Lowdin analysis
Matthias Krack
matthia... at psi.ch
Tue Dec 7 08:54:12 UTC 2010
Hi Teo,
I checked that already before my first reply. There is no numerical
problem in this case, i.e. there is no warning about quenched
eigenvalues.
Matthias
On Dec 7, 9:35 am, Teodoro Laino <teodor... at gmail.com> wrote:
> Hi Matthias,
>
> maybe yes - maybe no -
> I did not look into the condition number of that matrix -
> A definitive answer (and not just assumptions like mines or yours) would be confirmed or discarded by a more serious check.
>
> Best,
> Teo
>
> On Dec 7, 2010, at 9:30 AM, Matthias Krack wrote:
>
> > Hi Teo,
>
> > I doubt that the applied computational scheme or the numerics are part
> > of the problem, especially not in the case of a single water molecule,
> > and thus any clever approach to evaluate S**(1/2) won't change
> > anything. Maybe, my previous reply unintentionally implied that I
> > would blame the MOLOPT basis set to be the only problem in this case.
> > So let it put me more clearly: just the way how the Lowdin approach is
> > partitioning the charge does not work properly, i.e. giving physically
> > meaningful results, for all kinds of basis sets and the MOLOPT basis
> > sets (but not its SR variants) belong to this group.
>
> > Best,
>
> > Matthias
>
> > On Dec 6, 8:03 pm, Teodoro Laino <teodor... at gmail.com> wrote:
> >> Hi Matthias, Mahn,
>
> >> The real problem is not in the basis set itself but in how the population analysis is computed in CP2K.
> >> Diagonalizing S to evaluate S**(1/2) is probably not the smartest thing to do.
>
> >> There are ways to evaluate S**(1/2), definitely numerically more stable, that would allow to have meaningful population analysis even with these "problematic" basis sets (although I still think that it's not the basis set itself to be problematic, rather the computational scheme used).
>
> >> Best,
> >> Teo
>
> >> On Dec 5, 2010, at 3:06 PM, Matthias Krack wrote:
>
> >>> Hi Manh,
>
> >>> population analyses are known to be very sensible to the basis set
> >>> choice. I guess also in this case the TZV2P MOLOPT basis set is the
> >>> reason for the unexpected result. The MOLOPT basis sets include
> >>> relatively small exponents which might cause linear dependencies in
> >>> the overlap matrix. The Lowdin population analysis requires the
> >>> calculation of S**(1/2) which involves (in CP2K) a diagonalisation of
> >>> the overlap matrix. However, an ill-conditioned overlap matrix will
> >>> most likely result in a weird charge partition. Therefore, I would
> >>> suggest to employ different basis sets, e.g. the MOLOPT-SR or the DZVP/
> >>> TZVP basis sets.
>
> >>> Best,
>
> >>> Matthias
>
> >>> On 3 Dez., 17:46, Manh <manht... at gmail.com> wrote:
> >>>> Hello everyone,
>
> >>>> I calculate the Mulliken and Lowdin charges for a water molecule. The
> >>>> results are:
>
> >>>> ----------------------------------------------------------------
>
> >>>> MULLIKEN POPULATION ANALYSIS
>
> >>>> # Atom Element Kind Atomic population Net charge
> >>>> 1 H 1 0.780838 0.219162
> >>>> 2 H 1 0.780981 0.219019
> >>>> 3 O 2 6.438182 -0.438182
> >>>> # Total charge 8.000000 0.000000
>
> >>>> LOWDIN POPULATION ANALYSIS
>
> >>>> # Atom Element Kind Atomic population Net charge
> >>>> 1 H 1 1.210449 -0.210449
> >>>> 2 H 1 1.210473 -0.210473
> >>>> 3 O 2 5.579079 0.420921
> >>>> # Total charge 8.000000 0.000000
>
> >>>> --------------------------------------------------------
>
> >>>> I think that the Lowdin analysis has some problem.
>
> >>>> Here is my input:
>
> >>>> ---------------------------------------------
>
> >>>> &FORCE_EVAL
> >>>> METHOD Quickstep
> >>>> &DFT
> >>>> BASIS_SET_FILE_NAME ../../../BASIS_MOLOPT
> >>>> POTENTIAL_FILE_NAME ../../../GTH_POTENTIALS
> >>>> RESTART_FILE_NAME H2O-RESTART.wfn.wfn
> >>>> &QS
> >>>> METHOD GPW
> >>>> EXTRAPOLATION ASPC
> >>>> EXTRAPOLATION_ORDER 3
> >>>> &END QS
> >>>> &MGRID
> >>>> CUTOFF 400
> >>>> NGRIDS 5
> >>>> &END
> >>>> &SCF
> >>>> MAX_SCF 20
> >>>> SCF_GUESS RESTART
> >>>> EPS_SCF 1.0E-6
> >>>> &OT
> >>>> PRECONDITIONER FULL_SINGLE_INVERSE
> >>>> MINIMIZER CG
> >>>> &END
> >>>> &OUTER_SCF
> >>>> MAX_SCF 10
> >>>> EPS_SCF 1.0E-6
> >>>> &END
> >>>> &PRINT
> >>>> &RESTART
> >>>> &EACH
> >>>> QS_SCF 0
> >>>> GEO_OPT 2
> >>>> &END
> >>>> ADD_LAST NUMERIC
> >>>> FILENAME RESTART.wfn
> >>>> &END
> >>>> &RESTART_HISTORY OFF
> >>>> &END
> >>>> &END
> >>>> &END SCF
>
> >>>> &XC
> >>>> &XC_FUNCTIONAL PBE
> >>>> &END XC_FUNCTIONAL
> >>>> &END XC
>
> >>>> &PRINT
> >>>> &MULLIKEN
> >>>> &END MULLIKEN
>
> >>>> &LOWDIN
> >>>> &END LOWDIN
> >>>> &END
>
> >>>> &END DFT
> >>>> &SUBSYS
> >>>> &CELL
> >>>> ABC [angstrom] 30 30 30
> >>>> &END CELL
> >>>> &TOPOLOGY
> >>>> COORD_FILE_NAME water.xyz
> >>>> COORDINATE xyz
> >>>> &END
>
> >>>> &KIND O
> >>>> BASIS_SET TZV2P-MOLOPT-GTH
> >>>> POTENTIAL GTH-PBE-q6
> >>>> &END KIND
> >>>> &KIND H
> >>>> BASIS_SET TZV2P-MOLOPT-GTH
> >>>> POTENTIAL GTH-PBE-q1
> >>>> &END KIND
>
> >>>> &END SUBSYS
>
> >>>> &END FORCE_EVAL
>
> >>>> &GLOBAL
> >>>> PRINT_LEVEL LOW
> >>>> PROJECT H2O
> >>>> RUN_TYPE ENERGY
> >>>> WALLTIME 285000
> >>>> &END GLOBAL
>
> >>>> &MOTION
> >>>> &GEO_OPT
> >>>> MAX_ITER 5000
> >>>> MAX_FORCE 0.00010
> >>>> OPTIMIZER BFGS
> >>>> &BFGS
> >>>> &END
> >>>> &END
> >>>> &END
>
> >>>> ------------------------------------------------
> >>>> the water.xyz file is
> >>>> ----------------------------------------
> >>>> 3
> >>>> water
> >>>> H 8.4351137971 5.1620318678 12.1510352783
> >>>> H 8.5534822942 3.6347695084 12.1803075532
> >>>> O 7.9011326518 4.3528437024 12.1874564118
> >>>> ------------------------------------------------
>
> >>>> Regards,
> >>>> Manh
>
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