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

Fangyong Yan fyya... at gmail.com
Wed Jan 20 18:53:37 UTC 2021


Hi, Xiang-Yang,

I tested B3LYP some time ago using your geometry, which is reasonable:

         State    Excitation        Transition dipole (a.u.)
Oscillator

         number   energy (eV)       x           y           z     strength
(a.u.)


------------------------------------------------------------------------

 TDDFPT|      1       1.86120  -2.0023E+00  8.1993E-03 -3.3226E-03
1.82825E-01

 TDDFPT|      2       1.92870   9.9269E-03  2.2110E+00  4.4788E-03
2.31001E-01

 TDDFPT|      3       3.01758   8.6432E-02  1.8994E-04  7.7692E-06
5.52295E-04

 TDDFPT|      4       3.04539  -6.9340E-01  4.6654E-03 -6.3691E-05
3.58749E-02

 TDDFPT|      5       3.25891  -1.5458E-03 -7.2118E-02 -3.4034E-02
5.07928E-04



Below is the input (part):


      ABC  30. 30. 16.

      PERIODIC none

    &END CELL

    &COORD


 N                  0.01468800    2.00544200   -0.29683900

 N                 -2.37562900    2.41155000   -0.13186300

....

        &INTERACTION_POTENTIAL

          ! for condensed phase systems

          POTENTIAL_TYPE TRUNCATED

          ! should be less than halve the cell

          CUTOFF_RADIUS 6.0

          ! data file needed with the truncated operator

          T_C_G_DATA ./t_c_g.dat

        &END


Regards,


Fangyong

On Wed, Jan 20, 2021 at 12:58 PM Fangyong Yan <fyya... at gmail.com> wrote:

> 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
>> "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/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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