[CP2K-user] [CP2K:14596] Re: TDDFPT calculations with CP2K7.1 using the range-separated functionals

Fangyong Yan fyya... at gmail.com
Wed Jan 20 17:58:39 UTC 2021


Hi, Xiang-Yang,

Regards your comment:
"Since TDDFT is a single point calculation and I believe the single point
calculations using different programs should obtain similar results, which
is the spirit of Science."

I partially agree with you:
1) The cp2k uses pseudopotential for TDDFT, and Gaussian uses all-electron,
so they should not give the exactly same result;
2) the main difference only happens for hybrid functional, in Gaussian the
potential operator is 1/r; in cp2k, you use mix_CL_truncated, so it can
result in difference. Also, I dont know how the parameters are set up, such
as omega, scaled coulomb, scaled long range, etc.

Regards,

Fangyong



On Wed, Jan 20, 2021 at 11:02 AM liu xiangyang <lxyl... at gmail.com> wrote:

> Hi, Fangyong,
>
> Thanks a lot for your kindness and patience for doing so much testings and
> Sorry for the delay to reply so late since I have not login this site these
> days.
> I agree with your results since I have also test the results using pure
> functionals GGA such as PBE functional previously and the results agree
> perferctly well when using G09 and CP2K respectively, just as the BLYP
> functional you tested in the first place. However, as you have found, the
> results obtained using the range separated functional wB97XD are distinct
> from each other.
> I have noticed your suggestion that the optimization might be the origin
> of the discrepancy. However, this structure is modified from a previously
> optimized structure of ZnPc and I have not optimized it at all.
> Since TDDFT is a single point calculation and I believe the single point
> calculations using different programs should obtain similar results, which
> is the spirit of Science.
> I tend to believe that there are some differences between the TDDFPT
> method implemented in CP2K and TDDFT in G09, which makes the TDDFPT
> unsuitable for the calculation using the range-separated functionals.
> However, I have not found a efficient that could fix such differences yet
> and I believe this issue is important since the GGA functional might not be
> accurate enough for describing charge transfer states, which always need
> range separated functionals.
>
> Sincerely Yours,
> Xiang-Yang Liu
>
> On Friday, January 15, 2021 at 8:26:30 PM UTC+8 fy... at gmail.com wrote:
>
>> Hi, XIangyang,
>>
>> One possibility is that your structure has been optimized using Gaussian,
>> which uses all-electron calculation (I assume your structure is optimized).
>> While cp2k uses pseudopotential. So the Gaussian optimized structure may
>> not be the cp2k optimized structure.
>>
>> While this optimization issue may not be a problem with PBE/BLYP, it may
>> be a problem for hybrid functional, especially for your structure.
>>
>> So maybe you can optimize your structure using pseudopotential in cp2k,
>> once you get your optimized structure, you do tddfpt calculation.
>>
>> Regards,
>>
>> Fangyong
>>
>>
>> On Fri, Jan 15, 2021 at 6:40 AM Fangyong Yan <fy... at gmail.com> wrote:
>>
>>> 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 <fy... 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 <fy... 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 <el... 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 (<lx... 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*
>>>>>>>>>>>
>>>>>>>>>> --
>>>>>>>>>> You received this message because you are subscribed to the
>>>>>>>>>> Google Groups "cp2k" group.
>>>>>>>>>> To unsubscribe from this group and stop receiving emails from it,
>>>>>>>>>> send an email to cp... at googlegroups.com.
>>>>>>>>>> To view this discussion on the web visit
>>>>>>>>>> https://groups.google.com/d/msgid/cp2k/4897d4d1-a074-44f6-89ff-3b2c613eab83n%40googlegroups.com
>>>>>>>>>> <https://groups.google.com/d/msgid/cp2k/4897d4d1-a074-44f6-89ff-3b2c613eab83n%40googlegroups.com?utm_medium=email&utm_source=footer>
>>>>>>>>>> .
>>>>>>>>>>
>>>>>>>>> --
>>>>>>> You received this message because you are subscribed to the Google
>>>>>>> Groups "cp2k" group.
>>>>>>> To unsubscribe from this group and stop receiving emails from it,
>>>>>>> send an email to cp... at googlegroups.com.
>>>>>>> To view this discussion on the web visit
>>>>>>> https://groups.google.com/d/msgid/cp2k/64940b8a-9bef-4f42-9833-55b0ddaa7326n%40googlegroups.com
>>>>>>> <https://groups.google.com/d/msgid/cp2k/64940b8a-9bef-4f42-9833-55b0ddaa7326n%40googlegroups.com?utm_medium=email&utm_source=footer>
>>>>>>> .
>>>>>>>
>>>>>> --
>>>>>> You received this message because you are subscribed to the Google
>>>>>> Groups "cp2k" group.
>>>>>> To unsubscribe from this group and stop receiving emails from it,
>>>>>> send 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>
>>>>>> .
>>>>>>
>>>>> --
> You received this message because you are subscribed to the Google Groups
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> To unsubscribe from this group and stop receiving emails from it, send an
> email to cp... at googlegroups.com.
> To view this discussion on the web visit
> https://groups.google.com/d/msgid/cp2k/6540e59d-ff9f-4c8c-b550-2247e0d60cd1n%40googlegroups.com
> <https://groups.google.com/d/msgid/cp2k/6540e59d-ff9f-4c8c-b550-2247e0d60cd1n%40googlegroups.com?utm_medium=email&utm_source=footer>
> .
>
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