289     Total=    19.19660495
  Reference Point [Bohr]              0.01873172     -0.41964398      0.11026021
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.09450868 Y=    8.90293706 Z=    8.74094907     Total=    21.97902917
  Reference Point [Bohr]              0.01910734     -0.41941000      0.11076616
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.28690957 Y=  -19.21364454 Z=  -23.36887777     Total=    36.42564048
  Reference Point [Bohr]             -0.14957569     -0.41920731      0.11130583
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.71591313 Y=    7.75518955 Z=  -26.51145688     Total=    35.76329152
  Reference Point [Bohr]             -0.14918572     -0.41903345      0.11188576
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.50352324 Y=  -19.28635823 Z=   -1.29604851     Total=    19.64479653
  Reference Point [Bohr]             -0.14879819     -0.41889605      0.11250171
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.34858735 Y=   10.23428949 Z=   22.49389045     Total=    34.69249912
  Reference Point [Bohr]             -0.31747986     -0.41878830      0.11314297
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.69542136 Y=  -13.01732861 Z=   13.49488429     Total=    30.21648126
  Reference Point [Bohr]             -0.31707963     -0.41868873      0.11379892
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.80582769 Y=   -6.54733250 Z=  -19.52686612     Total=    21.39798352
  Reference Point [Bohr]             -0.31667586     -0.41859164      0.11445958
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.47286620 Y=   -2.40231514 Z=  -22.80989003     Total=    26.10813269
  Reference Point [Bohr]             -0.31628471     -0.41850082      0.11512482
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.71326244 Y=   -1.88511738 Z=   -0.47151924     Total=    25.78658301
  Reference Point [Bohr]             -0.14684724     -0.41840046      0.11579183
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.69644184 Y=   -2.74860400 Z=   26.63040133     Total=    37.10849259
  Reference Point [Bohr]             -0.14651067     -0.24918453      0.28552096
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.10496400 Y=   23.58016995 Z=  -24.85538858     Total=    34.50602101
  Reference Point [Bohr]             -0.14618607     -0.24898479      0.28616649
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.42003123 Y=   -5.29776352 Z=    7.33518473     Total=    22.33492576
  Reference Point [Bohr]             -0.14584730     -0.24875616      0.28682057
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.81082412 Y=   -6.45044080 Z=   12.25465740     Total=    16.41387938
  Reference Point [Bohr]             -0.14547582     -0.24853898      0.28749902
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.92484105 Y=   21.09491215 Z=   15.80496008     Total=    32.44906302
  Reference Point [Bohr]             -0.14507700     -0.24833806      0.28820206
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.62382760 Y=   -3.37430613 Z=  -11.34232791     Total=    23.77764936
  Reference Point [Bohr]              0.02440354     -0.24814478      0.28891930
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.28437558 Y=    1.03656424 Z=  -12.52638485     Total=    26.46028967
  Reference Point [Bohr]              0.02480957     -0.24795916      0.28964281
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.21451888 Y=    1.10861701 Z=   -9.77396684     Total=    28.93768300
  Reference Point [Bohr]              0.02522474     -0.24777038      0.29035451
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.12184777 Y=   -2.44459451 Z=   19.99112687     Total=    20.78110970
  Reference Point [Bohr]              0.02565292     -0.24756641      0.29102535
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.64068674 Y=   -8.69988494 Z=  -11.87623620     Total=    18.16472401
  Reference Point [Bohr]              0.02608199     -0.24735262      0.12257318
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.65618675 Y=  -10.32235079 Z=   10.19865510     Total=    20.62443458
  Reference Point [Bohr]              0.02650270     -0.24715012      0.12315029
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.71169104 Y=   -7.68197168 Z=    7.63714081     Total=    15.95312871
  Reference Point [Bohr]              0.02691631     -0.24697818      0.12370292
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.52825865 Y=   -6.63932660 Z=    9.19759966     Total=    16.90070301
  Reference Point [Bohr]              0.02733183     -0.41590211      0.12425872
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.14784083 Y=   -7.51380358 Z=   13.43073652     Total=    21.59395771
  Reference Point [Bohr]              0.02777044     -0.41575683      0.12481915
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.23052778 Y=   18.28979830 Z=   -9.06712403     Total=    30.92550535
  Reference Point [Bohr]              0.02826198     -0.41561385      0.12536135
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.05949107 Y=   16.62698577 Z=   -5.80865008     Total=    18.07419540
  Reference Point [Bohr]              0.02882239     -0.41547551      0.12586235
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.07663123 Y=  -11.75863176 Z=   20.91225260     Total=    30.65135541
  Reference Point [Bohr]              0.02943982     -0.41534153      0.12631696
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.65230681 Y=   15.32052144 Z=   16.58598160     Total=    33.42976809
  Reference Point [Bohr]              0.03008977     -0.41521168      0.29581150
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.12135430 Y=  -15.08652292 Z=  -13.46859132     Total=    33.03530349
  Reference Point [Bohr]              0.19983400     -0.41508688      0.29621902
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.92010526 Y=  -21.94164961 Z=   21.37332903     Total=    31.90334558
  Reference Point [Bohr]              0.20052777     -0.24589864      0.29662231
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.86864594 Y=    1.10404431 Z=   -2.33900148     Total=    10.20196130
  Reference Point [Bohr]              0.03217376     -0.24578960      0.29701353
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.08916748 Y=   23.23379456 Z=   -1.06349827     Total=    23.80839902
  Reference Point [Bohr]              0.03291715     -0.24568207      0.12830357
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.59917916 Y=  -23.68049125 Z=  -25.54651714     Total=    37.76938226
  Reference Point [Bohr]              0.03366907     -0.07652512      0.12864005
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.84130508 Y=    2.24303803 Z=   10.15323735     Total=    20.65022070
  Reference Point [Bohr]              0.03440697     -0.07648333      0.12897573
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.93289628 Y=  -25.76428434 Z=  -23.16418719     Total=    35.77952699
  Reference Point [Bohr]              0.03512738     -0.07646065      0.12932864
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.04748753 Y=   24.59548557 Z=  -22.13093915     Total=    36.77279203
  Reference Point [Bohr]              0.03583957     -0.07642358     -0.03937948
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.54486190 Y=   19.65795219 Z=    4.95887112     Total=    24.95152290
  Reference Point [Bohr]              0.03655360     -0.07636517     -0.03899913
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -18.58204580 Y=   16.24839232 Z=  -25.63373302     Total=    35.58638711
  Reference Point [Bohr]              0.03727507     -0.07629991      0.13047590
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.17199468 Y=  -12.21256887 Z=   -1.67074036     Total=    28.92942304
  Reference Point [Bohr]              0.03800432     -0.07623658      0.13090351
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.07361261 Y=  -11.79555737 Z=   -7.40709215     Total=    17.18946942
  Reference Point [Bohr]              0.03875154     -0.24524564      0.13136643
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.49364469 Y=   16.51146122 Z=  -10.40363789     Total=    22.64879469
  Reference Point [Bohr]             -0.12955266     -0.24517507      0.13185972
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.84574985 Y=   -8.41219054 Z=   -8.54789632     Total=    21.50121552
  Reference Point [Bohr]             -0.12878315     -0.24508877      0.13236551
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.88259719 Y=   -4.32330602 Z=   20.74148043     Total=    27.72520997
  Reference Point [Bohr]             -0.12803340     -0.24499884      0.13287560
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.66516679 Y=    0.84008465 Z=   25.33713989     Total=    30.89877858
  Reference Point [Bohr]             -0.12730022     -0.24492948      0.13339684
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.34376424 Y=    5.33052593 Z=  -14.79417204     Total=    24.92916461
  Reference Point [Bohr]             -0.12657240     -0.24488047      0.13394548
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.93876757 Y=    6.89026419 Z=  -10.96771839     Total=    27.21821412
  Reference Point [Bohr]             -0.12584029     -0.24482610      0.13453360
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.15665709 Y=  -22.18531784 Z=   16.14375021     Total=    28.62411664
  Reference Point [Bohr]             -0.12509760     -0.24473960      0.13515691
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.87647774 Y=    2.05415394 Z=  -13.01279080     Total=    16.46502613
  Reference Point [Bohr]             -0.12434809     -0.24462481      0.13580459
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.36507575 Y=   24.12148234 Z=   12.68274597     Total=    30.80670961
  Reference Point [Bohr]             -0.12360085     -0.07542664      0.13647752
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.45044343 Y=   15.84784561 Z=  -15.66228351     Total=    30.24370963
  Reference Point [Bohr]             -0.12284973     -0.07529237      0.13717991
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.69839149 Y=    7.46230661 Z=   14.43919072     Total=    16.26849715
  Reference Point [Bohr]             -0.12208155     -0.07512885     -0.03116744
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.20530564 Y=   22.41203791 Z=    0.62615776     Total=    32.26728570
  Reference Point [Bohr]             -0.12130140     -0.07492609     -0.03042785
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.14191236 Y=   11.14334024 Z=    8.86239841     Total=    30.64962551
  Reference Point [Bohr]             -0.12051960     -0.07468779     -0.02969347
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.61655731 Y=  -15.01507014 Z=    6.93542120     Total=    17.46705798
  Reference Point [Bohr]             -0.11973638     -0.07441756     -0.02899288
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.69524053 Y=  -11.27612213 Z=    1.95793849     Total=    19.42485595
  Reference Point [Bohr]             -0.11894254     -0.07411840     -0.02834380
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.73446106 Y=   21.40943551 Z=   24.21627653     Total=    34.74130793
  Reference Point [Bohr]             -0.11812671     -0.07380175     -0.02774645
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.41230955 Y=   -3.03613465 Z=   -6.70618025     Total=    11.94916475
  Reference Point [Bohr]             -0.11729084     -0.07348957     -0.02719276
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.74418391 Y=   17.86893841 Z=   19.77811021     Total=    35.69676278
  Reference Point [Bohr]             -0.11645112     -0.07320204      0.14240550
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.94281457 Y=   -1.70781908 Z=    3.98588223     Total=     5.86086085
  Reference Point [Bohr]             -0.11561107     -0.24202243     -0.02617036
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.64626556 Y=  -24.47728143 Z=   18.91778470     Total=    38.93797323
  Reference Point [Bohr]             -0.11476580     -0.24179662     -0.02571747
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.67093102 Y=    4.68703074 Z=  -19.64947609     Total=    23.84581013
  Reference Point [Bohr]             -0.11392111     -0.24158575     -0.02530969
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.60439024 Y=    3.82035701 Z=  -20.48519764     Total=    22.94521218
  Reference Point [Bohr]             -0.28215368     -0.24139173     -0.02492029
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.25318175 Y=   -0.28411760 Z=   23.62021635     Total=    25.02219719
  Reference Point [Bohr]             -0.28130791     -0.24121997     -0.02452017
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.98536673 Y=   -4.84412702 Z=   18.98507105     Total=    33.34829091
  Reference Point [Bohr]             -0.28044378     -0.24106537     -0.02409899
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.03757809 Y=   20.47675589 Z=   13.60208859     Total=    35.08838358
  Reference Point [Bohr]             -0.27954879     -0.24092986     -0.02367171
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.06050061 Y=   20.93717498 Z=   -7.16642732     Total=    22.70091723
  Reference Point [Bohr]             -0.27861558     -0.24082501     -0.02325562
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.09139165 Y=   17.59112176 Z=   26.64937090     Total=    32.19279453
  Reference Point [Bohr]             -0.27765027     -0.24075647     -0.02284457
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.40379098 Y=   18.46074748 Z=   18.51278967     Total=    29.37999645
  Reference Point [Bohr]              0.06147108     -0.24071686     -0.02241192
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.56814395 Y=   -8.57331323 Z=  -15.78884083     Total=    28.84632240
  Reference Point [Bohr]              0.06242813     -0.24067328     -0.02193386
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.04116161 Y=   14.55387944 Z=   10.27838813     Total=    19.54791420
  Reference Point [Bohr]              0.06335313     -0.24058920      0.14766448
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.93080504 Y=  -16.71257912 Z=    8.58893361     Total=    22.25812639
  Reference Point [Bohr]              0.06425336     -0.07138854      0.14821821
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.84879712 Y=    3.55868414 Z=   10.27950036     Total=    16.08497292
  Reference Point [Bohr]              0.06515568     -0.07123573      0.14877888
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.38777502 Y=   -3.61976019 Z=  -14.87228437     Total=    17.95599694
  Reference Point [Bohr]              0.06607252     -0.24013657      0.14933077
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.69620959 Y=   -9.01097637 Z=   16.98078022     Total=    19.29823098
  Reference Point [Bohr]              0.06699674     -0.23993829      0.14987156
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.18162089 Y=   17.04588706 Z=   21.39070838     Total=    30.36247355
  Reference Point [Bohr]              0.06793263     -0.40878232      0.15041257
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.31838480 Y=   -5.83988124 Z=   -4.39515160     Total=     8.48940621
  Reference Point [Bohr]              0.06889128     -0.40852882      0.15097292
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -27.49760503 Y=   25.14820402 Z=  -16.94836861     Total=    40.93650750
  Reference Point [Bohr]              0.06987460     -0.40828061     -0.01750436
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.36962642 Y=    1.99278691 Z=  -21.67779941     Total=    22.02844908
  Reference Point [Bohr]             -0.09819855     -0.40807328     -0.01687331
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.42156304 Y=   27.16190999 Z=  -25.11265061     Total=    37.54531990
  Reference Point [Bohr]             -0.09721104     -0.23884988     -0.18530145
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.09023266 Y=  -22.14068751 Z=   -6.20144064     Total=    29.88486059
  Reference Point [Bohr]             -0.09625646     -0.23874747     -0.18466462
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   19.55500468 Y=   12.76044569 Z=   10.60596224     Total=    25.64592789
  Reference Point [Bohr]             -0.09530850     -0.23866281     -0.18404561
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.20504926 Y=    9.86552580 Z=    7.14747389     Total=    21.90522315
  Reference Point [Bohr]             -0.09433159     -0.23856932     -0.18344194
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.14902406 Y=    5.48755402 Z=    4.03714705     Total=     9.87523926
  Reference Point [Bohr]             -0.09330987     -0.23845466     -0.18285181
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.99127881 Y=  -22.16212635 Z=   -0.43110134     Total=    29.18928508
  Reference Point [Bohr]             -0.09224695     -0.23831880     -0.01320146
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.33154896 Y=    5.75024251 Z=   -6.16722609     Total=    14.12458737
  Reference Point [Bohr]             -0.09115688     -0.23817927     -0.01262864
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.56756270 Y=  -20.96702255 Z=  -11.98333077     Total=    26.77731796
  Reference Point [Bohr]              0.07902395     -0.40713102     -0.01204524
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.68991934 Y=    8.01835303 Z=  -15.81198701     Total=    18.10879408
  Reference Point [Bohr]              0.08012342     -0.40703037     -0.18051823
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.19537206 Y=    9.88241091 Z=  -17.96003703     Total=    20.50032062
  Reference Point [Bohr]              0.08117808     -0.57600765     -0.17990157
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.03260541 Y=  -16.71183534 Z=  -19.48900308     Total=    25.67309378
  Reference Point [Bohr]              0.08219137     -0.57588799     -0.17926797
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.83386050 Y=  -15.37833647 Z=    6.92285406     Total=    28.38669276
  Reference Point [Bohr]              0.08319812     -0.57572933      0.15952295
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.11707997 Y=    3.26007319 Z=    5.79049017     Total=    15.60287795
  Reference Point [Bohr]              0.08421485     -0.57553544      0.16016183
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.57271211 Y=    8.69444110 Z=  -22.96620491     Total=    28.05812517
  Reference Point [Bohr]              0.08525539     -0.57530694      0.16078664
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.95137842 Y=  -11.61194942 Z=  -23.27126368     Total=    26.08058589
  Reference Point [Bohr]             -0.08273592     -0.57504429      0.16139632
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.63632594 Y=  -27.15487045 Z=    7.70159332     Total=    29.24063957
  Reference Point [Bohr]              0.08747269     -0.57475632      0.16199294
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.94076404 Y=  -24.47768038 Z=  -13.47145409     Total=    34.91636451
  Reference Point [Bohr]              0.08866397     -0.57444638      0.16258430
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.90927405 Y=    3.66645829 Z=   -9.95910167     Total=    10.78294718
  Reference Point [Bohr]              0.08989011     -0.40504530      0.16317649
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   27.43534413 Y=  -25.14050496 Z=   21.71766033     Total=    43.08595905
  Reference Point [Bohr]              0.09112363     -0.40471413      0.16376365
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -24.78045339 Y=   25.44725349 Z=   -0.01254705     Total=    35.51948392
  Reference Point [Bohr]             -0.07672196     -0.06624133      0.16433320
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.32595826 Y=   21.00476212 Z=    2.75783854     Total=    26.74588975
  Reference Point [Bohr]             -0.07551110     -0.06592105     -0.00419668
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.37413378 Y=   17.99829262 Z=  -25.01132856     Total=    38.08026991
  Reference Point [Bohr]             -0.07432072     -0.06560027      0.16540578
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.89267217 Y=    1.15873167 Z=    0.64217287     Total=     2.31024955
  Reference Point [Bohr]             -0.07314822     -0.06527293      0.16593900
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.14312994 Y=   -1.46435287 Z=   24.61517382     Total=    26.29920031
  Reference Point [Bohr]             -0.07197814     -0.06494015      0.16648911
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.51141044 Y=   -1.63339213 Z=  -13.75385381     Total=    25.58470722
  Reference Point [Bohr]             -0.07079919     -0.06460730     -0.00201866
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.85454826 Y=   -3.03361883 Z=    3.39844623     Total=     8.23025588
  Reference Point [Bohr]             -0.06961598     -0.06428477     -0.00144969
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.74528945 Y=   19.69708400 Z=   -0.53782829     Total=    30.09339744
  Reference Point [Bohr]             -0.06843294     -0.06398283     -0.00087936
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    1.03674670 Y=   12.77961058 Z=   24.98912725     Total=    28.08646953
  Reference Point [Bohr]              0.10184239     -0.06370574     -0.00030150
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.61776092 Y=  -23.70893923 Z=   25.38228117     Total=    35.78602800
  Reference Point [Bohr]              0.10308576     -0.06345389      0.00026958
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.81320566 Y=   -7.74149279 Z=  -20.01966557     Total=    25.52493625
  Reference Point [Bohr]              0.10436458     -0.06323115      0.00081360
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.39539189 Y=  -10.15865130 Z=    5.31604035     Total=    20.00668279
  Reference Point [Bohr]              0.10565187     -0.06304454      0.00133770
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.29707046 Y=   -8.41488102 Z=    8.29307069     Total=    21.77999154
  Reference Point [Bohr]              0.10692102     -0.06288779      0.00186025
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.91147863 Y=   22.32883359 Z=    2.92253590     Total=    30.73122133
  Reference Point [Bohr]              0.10816084     -0.06274991      0.00238970
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.02432140 Y=   -3.50141507 Z=  -10.11087183     Total=    25.38915147
  Reference Point [Bohr]              0.10937095     -0.06262732      0.00291508
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.85289758 Y=   -3.50169776 Z=   17.53475507     Total=    18.29137345
  Reference Point [Bohr]              0.11054870     -0.06251835      0.00341520
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.04421239 Y=   -4.93491922 Z=   -3.93502572     Total=    23.89296088
  Reference Point [Bohr]              0.11170647     -0.06242238      0.17295894
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.97023853 Y=   21.01715398 Z=    5.53726908     Total=    22.53942897
  Reference Point [Bohr]              0.11286305     -0.06233495      0.17340594
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.00793037 Y=   21.42487000 Z=  -11.64211675     Total=    25.66497391
  Reference Point [Bohr]             -0.05504283     -0.06225092      0.17383007
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.25576868 Y=   -7.16760802 Z=   24.02275636     Total=    30.43401026
  Reference Point [Bohr]             -0.05384819     -0.06217013      0.17423349
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.34111324 Y=   17.18867037 Z=  -25.64255409     Total=    36.42896692
  Reference Point [Bohr]             -0.05261577     -0.06210445      0.00555016
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.91917421 Y=   14.53691212 Z=  -21.86918936     Total=    26.27599929
  Reference Point [Bohr]             -0.05135617     -0.06207531     -0.16313853
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.58611798 Y=  -14.59675368 Z=    9.62112527     Total=    17.55411746
  Reference Point [Bohr]             -0.05008859     -0.06207702     -0.16276115
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.22574879 Y=  -15.75448247 Z=  -13.74090691     Total=    21.32775641
  Reference Point [Bohr]             -0.04881652     -0.23115198     -0.16241001
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.33817538 Y=  -16.51830348 Z=   15.66972171     Total=    23.92160835
  Reference Point [Bohr]             -0.04754438     -0.23114999     -0.16210034
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.65697553 Y=  -16.67294337 Z=   15.50034688     Total=    24.72862653
  Reference Point [Bohr]             -0.04629067     -0.23117943      0.00725558
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.03998374 Y=   11.29086576 Z=   13.99694944     Total=    24.09728868
  Reference Point [Bohr]             -0.04505551     -0.23128192      0.00754502
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.02661217 Y=   11.46054285 Z=  -19.29881112     Total=    26.46760288
  Reference Point [Bohr]             -0.21290228     -0.23147467      0.00785833
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.19440601 Y=    8.38095107 Z=   13.68555277     Total=    20.15535248
  Reference Point [Bohr]             -0.21169633     -0.23174671      0.00818156
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.13961698 Y=    9.31254385 Z=  -18.85425074     Total=    23.34562221
  Reference Point [Bohr]             -0.21053131     -0.23207192      0.00849333
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.08503972 Y=  -16.03900270 Z=  -20.08888541     Total=    26.66478413
  Reference Point [Bohr]             -0.20940545     -0.23242624      0.17786088
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.76867509 Y=  -16.48078837 Z=    6.71126224     Total=    29.69187333
  Reference Point [Bohr]             -0.20830451     -0.23280351      0.17814378
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.59759999 Y=    3.09936102 Z=  -24.94301920     Total=    25.18556275
  Reference Point [Bohr]             -0.20722087     -0.23321680      0.17842534
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.98898669 Y=   23.91982295 Z=  -26.48520343     Total=    44.14806179
  Reference Point [Bohr]             -0.20615430     -0.23367802      0.17871041
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.05276827 Y=   19.58645698 Z=   -1.14290577     Total=    19.85585366
  Reference Point [Bohr]             -0.20510314     -0.23417876      0.17899290
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.42878458 Y=   17.77146473 Z=   22.89144963     Total=    29.18218615
  Reference Point [Bohr]             -0.20406528     -0.06562777      0.17926029
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.19482732 Y=   16.46949742 Z=   10.94127779     Total=    19.77356474
  Reference Point [Bohr]             -0.20304393     -0.06615721      0.17949544
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.22102437 Y=   14.66579889 Z=  -25.89896466     Total=    35.98238255
  Reference Point [Bohr]             -0.20203728     -0.06667963      0.17968581
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.58473993 Y=   11.75382982 Z=   26.62009809     Total=    32.11428494
  Reference Point [Bohr]             -0.20103937     -0.06718550      0.17984500
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.67133136 Y=    9.23134438 Z=   -2.12737925     Total=    12.18986409
  Reference Point [Bohr]             -0.20004956     -0.06767847      0.17999580
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.80878337 Y=  -21.31031397 Z=   -1.56779661     Total=    21.38320833
  Reference Point [Bohr]             -0.19907213     -0.06816570      0.18014780
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.19520841 Y=   25.00919262 Z=    0.41129829     Total=    30.35299119
  Reference Point [Bohr]             -0.19811575     -0.06864263      0.18029415
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.04730109 Y=   20.79478560 Z=   11.05933321     Total=    28.49996196
  Reference Point [Bohr]             -0.19717997     -0.06910660      0.18041949
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.47924779 Y=   -7.65674431 Z=   18.57361252     Total=    22.21398105
  Reference Point [Bohr]             -0.19624552     -0.06955533      0.18052907
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.50899903 Y=   22.53743871 Z=  -10.71806478     Total=    29.92256850
  Reference Point [Bohr]             -0.19529993     -0.06998267      0.18065469
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.30695822 Y=  -23.97086025 Z=  -13.44696979     Total=    29.35398654
  Reference Point [Bohr]             -0.19435788     -0.07038309      0.18081289
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.16058302 Y=  -12.90721451 Z=  -12.36255703     Total=    18.60270464
  Reference Point [Bohr]             -0.19343676     -0.07075782      0.18098820
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.33959418 Y=   -5.03207058 Z=   16.40364415     Total=    17.31689858
  Reference Point [Bohr]             -0.19252461     -0.24018850      0.18116188
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.33987519 Y=    2.23408412 Z=  -10.76030653     Total=    28.54057382
  Reference Point [Bohr]             -0.02253446     -0.24052945      0.18132839
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.18755984 Y=  -17.45119075 Z=   16.14248383     Total=    33.20823353
  Reference Point [Bohr]             -0.02161074     -0.24084403      0.18149283
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.90824891 Y=  -12.24858204 Z=   13.83714660     Total=    29.43267328
  Reference Point [Bohr]             -0.02066470     -0.24112900      0.18166787
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.08408911 Y=  -11.96759285 Z=  -16.77957319     Total=    22.13887648
  Reference Point [Bohr]             -0.01969104     -0.24140125      0.18186721
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.10453359 Y=   14.47116312 Z=  -18.05372581     Total=    28.19055835
  Reference Point [Bohr]             -0.01870006     -0.24168289      0.18209457
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.75829802 Y=   12.38838334 Z=  -19.39838297     Total=    29.07105867
  Reference Point [Bohr]             -0.01769934     -0.07290897      0.18233260
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.68069412 Y=    8.93607968 Z=    7.64775498     Total=    23.79144354
  Reference Point [Bohr]             -0.01668751     -0.07320995      0.18256170
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    2.95347662 Y=    5.74457205 Z=  -19.38123676     Total=    20.42927974
  Reference Point [Bohr]             -0.01565378     -0.07348450      0.18278339
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.53874564 Y=  -24.25769601 Z=   10.31276736     Total=    36.01303963
  Reference Point [Bohr]             -0.01458995     -0.07372831      0.18302067
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.70336122 Y=  -26.83954249 Z=   13.37272317     Total=    38.22355424
  Reference Point [Bohr]             -0.01349302     -0.07395769      0.18328581
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.48255017 Y=   -2.77505735 Z=   11.62148520     Total=    11.95795619
  Reference Point [Bohr]             -0.01236341     -0.07417397      0.18356314
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.41788840 Y=   -7.24758648 Z=  -21.84950322     Total=    23.27252161
  Reference Point [Bohr]             -0.01121150     -0.07435940      0.18383164
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.98297724 Y=   15.72948083 Z=   -1.81974802     Total=    16.92702179
  Reference Point [Bohr]             -0.01004149     -0.07450050      0.01501291
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.79652109 Y=  -15.69192288 Z=   -6.65246484     Total=    26.88841799
  Reference Point [Bohr]             -0.00885539     -0.07459856      0.01525967
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.41568697 Y=  -19.27517593 Z=   18.33069859     Total=    33.53128677
  Reference Point [Bohr]             -0.00767050     -0.07467529      0.01550425
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.34541523 Y=  -22.66659736 Z=  -10.42240351     Total=    26.30678784
  Reference Point [Bohr]             -0.00649767     -0.07475837      0.01575462
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.09576895 Y=    1.90590571 Z=   -9.67882747     Total=    19.73771754
  Reference Point [Bohr]             -0.00532698     -0.07486452      0.01601990
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.56537999 Y=   27.17736737 Z=   -5.18101761     Total=    30.38652686
  Reference Point [Bohr]             -0.00414804     -0.07500437      0.01630402
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.86974099 Y=  -27.26979634 Z=   26.62346069     Total=    40.55638256
  Reference Point [Bohr]             -0.00296554     -0.07518057      0.01660552
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.79686403 Y=   10.32585425 Z=   -0.72181295     Total=    17.24812271
  Reference Point [Bohr]             -0.00179238     -0.07538737      0.01693451
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.42449409 Y=  -16.35452034 Z=   25.23714512     Total=    32.53846774
  Reference Point [Bohr]             -0.16972043     -0.24468742      0.01730345
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.68729552 Y=  -17.79473367 Z=   23.92147231     Total=    32.40149458
  Reference Point [Bohr]             -0.16861972     -0.24491162      0.01770245
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.16183247 Y=  -18.63031894 Z=   -4.49547041     Total=    28.55032735
  Reference Point [Bohr]             -0.16754405     -0.24511169     -0.15096416
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.51910846 Y=    7.89585531 Z=   21.91367363     Total=    33.10139100
  Reference Point [Bohr]             -0.16645758     -0.24528895      0.01850223
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.54262829 Y=  -21.29949255 Z=   -6.34158537     Total=    22.68302360
  Reference Point [Bohr]             -0.16535571     -0.24545051      0.01887126
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.97128384 Y=  -23.82348358 Z=   -5.23606620     Total=    32.82852529
  Reference Point [Bohr]             -0.16426213     -0.07652050      0.01922511
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.03479858 Y=    0.33401637 Z=   -2.44123550     Total=    21.17862009
  Reference Point [Bohr]             -0.16318827     -0.07666101      0.01957606
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.10102700 Y=   -3.11227089 Z=  -26.81550039     Total=    27.91382947
  Reference Point [Bohr]             -0.16211606     -0.07682259      0.01992004
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.05390127 Y=   22.21347322 Z=  -24.53016983     Total=    38.69530437
  Reference Point [Bohr]             -0.16102051     -0.24607707      0.02023971
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.63661007 Y=   22.44588418 Z=    4.29554163     Total=    24.09537732
  Reference Point [Bohr]              0.00918676     -0.24625936      0.02052241
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.98493044 Y=   25.38073160 Z=  -22.40723722     Total=    34.56956854
  Reference Point [Bohr]              0.01036483     -0.24642267      0.02077910
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -19.58137078 Y=  -25.32001202 Z=  -22.31870781     Total=    39.02124817
  Reference Point [Bohr]              0.01158139     -0.24654891      0.02104356
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   11.22075854 Y=    6.34620379 Z=    4.65206640     Total=    13.70479648
  Reference Point [Bohr]              0.01282057     -0.24664201      0.02134763
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.17313391 Y=  -17.47258247 Z=   -2.60017666     Total=    19.90473417
  Reference Point [Bohr]              0.01406587     -0.24672419      0.02169879
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.22134327 Y=  -13.23917306 Z=   -5.95879719     Total=    15.79519166
  Reference Point [Bohr]              0.01530451     -0.24681130      0.02208099
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.20544003 Y=   20.17818841 Z=  -12.27238762     Total=    34.54106241
  Reference Point [Bohr]              0.01652723     -0.24690527      0.02247254
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.83714112 Y=   -5.38414078 Z=    8.06887187     Total=    10.10668268
  Reference Point [Bohr]              0.01772521     -0.24700141      0.02285234
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.49774722 Y=   21.73663722 Z=  -25.40301622     Total=    34.05899807
  Reference Point [Bohr]              0.01889164     -0.24709560      0.02320129
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.05735041 Y=   22.63079541 Z=   -1.93772065     Total=    23.78474000
  Reference Point [Bohr]             -0.14904627     -0.24718136      0.02352194
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.31544288 Y=   24.05638192 Z=   -5.00621517     Total=    25.14012002
  Reference Point [Bohr]             -0.14793095     -0.07817645      0.02383209
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.97615452 Y=   25.38253700 Z=   18.39872738     Total=    40.71298266
  Reference Point [Bohr]             -0.14684457     -0.07822054      0.02412836
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.11584547 Y=   -1.06903132 Z=   11.39622219     Total=    28.51410340
  Reference Point [Bohr]             -0.14581081     -0.24730899      0.02440507
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.54103619 Y=   -2.17608055 Z=  -24.72116215     Total=    32.86164063
  Reference Point [Bohr]             -0.14482339     -0.24729534      0.19375168
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.39236817 Y=   17.01147357 Z=   -1.81926088     Total=    17.66331909
  Reference Point [Bohr]             -0.14383978     -0.24725617      0.19403982
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.89016870 Y=   10.41563396 Z=   -0.87366644     Total=    26.07659648
  Reference Point [Bohr]             -0.14280959     -0.24719566     -0.14379054
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.17870834 Y=    5.70324903 Z=  -24.31180991     Total=    26.60525958
  Reference Point [Bohr]             -0.14171440     -0.24712164     -0.14343188
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -15.67312280 Y=  -24.91913062 Z=    3.15686556     Total=    29.60702027
  Reference Point [Bohr]             -0.14058725     -0.24704900     -0.14302600
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.79457359 Y=   -2.17098586 Z=   20.36614238     Total=    24.14941093
  Reference Point [Bohr]             -0.13947036     -0.24699079     -0.14258371
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -14.50546262 Y=  -12.07003448 Z=    8.58989075     Total=    20.73355737
  Reference Point [Bohr]             -0.13838352     -0.24694308     -0.14211699
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.60480323 Y=  -17.36068030 Z=   26.36597320     Total=    33.30194611
  Reference Point [Bohr]             -0.13732260     -0.24689629     -0.14163137
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.19646309 Y=   22.39294428 Z=   19.27660188     Total=    31.96537260
  Reference Point [Bohr]             -0.13626557     -0.07778572     -0.14114297
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.91262033 Y=   11.80066663 Z=   15.81902178     Total=    24.73627757
  Reference Point [Bohr]             -0.13519158     -0.07777141     -0.14066759
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.01325385 Y=    8.18172006 Z=    9.99215341     Total=    18.33380617
  Reference Point [Bohr]             -0.13409006     -0.07776984     -0.14019883
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.12590371 Y=    5.35829252 Z=  -25.05473707     Total=    30.81797732
  Reference Point [Bohr]             -0.13295984     -0.24682887     -0.13972208
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    3.27994554 Y=    4.22664546 Z=   23.13033796     Total=    23.74100059
  Reference Point [Bohr]             -0.13181687     -0.24678175     -0.13924004
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   14.29099190 Y=   12.35210916 Z=   16.80541544     Total=    25.28297922
  Reference Point [Bohr]             -0.13067972     -0.24670300     -0.13876647
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.29959740 Y=   22.05644505 Z=  -20.25007697     Total=    32.76326719
  Reference Point [Bohr]             -0.12954847     -0.24660776     -0.13830666
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.83606702 Y=   -3.12392683 Z=   16.87096426     Total=    27.77052712
  Reference Point [Bohr]             -0.12841586     -0.24651735     -0.13785896
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -26.26048313 Y=    3.43692881 Z=  -17.49841365     Total=    31.74302969
  Reference Point [Bohr]             -0.12729588     -0.24645179     -0.13741410
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.07999993 Y=   10.51850847 Z=  -18.74142978     Total=    30.81244242
  Reference Point [Bohr]             -0.12620163     -0.24641033     -0.13695135
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.95844003 Y=   14.57131891 Z=  -16.97459618     Total=    24.09800610
  Reference Point [Bohr]             -0.12511688     -0.24637706     -0.13645603
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.69832198 Y=   16.26514279 Z=   15.09270589     Total=    27.77010260
  Reference Point [Bohr]             -0.12402606     -0.24634609     -0.13592996
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -16.76888031 Y=   16.76575666 Z=   21.88185343     Total=    32.26610377
  Reference Point [Bohr]             -0.12293933     -0.41539717     -0.13538171
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.12597428 Y=   17.32051432 Z=    1.58950575     Total=    19.19786975
  Reference Point [Bohr]             -0.12187348     -0.41538985      0.03425261
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.72351875 Y=   18.92677296 Z=  -20.10231230     Total=    37.73625725
  Reference Point [Bohr]             -0.12082420     -0.41540154      0.03481998
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   16.32714239 Y=   21.77025261 Z=  -15.97267841     Total=    31.55385765
  Reference Point [Bohr]             -0.11977435     -0.24636508      0.03539777
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.20552583 Y=   24.26037257 Z=  -13.02823517     Total=    31.45645569
  Reference Point [Bohr]             -0.11871942     -0.24642923      0.03599105
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.72121092 Y=   24.93134177 Z=   16.90705965     Total=    39.61061927
  Reference Point [Bohr]             -0.11766846     -0.24651505      0.20567836
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.03745545 Y=   -2.57639825 Z=   19.61853196     Total=    23.16084969
  Reference Point [Bohr]             -0.11663240     -0.24660749      0.20632307
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.31107855 Y=   26.08118530 Z=   23.13907018     Total=    36.65494910
  Reference Point [Bohr]             -0.11561990     -0.24667885      0.20699529
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.04341930 Y=    0.34199656 Z=   -0.66718513     Total=     8.07828519
  Reference Point [Bohr]             -0.11463381     -0.24672491      0.20767072
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.47233735 Y=    1.82302621 Z=  -25.19602689     Total=    33.81078440
  Reference Point [Bohr]             -0.11366379     -0.24676278      0.03925111
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.18824385 Y=    2.99871820 Z=  -23.18109270     Total=    34.36281417
  Reference Point [Bohr]             -0.11269002     -0.24679902      0.03987402
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.09132301 Y=    3.73701373 Z=  -22.10352452     Total=    30.77945702
  Reference Point [Bohr]              0.05736917     -0.24682983      0.04047407
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.62366971 Y=  -24.42035813 Z=   26.33716261     Total=    38.41359658
  Reference Point [Bohr]              0.05835728     -0.24684852      0.04106942
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.02650229 Y=  -27.14031315 Z=   25.39756052     Total=    40.88440361
  Reference Point [Bohr]              0.05934230     -0.24685797      0.04167462
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.51046177 Y=   23.79999339 Z=    0.43465733     Total=    32.76201308
  Reference Point [Bohr]              0.06033180     -0.07780015      0.04229530
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.47976708 Y=   21.95612749 Z=  -24.37347290     Total=    41.53740780
  Reference Point [Bohr]              0.06133538     -0.07782816      0.04293340
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   10.87690380 Y=   18.48613774 Z=   25.77569204     Total=    33.53253085
  Reference Point [Bohr]              0.06236430     -0.07786066      0.04358133
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.46341929 Y=   14.10451772 Z=    6.48323557     Total=    24.12193225
  Reference Point [Bohr]              0.06342884     -0.07788329      0.04421877
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.91306773 Y=   10.89815640 Z=   -3.62817189     Total=    23.85979560
  Reference Point [Bohr]              0.06452651     -0.07787971      0.04482627
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -7.18909644 Y=    9.93498241 Z=   26.01760199     Total=    28.76286836
  Reference Point [Bohr]              0.06564717     -0.07784994      0.04540057
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -6.72492750 Y=  -15.70358465 Z=   25.30436306     Total=    30.53093530
  Reference Point [Bohr]              0.06677969     -0.07779380      0.04595324
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -5.23025434 Y=   15.52502961 Z=   24.54810167     Total=    29.51256343
  Reference Point [Bohr]              0.06791328     -0.07771121      0.04649394
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -2.82590469 Y=   18.55183318 Z=   24.34476647     Total=    30.73798800
  Reference Point [Bohr]             -0.10004233     -0.07760926      0.04702461
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    0.30252120 Y=   -9.03098103 Z=   27.32701544     Total=    28.78221517
  Reference Point [Bohr]             -0.09895995     -0.07750129      0.04755019
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.79636199 Y=   15.51657413 Z=    6.88795716     Total=    29.23140214
  Reference Point [Bohr]             -0.09791281     -0.07739107      0.04808171
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.27550249 Y=   11.47251520 Z=    8.99564576     Total=    19.05854688
  Reference Point [Bohr]             -0.09687834     -0.07725241      0.04862863
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -12.71126317 Y=  -21.26090289 Z=    9.62401140     Total=    26.57487156
  Reference Point [Bohr]             -0.09583282     -0.07704549      0.04919687
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.92526018 Y=  -25.54634846 Z=   10.05183302     Total=    31.73750429
  Reference Point [Bohr]             -0.09476636     -0.07676613      0.04978879
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.32483171 Y=    0.07686378 Z=    9.97742904     Total=    13.65677432
  Reference Point [Bohr]             -0.09368923     -0.07645631      0.05039413
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.35414902 Y=   26.39159664 Z=    8.75430798     Total=    35.05929209
  Reference Point [Bohr]             -0.09261919     -0.07615580      0.05099649
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.23272079 Y=   24.10890138 Z=    5.94576229     Total=    24.86183452
  Reference Point [Bohr]             -0.09156526     -0.07587261      0.05159024
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.83371499 Y=   19.94609369 Z=    2.52640726     Total=    21.57768472
  Reference Point [Bohr]             -0.09052602     -0.07560668      0.05218067
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   18.62198966 Y=   15.64081956 Z=  -26.59568460     Total=    36.03809339
  Reference Point [Bohr]             -0.08949301     -0.07534852      0.05278069
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.75372109 Y=   12.48071254 Z=   14.91178133     Total=    19.80454063
  Reference Point [Bohr]             -0.08845576     -0.07507444      0.05340524
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -1.04474489 Y=  -18.95714473 Z=   17.74496539     Total=    25.98747053
  Reference Point [Bohr]             -0.08740228     -0.07478105      0.05405546
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   21.52922074 Y=    9.94519852 Z=    0.48873429     Total=    23.72031156
  Reference Point [Bohr]             -0.08633000     -0.07448222      0.22379024
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.86446683 Y=    6.01975858 Z=    4.73786387     Total=    22.22635425
  Reference Point [Bohr]              0.08383393     -0.07418573      0.22445963
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    5.75075502 Y=  -21.99489529 Z=  -26.41434131     Total=    34.85059582
  Reference Point [Bohr]              0.08495508     -0.07388980      0.05607139
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.03213829 Y=    6.79039202 Z=   23.49320836     Total=    33.59344664
  Reference Point [Bohr]              0.08610953     -0.07358928      0.05677131
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -23.44658833 Y=  -18.65157464 Z=   -7.42768169     Total=    30.86736458
  Reference Point [Bohr]              0.08729290     -0.07327551      0.05748075
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.42297357 Y=  -16.16260476 Z=   -9.00583941     Total=    29.07102819
  Reference Point [Bohr]             -0.08056955     -0.07294046      0.05819225
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    7.55265462 Y=  -13.66960647 Z=   16.82184849     Total=    22.95376483
  Reference Point [Bohr]             -0.07932414     -0.07259289      0.05889582
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   13.50204414 Y=  -12.02524095 Z=   20.41042564     Total=    27.26714306
  Reference Point [Bohr]             -0.07804919     -0.24132769      0.05958341
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   26.90324081 Y=  -11.33353729 Z=  -12.87759296     Total=    31.90714394
  Reference Point [Bohr]             -0.07676876     -0.24100048      0.06025528
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -10.41484567 Y=   17.21021079 Z=   10.62599723     Total=    22.75021281
  Reference Point [Bohr]             -0.07550423     -0.40974298      0.06092691
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -4.30766167 Y=   20.32021162 Z=    6.21907832     Total=    21.68280158
  Reference Point [Bohr]             -0.24333530     -0.40940773      0.06162300
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -3.60544456 Y=   -1.25738967 Z=  -19.26717772     Total=    19.64190409
  Reference Point [Bohr]             -0.24211427     -0.40907396      0.06236210
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.23666194 Y=    4.12616199 Z=   23.99007632     Total=    26.03583873
  Reference Point [Bohr]             -0.24090788     -0.40873162      0.06314789
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    9.56920058 Y=  -21.18801363 Z=   -0.99056520     Total=    23.26978171
  Reference Point [Bohr]             -0.23971231     -0.40836269      0.06396777
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -25.23123912 Y=  -22.52798074 Z=    6.35009362     Total=    34.41582533
  Reference Point [Bohr]             -0.23853001     -0.40795914      0.23386701
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   24.23116435 Y=   27.04930846 Z=   16.04641429     Total=    39.70266774
  Reference Point [Bohr]             -0.23734937     -0.40753025      0.23466950
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -8.11376707 Y=   -4.10332765 Z=   24.04806165     Total=    25.70952708
  Reference Point [Bohr]             -0.23615005     -0.40708498      0.06636547
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.36004244 Y=   -2.73824175 Z=  -26.41248657     Total=    30.67651086
  Reference Point [Bohr]             -0.23492511     -0.40662225      0.06710680
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.27677255 Y=   -0.04829830 Z=    1.49304716     Total=    12.36732254
  Reference Point [Bohr]             -0.23368706     -0.40614610      0.06783074
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -17.81928583 Y=   26.36352869 Z=   24.14421555     Total=    39.94378221
  Reference Point [Bohr]             -0.23245062     -0.40567030      0.06854948
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.29185663 Y=   -4.49651172 Z=  -11.92538894     Total=    24.81484793
  Reference Point [Bohr]             -0.23122084     -0.23613175      0.06926236
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.44946784 Y=   20.06088889 Z=  -16.41424491     Total=    28.75510300
  Reference Point [Bohr]             -0.23000020     -0.23568445      0.23903538
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.34543614 Y=   -7.32894065 Z=    9.30380770     Total=    14.48863393
  Reference Point [Bohr]             -0.22878959     -0.23525205      0.23972268
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    6.79921566 Y=   26.02275753 Z=    9.12104262     Total=    28.40082149
  Reference Point [Bohr]             -0.22758732     -0.23481821      0.24040121
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.75007281 Y=    6.67643228 Z=  -18.62622042     Total=    29.40368178
  Reference Point [Bohr]             -0.22638962     -0.23436799      0.07199766
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.53981629 Y=   10.66146334 Z=    8.35828243     Total=    25.44585176
  Reference Point [Bohr]             -0.22518685     -0.06481594      0.07265898
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    4.54283865 Y=   13.86771104 Z=  -19.12242612     Total=    24.05447928
  Reference Point [Bohr]             -0.22398075     -0.06430094     -0.09575543
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -21.81811784 Y=  -14.03479610 Z=    5.37409232     Total=    26.49314318
  Reference Point [Bohr]             -0.05372167     -0.06375761     -0.09508602
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=    8.74895406 Y=   12.94391710 Z=    4.00134177     Total=    16.12761368
  Reference Point [Bohr]             -0.05257309     -0.06320042     -0.09439376
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.05883255 Y=  -17.03456245 Z=    4.35472603     Total=    21.90143977
  Reference Point [Bohr]             -0.05145427     -0.06263587     -0.09367249
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   25.62093807 Y=  -20.42304976 Z=    6.69663574     Total=    33.44216440
  Reference Point [Bohr]             -0.05035489     -0.06206569     -0.09292875
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   17.76869386 Y=    8.09609070 Z=  -13.96697686     Total=    24.00728241
  Reference Point [Bohr]             -0.04927582     -0.06149192     -0.09217108
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -22.24710362 Y=   11.80403235 Z=   -7.72389191     Total=    26.34249998
  Reference Point [Bohr]             -0.04821854     -0.06092010     -0.09140380
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -13.75645670 Y=  -13.56017189 Z=   -5.75375475     Total=    20.15500078
  Reference Point [Bohr]             -0.04718089     -0.06036436     -0.09063893
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.38952941 Y=   15.29427402 Z=   24.20140761     Total=    35.14762948
  Reference Point [Bohr]             -0.04616884     -0.05984471     -0.08989266
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -0.37495260 Y=  -10.52327561 Z=  -26.61416817     Total=    28.62156296
  Reference Point [Bohr]             -0.04519233     -0.22843335     -0.08916684
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -20.79588464 Y=   -8.59926482 Z=  -26.68558876     Total=    34.90754676
  Reference Point [Bohr]             -0.04424195     -0.22795272      0.08062612
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   12.57873304 Y=   20.81419228 Z=    7.70125117     Total=    25.51008417
  Reference Point [Bohr]             -0.04329004     -0.22745542      0.08134714
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=  -11.47177432 Y=   -5.04292439 Z=  -13.72364102     Total=    18.58416033
  Reference Point [Bohr]             -0.04232749     -0.22695125      0.08205906
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   -9.14420495 Y=   23.71043858 Z=  -16.75989581     Total=    30.44167357
  Reference Point [Bohr]             -0.04137631     -0.22644863      0.08275505
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   20.53066364 Y=   -2.66593909 Z=    8.23944882     Total=    22.28236741
  Reference Point [Bohr]             -0.04045604     -0.22593538      0.08344885
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   22.37164245 Y=   -1.14082136 Z=  -21.14560984     Total=    30.80468592
  Reference Point [Bohr]             -0.03956395     -0.22540442     -0.08492736
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=    -0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   23.44754983 Y=    1.17811984 Z=  -22.21304597     Total=    32.32019447
  Reference Point [Bohr]             -0.03868767     -0.22485630     -0.08424108
  Charges
    Electronic=   1024.00000000    Core= -1024.00000000    Total=     0.00000000
  Dipole vectors are based on the periodic (Berry phase) operator.
  They are defined modulo integer multiples of the cell matrix [Debye].
  [X] [   55.00697738     0.00000000     0.00000000 ] [i]
  [Y]=[    0.00000000    55.00697738     0.00000000 ]*[j]
  [Z] [    0.00000000     0.00000000    55.00697738 ] [k]
  Dipole moment [Debye]
    X=   15.63422196 Y=  -25.25688248 Z=    5.15701792     Total=    30.14852970
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