[CP2K-user] [CP2K:14520] Re: TDDFPT calculations with CP2K7.1 using the range-separated functionals

Fangyong Yan fyya... at gmail.com
Fri Jan 15 11:40:27 UTC 2021


Hi, Xiangyang,

I tested your functional, and got the similar result as yours.

However, I have tested both blyp and pbe, both are in good agreement with
Gaussian. So the discrepancy may only happen for hybrid functionals, and I
dont know the reason.

Regards,

Fangyong

On Thu, Jan 14, 2021 at 7:20 PM Fangyong Yan <fyya... at gmail.com> wrote:

> Hi, XIangyan,
>
> I changed the functional type for atoms, from GTH-PBE-q4 => GTH-BLYP-q4,
> since I am using BLYP. (Sorry, I just copied your basis set and functionals
> and did not realize the difference.)
>
> Here is the result, and is in good agreement with Gaussian 09.
>
>          State    Excitation        Transition dipole (a.u.)
> Oscillator
>
>          number   energy (eV)       x           y           z     strength
> (a.u.)
>
>
> ------------------------------------------------------------------------
>
>  TDDFPT|      1       2.08325  -2.4674E+00  8.6733E-03 -6.5509E-03
> 3.10723E-01
>
>  TDDFPT|      2       2.16407   1.4338E-02  2.9818E+00  1.0596E-02
> 4.71397E-01
>
>  TDDFPT|      3       2.52106   1.3816E-01  1.4082E-03 -1.0486E-04
> 1.17904E-03
>
>  TDDFPT|      4       2.55291  -8.4802E-01  4.4219E-03 -1.5266E-04
> 4.49799E-02
>
>  TDDFPT|      5       2.58935   1.4471E-04 -4.8114E-02  4.4750E-02
> 2.73894E-04
>
>
> I will test your functional, since it is hybrid, it will take some time.
>
>
> Regards,
>
>
> Fangyong
>
> On Thu, Jan 14, 2021 at 6:47 PM Fangyong Yan <fyya... at gmail.com> wrote:
>
>> Hi, XIangyan,
>>
>> I used you structure, and tested both Gaussian and cp2k, and they have
>> good agreement.
>>
>> So Gaussian and cp2k can both give reasonable results for the excitation
>> energies of your molecule.
>>
>> Gaussian 09, blyp/6-31G*,
>>
>> Excited State   1:      Singlet-A      1.9414 eV  638.63 nm  f=0.2542
>> <S**2>=0.000
>>
>> Excited State   2:      Singlet-A      1.9724 eV  628.58 nm  f=0.3319
>> <S**2>=0.000
>>
>> Excited State   3:      Singlet-A      2.5113 eV  493.71 nm  f=0.0038
>> <S**2>=0.000
>>
>> Excited State   4:      Singlet-A      2.5205 eV  491.90 nm  f=0.0341
>> <S**2>=0.000
>>
>> Excited State   5:      Singlet-A      2.5764 eV  481.23 nm  f=0.0001
>> <S**2>=0.000
>>
>> cp2k, blyp/TZVP, with GTH pseudopotential,
>>
>> I get
>>
>>          State    Excitation        Transition dipole (a.u.)
>> Oscillator
>>
>>          number   energy (eV)       x           y           z     strength
>> (a.u.)
>>
>>
>> ------------------------------------------------------------------------
>>
>>  TDDFPT|      1       2.08760   2.4868E+00 -8.6129E-03  6.4653E-03
>> 3.16297E-01
>>
>>  TDDFPT|      2       2.16739  -1.4224E-02 -2.9924E+00 -1.0393E-02
>> 4.75501E-01
>>
>>  TDDFPT|      3       2.52956  -1.3916E-01 -1.4062E-03  1.0520E-04
>> 1.20031E-03
>>
>>  TDDFPT|      4       2.56128   8.4944E-01 -4.4270E-03  1.5135E-04
>> 4.52790E-02
>>
>>  TDDFPT|      5       2.59590  -1.3595E-04  4.4904E-02 -4.4546E-02
>> 2.54439E-04
>>
>>  TDDFPT|      6       2.60688  -3.1839E-03  4.1336E-02  2.5674E-02
>> 1.51876E-04
>>
>>  TDDFPT|      7       2.76485  -3.0533E-03 -2.4437E-01  1.0913E-03
>> 4.04581E-03
>>
>>  TDDFPT|      8       2.80552  -2.7107E-01 -4.8867E-03 -9.2586E-04
>> 5.05222E-03
>>
>>  TDDFPT|      9       2.88205  -1.2938E-02 -1.3849E-04  1.2856E-03
>> 1.19366E-05
>>
>>  TDDFPT|     10       2.92954   2.8231E-05  6.4011E-03 -8.3886E-02
>> 5.07991E-04
>>
>> ****************** Below is the input.
>>
>>   &SUBSYS
>>
>>     &CELL
>>
>>       ABC  30. 30. 6.
>>
>>       PERIODIC none
>>
>>     &END CELL
>>
>>     &COORD
>>
>>     &KIND C
>>
>>       BASIS_SET TZVP-GTH
>>
>>       POTENTIAL GTH-PBE-q4
>>
>>     &END KIND
>>
>>     &KIND N
>>
>>       BASIS_SET TZVP-GTH
>>
>>       POTENTIAL GTH-PBE-q5
>>
>>     &END KIND
>>
>>     &KIND H
>>
>>       BASIS_SET TZVP-GTH
>>
>>       POTENTIAL GTH-PBE-q1
>>
>>     &END KIND
>>
>>     &QS
>>
>>       METHOD GPW
>>
>>       MAP_CONSISTENT  T
>>
>>       EPS_DEFAULT 1.0E-9
>>
>>     &END QS
>>
>>     &XC
>>
>>       &XC_FUNCTIONAL BLYP
>>
>>       &END XC_FUNCTIONAL
>>
>>
>>       &XC_GRID
>>
>>         XC_DERIV SPLINE2_SMOOTH      # this is needed for the 2nd
>> derivatives of the XC functional
>>
>>       &END XC_GRID
>>
>>     &END XC
>>
>>     &SCF
>>
>>       MAX_SCF   250
>>
>>       EPS_SCF   1e-8
>>
>>       SCF_GUESS atomic
>>
>>     &END SCF
>>
>>     &MGRID
>>
>>       CUTOFF 600
>>
>>       NGRIDS 4
>>
>>       REL_CUTOFF 60
>>
>>     &END MGRID
>>
>>
>>     &POISSON
>>
>>        PERIODIC none
>>
>>        POISSON_SOLVER MT
>>
>>     &END POISSON
>>
>>   &PROPERTIES
>>
>>     &TDDFPT
>>
>>        NSTATES     10             # number of excited states
>>
>>        MAX_ITER    100             # maximum number of Davidson
>> iterations
>>
>>        CONVERGENCE [eV] 1.0e-3    # convergence on maximum energy change
>> between iterations
>>
>>
>>        &MGRID
>>
>>           CUTOFF 300  # separate cutoff for TDDFPT calc
>>
>>        &END
>>
>>     &END TDDFPT
>>
>>   &END PROPERTIES
>>
>>
>> Regares,
>>
>>
>> Fangyong
>>
>> On Tue, Jan 12, 2021 at 6:50 PM Lucas Lodeiro <eluni... at gmail.com>
>> wrote:
>>
>>> Hi Liu,
>>>
>>> As you mention it is a little weird if other molecules work fine with
>>> the same input. I guess the next test is to tighten the convergence
>>> criteria in CP2K if it is possible.
>>> Another thing, remember that for non periodic calculations, you have to
>>> set periodic none in the poisson and cell section.
>>>
>>> *    &CELL*
>>> *      ABC 30.0 30.0 30.0*
>>> *      PERIODIC NONE*
>>> *    &END CELL*
>>>
>>> I see the transition energies change a little bit, it is at least
>>> comfortable, showing that one or more changes you did affect the result.
>>> Maybe as the last chance there will be  useful to know which change was the
>>> one that caused the variation a the energies.
>>>
>>> Sorry, it does not seem a simple problem.
>>> Regards
>>>
>>>
>>> El mar, 12 ene 2021 a las 1:49, liu xiangyang (<lxyl... at gmail.com>)
>>> escribió:
>>>
>>>> Hi  Vladimir  & Lucas,
>>>>
>>>> Thanks a lot for your kindly responses. Actually, I have also tested
>>>> small molecule such as H2CO using present settings and the results obtained
>>>> by CP2K and G09 are quanlitatively in good agreement with each other and
>>>> THAT IS THE FACT THAT PUZZLES ME MOST.
>>>>
>>>> According to your suggestions, I have made several changes to my input
>>>> file, including removal of the periodic conditions, removal of the ADMM
>>>> approximations to avoid possible mistakes, and  lower the convergence in
>>>> G09 since the computational efforts of CP2K is much larger. The basis sets
>>>> are not changed since the TDDFPT in CP2K is implemented only in GPW method,
>>>> which is unable to do calculations with all electron basis sets such as
>>>> Pople basis sets. However, I believe the difference of basis set (DZVP-GTH
>>>> vs. 6-31G*) should not be so large. Unfortunately, the results of CP2K7.1
>>>> is still about 1 eV lower than that obtained in G09 (1.19 and 1.25 eV in
>>>> CP2K vs. 2.18 and 2.26 eV in G09).
>>>>
>>>> PS. I have also run GAPW calculations in CP2K using the WB97XD/6-31G**
>>>> and the resulted ground state energy are nearly the same as that obtained
>>>> in G09 (differenceless than 0.002 hartree).
>>>>
>>>> The modified DFT parts of CP2K  input file is attatched also:
>>>>
>>>> &DFT
>>>>     BASIS_SET_FILE_NAME BASIS_MOLOPT
>>>>     POTENTIAL_FILE_NAME POTENTIAL
>>>>
>>>>     CHARGE 0
>>>>     &MGRID
>>>>       CUTOFF 400
>>>>     &END MGRID
>>>>     &QS
>>>>       METHOD gpw
>>>>       EPS_PGF_ORB 1e-12
>>>>     &END QS
>>>>     &SCF
>>>>       MAX_SCF   100
>>>>       EPS_SCF   1e-5
>>>>       SCF_GUESS atomic
>>>>
>>>>       &DIAGONALIZATION
>>>>         ALGORITHM STANDARD
>>>>       &END DIAGONALIZATION
>>>>
>>>>       &MIXING T
>>>>         ALPHA 0.5
>>>>         METHOD PULAY_MIXING
>>>>         NPULAY 5
>>>>       &END MIXING
>>>>     &END SCF
>>>>     &POISSON
>>>>        PERIODIC NONE
>>>>        PSOLVER MT
>>>>     &END POISSON
>>>>
>>>>     &XC
>>>>       &XC_FUNCTIONAL
>>>>         &LIBXC
>>>>           FUNCTIONAL HYB_GGA_XC_WB97X_D
>>>>         &END
>>>>       &END XC_FUNCTIONAL
>>>>       &HF
>>>>        &SCREENING
>>>>          EPS_SCHWARZ 1.0E-6
>>>>        &END
>>>>        &MEMORY
>>>>          MAX_MEMORY 100
>>>>        &END
>>>>        &INTERACTION_POTENTIAL
>>>>          POTENTIAL_TYPE MIX_CL
>>>>          OMEGA 0.2
>>>>          SCALE_LONGRANGE 0.777964
>>>>          SCALE_COULOMB 0.222036
>>>>        &END
>>>>       &END
>>>>     &END XC
>>>>
>>>>   &END DFT
>>>>
>>>> Best wishes,
>>>> Xiang-Yang Liu
>>>>
>>>> On Tuesday, January 12, 2021 at 7:07:34 AM UTC+8 ry... at gmail.com
>>>> wrote:
>>>>
>>>>> Sorry, I really read the differences incorrectly. Thank you, Lukas,
>>>>> for correcting me.
>>>>>
>>>>> понедельник, 11 января 2021 г. в 21:02:30 UTC+1, Lucas Lodeiro:
>>>>>
>>>>>> Hi Liu,
>>>>>> I did not run TDDFT calculations, but I did some tests between CP2K
>>>>>> and other programs like G09. As Vladimir says, your basis sets are not the
>>>>>> same, and some difference could appear due to this reason. But in your case
>>>>>> the differences are big, 1.6 eV approx. I found that some default settings
>>>>>> of convergences criterium are differents, for example the *EPS_SCF* which
>>>>>> is 1E-8 in G09, you could tight your convergence criterion,
>>>>>> *EPS_SCF, **EPS_DEFAULT, **EPS_SCHWARZ* to -8, -12 and -8 to get
>>>>>> results with similar convergences in both programs. Also, you are using a
>>>>>> PBC calculation in a big cell, but maybe it is no sufficient to mimic the
>>>>>> isolated molecule as in G09... and yout cutoff radius for HF is a little
>>>>>> bit short, if you run a non-periodic calculation, you can use just the long
>>>>>> range potential without the truncation.
>>>>>> Finally, just to speed up, you can use OT instead of diagonalization
>>>>>> method, with it you can use *ADMM_PURIFICATION_METHOD *MO_DIAG.
>>>>>>
>>>>>> In order to have the same basis sets, as vladimir says, you could
>>>>>> explore  to use the same basis sets in both programs, you can get basis
>>>>>> sets to both programs from: https://www.basissetexchange.org/
>>>>>> And the Auxiliary basis set is the minimum one, you could explore FIT
>>>>>> and pFIT basis set to check if the result is sensitive.
>>>>>>
>>>>>> Regards
>>>>>> Lucas Lodeiro
>>>>>>
>>>>>> El lun, 11 ene 2021 a las 13:01, Vladimir Rybkin (<ry... at gmail.com>)
>>>>>> escribió:
>>>>>>
>>>>>>> Dear Xiang-Yang Liu,
>>>>>>>
>>>>>>> most importantly: you are using different basis sets in Gaussian and
>>>>>>> CP2K (CP2K also use pseudopotentials). With this difference in mind you
>>>>>>> differences are within reasonable. Generally, difference below 0.1 eV for
>>>>>>> TDDFT implementations is not "great".
>>>>>>>
>>>>>>> Yours,
>>>>>>>
>>>>>>> Vladimir
>>>>>>>
>>>>>>> понедельник, 11 января 2021 г. в 14:49:47 UTC+1, lx... at gmail.com:
>>>>>>>
>>>>>>>> Dear All,
>>>>>>>>
>>>>>>>> I have tried to use the TDDFPT method implemented in CP2K7.1 to do
>>>>>>>> excited state calculations with the range-separated functionals such as
>>>>>>>> wB97XD.
>>>>>>>> However, after several tests with a small molecule, namely H2Pc, I
>>>>>>>> found that the first two excitation energies are greatly underestimated in
>>>>>>>> comparison with the LR-TDDFT results obtained in  GAUSSIAN09 (ca. 0.51 and
>>>>>>>> 0.60 eV (CP2K7.1) vs. 2.18 and 2.26 eV (GAUSSIAN09)).
>>>>>>>> I wonder whether there are some mistakes with my input file or
>>>>>>>> there are some problem of TDDFPT for such calculations?
>>>>>>>>
>>>>>>>> The input file used in my calculations is written as follows:
>>>>>>>>
>>>>>>>> *&GLOBAL*
>>>>>>>> *  PROJECT tddfpt*
>>>>>>>> *  RUN_TYPE energy*
>>>>>>>> *  PRINT_LEVEL medium*
>>>>>>>> *&END GLOBAL*
>>>>>>>>
>>>>>>>> *&FORCE_EVAL*
>>>>>>>> *  METHOD Quickstep*
>>>>>>>>
>>>>>>>> *  &PROPERTIES*
>>>>>>>> *    &TDDFPT*
>>>>>>>> *       NSTATES  5            # number of excited states*
>>>>>>>> *    &END TDDFPT*
>>>>>>>> *  &END PROPERTIES*
>>>>>>>>
>>>>>>>> *&DFT*
>>>>>>>> *    BASIS_SET_FILE_NAME GTH_BASIS_SETS*
>>>>>>>> *    POTENTIAL_FILE_NAME POTENTIAL*
>>>>>>>> *    BASIS_SET_FILE_NAME BASIS_ADMM_MOLOPT*
>>>>>>>> *    BASIS_SET_FILE_NAME BASIS_ADMM*
>>>>>>>>
>>>>>>>> *    &AUXILIARY_DENSITY_MATRIX_METHOD*
>>>>>>>> *      METHOD BASIS_PROJECTION*
>>>>>>>> *      ADMM_PURIFICATION_METHOD NONE *
>>>>>>>> *      EXCH_CORRECTION_FUNC BECKE88X*
>>>>>>>> *    &END AUXILIARY_DENSITY_MATRIX_METHOD*
>>>>>>>>
>>>>>>>> *    CHARGE 0 *
>>>>>>>> *    &MGRID*
>>>>>>>> *      CUTOFF 400*
>>>>>>>> *    &END MGRID*
>>>>>>>> *    &QS*
>>>>>>>> *      METHOD gpw*
>>>>>>>> *      EPS_PGF_ORB 1e-12*
>>>>>>>> *    &END QS*
>>>>>>>> *    &SCF*
>>>>>>>> *      MAX_SCF   100*
>>>>>>>> *      EPS_SCF   1e-5*
>>>>>>>> *      SCF_GUESS atomic*
>>>>>>>>
>>>>>>>> *      &DIAGONALIZATION*
>>>>>>>> *        ALGORITHM STANDARD*
>>>>>>>> *      &END DIAGONALIZATION*
>>>>>>>>
>>>>>>>> *      &MIXING T*
>>>>>>>> *        ALPHA 0.5*
>>>>>>>> *        METHOD PULAY_MIXING*
>>>>>>>> *        NPULAY 5*
>>>>>>>> *      &END MIXING*
>>>>>>>> *    &END SCF*
>>>>>>>> *    &POISSON*
>>>>>>>> *       PERIODIC XYZ*
>>>>>>>> *    &END POISSON*
>>>>>>>>
>>>>>>>> *    &XC*
>>>>>>>> *      &XC_FUNCTIONAL*
>>>>>>>> *        &LIBXC*
>>>>>>>> *          FUNCTIONAL HYB_GGA_XC_WB97X_D*
>>>>>>>> *        &END*
>>>>>>>> *      &END XC_FUNCTIONAL*
>>>>>>>> *      &HF*
>>>>>>>> *       &SCREENING*
>>>>>>>> *         EPS_SCHWARZ 1.0E-6*
>>>>>>>> *       &END*
>>>>>>>> *       &MEMORY*
>>>>>>>> *         MAX_MEMORY 100*
>>>>>>>> *       &END*
>>>>>>>> *       &INTERACTION_POTENTIAL*
>>>>>>>> *         POTENTIAL_TYPE MIX_CL_TRUNC*
>>>>>>>> *         OMEGA 0.2*
>>>>>>>> *         SCALE_LONGRANGE 0.777964*
>>>>>>>> *         SCALE_COULOMB 0.222036*
>>>>>>>> *         CUTOFF_RADIUS 5.0*
>>>>>>>> *         T_C_G_DATA t_c_g.dat*
>>>>>>>> *       &END*
>>>>>>>> *      &END*
>>>>>>>> *      &XC_GRID*
>>>>>>>> *        XC_DERIV SPLINE2_SMOOTH      # this is needed for the 2nd
>>>>>>>> derivatives of the XC functional*
>>>>>>>> *      &END XC_GRID*
>>>>>>>> *    &END XC*
>>>>>>>>
>>>>>>>> *  &END DFT*
>>>>>>>> *  &SUBSYS*
>>>>>>>> *    &TOPOLOGY*
>>>>>>>> *       &CENTER_COORDINATES*
>>>>>>>> *       &END CENTER_COORDINATES*
>>>>>>>> *    &END TOPOLOGY*
>>>>>>>> *    &CELL*
>>>>>>>> *      ABC 30.0 30.0 30.0*
>>>>>>>> *      PERIODIC XYZ*
>>>>>>>> *    &END CELL*
>>>>>>>> *    &COORD*
>>>>>>>> * N                  0.01468800    2.00544200   -0.29683900*
>>>>>>>> * N                 -2.37562900    2.41155000   -0.13186300*
>>>>>>>> * N                 -2.41200400   -2.37377100   -0.17491600*
>>>>>>>> * N                  2.41112400    2.37299900   -0.12658700*
>>>>>>>> * N                 -0.01307800   -2.00591400   -0.34375500*
>>>>>>>> * N                  2.37788800   -2.41418900   -0.17065800*
>>>>>>>> * C                 -4.17222800    0.73645800   -0.00309900*
>>>>>>>> * C                 -0.67412900    4.18239500    0.01934000*
>>>>>>>> * C                 -4.18380100   -0.67562700   -0.02014000*
>>>>>>>> * C                  0.73808000    4.17070300    0.02178600*
>>>>>>>> * C                 -2.78102300    1.14403300   -0.18692600*
>>>>>>>> * C                 -1.10192300    2.79691600   -0.16605600*
>>>>>>>> * C                 -2.79906300   -1.10173400   -0.21220500*
>>>>>>>> * C                  1.14375300    2.77826000   -0.16260500*
>>>>>>>> * C                 -0.73890800   -4.16630900   -0.00019300*
>>>>>>>> * C                  4.18311400    0.67096100    0.00115100*
>>>>>>>> * C                  0.67355900   -4.17905700    0.00226800*
>>>>>>>> * C                  4.17314700   -0.74140800   -0.01277100*
>>>>>>>> * C                 -1.14329800   -2.77792600   -0.20621200*
>>>>>>>> * C                  2.79688300    1.09912600   -0.17512500*
>>>>>>>> * C                  1.10326800   -2.79777700   -0.20275300*
>>>>>>>> * C                  2.78178900   -1.14729500   -0.19912900*
>>>>>>>> * C                 -5.34524900    1.46617200    0.20504700*
>>>>>>>> * C                 -1.38645100    5.36877700    0.20954200*
>>>>>>>> * C                 -5.36863500   -1.39063500    0.17089500*
>>>>>>>> * C                  1.47037200    5.34443400    0.21437700*
>>>>>>>> * C                 -6.53049700    0.75063900    0.38667600*
>>>>>>>> * C                 -0.65342400    6.54324100    0.39406800*
>>>>>>>> * C                 -6.54209900   -0.66018000    0.36971000*
>>>>>>>> * C                  0.75719100    6.53149500    0.39645600*
>>>>>>>> * C                 -1.47251300   -5.33425600    0.22345700*
>>>>>>>> * C                  5.36943600    1.38205000    0.19903500*
>>>>>>>> * C                  1.38473700   -5.36039200    0.22884400*
>>>>>>>> * C                  5.34798200   -1.47459500    0.17084800*
>>>>>>>> * C                 -0.76071300   -6.51537100    0.44153000*
>>>>>>>> * C                  6.54461400    0.64821000    0.37381100*
>>>>>>>> * C                  0.65044900   -6.52827600    0.44412700*
>>>>>>>> * C                  6.53422100   -0.76263800    0.36007100*
>>>>>>>> * H                 -5.31982100    2.55648400    0.22741200*
>>>>>>>> * H                 -2.47726000    5.36199000    0.21499900*
>>>>>>>> * H                 -5.36047700   -2.48141400    0.16783300*
>>>>>>>> * H                  2.56090800    5.31878300    0.22274500*
>>>>>>>> * H                 -7.46690300    1.28881400    0.54987000*
>>>>>>>> * H                 -1.17840000    7.48942700    0.54335800*
>>>>>>>> * H                 -7.48727000   -1.18662900    0.52012100*
>>>>>>>> * H                  1.29740200    7.46875700    0.54746900*
>>>>>>>> * H                 -2.56294400   -5.30668600    0.23110100*
>>>>>>>> * H                  5.36158400    2.47267500    0.21857200*
>>>>>>>> * H                  2.47541900   -5.35281000    0.24119000*
>>>>>>>> * H                  5.32277600   -2.56515200    0.16738300*
>>>>>>>> * H                 -1.30192600   -7.44735900    0.61932200*
>>>>>>>> * H                  7.49034300    1.17231500    0.52877000*
>>>>>>>> * H                  1.17373400   -7.47001200    0.62407400*
>>>>>>>> * H                  7.47217800   -1.30348900    0.50426500*
>>>>>>>> * H                 -0.95410508    0.01210298   -0.52371821*
>>>>>>>> * H                  0.94993522   -0.00596112   -0.48792422*
>>>>>>>> * N                 -2.00779500    0.01729500   -0.33767900*
>>>>>>>> * N                  2.00585900   -0.01636500   -0.31524900*
>>>>>>>> *    &END COORD*
>>>>>>>> *    &KIND N*
>>>>>>>> *      BASIS_SET DZVP-GTH*
>>>>>>>> *      POTENTIAL GTH-PBE*
>>>>>>>> *      BASIS_SET AUX_FIT cFIT3*
>>>>>>>> *    &END KIND*
>>>>>>>> *    &KIND C*
>>>>>>>> *      BASIS_SET DZVP-GTH*
>>>>>>>> *      POTENTIAL GTH-PBE*
>>>>>>>> *      BASIS_SET AUX_FIT cFIT3*
>>>>>>>> *    &END KIND*
>>>>>>>> *    &KIND H*
>>>>>>>> *      BASIS_SET DZVP-GTH*
>>>>>>>> *      POTENTIAL GTH-PBE*
>>>>>>>> *      BASIS_SET AUX_FIT cFIT3*
>>>>>>>> *    &END KIND*
>>>>>>>> *  &END SUBSYS*
>>>>>>>> *&END FORCE_EVAL*
>>>>>>>>
>>>>>>>> *Best wishes, *
>>>>>>>> *Xiang-Yang Liu*
>>>>>>>>
>>>>>>> --
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>>>>>>>
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>>> an email to cp... at googlegroups.com.
>>> To view this discussion on the web visit
>>> https://groups.google.com/d/msgid/cp2k/CAOFT4PJ1bAsK-iK5Lnd7YikGQjJYgDxb47dNh5bNH_FeM1U%2BrQ%40mail.gmail.com
>>> <https://groups.google.com/d/msgid/cp2k/CAOFT4PJ1bAsK-iK5Lnd7YikGQjJYgDxb47dNh5bNH_FeM1U%2BrQ%40mail.gmail.com?utm_medium=email&utm_source=footer>
>>> .
>>>
>>
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