[CP2K-user] cutoff-convergence
Travis
polla... at gmail.com
Thu Oct 10 20:07:57 UTC 2019
Hi,
The tutorial works because it is a simple case with small exponents in the
basis set. If you have an element (or especially cation) with large
exponents in the basis set, you need to use a higher cutoff. The CUTOFF
should be at least as large as the largest exponent in your basis set
multiplied by the REL_CUTOFF. Then round up to a nice number to report in
the paper, nearest 10, 20, 50, or 100 are common. Na, Mg, H, and O are
common elements to base your cutoff on.
Na DZVP-GTH-q9 DZVP-GTH
2
2 0 1 6 3 2
*17.6698382207* -0.1362364777 0.0270957219 0.0000000000
0.0791980974 0.0000000000
6.9070658063 -0.0645835666 0.0098734119 0.0000000000
0.2184139257 0.0000000000
2.6098601451 0.3866153961 -0.0737170396 0.0000000000
0.3764887364 0.0000000000
0.9649548796 0.5971358883 -0.2186742776 0.0000000000
0.3922304007 0.0000000000
0.3400348369 0.1756697026 -0.0301066303 0.0000000000
0.1808407220 0.0000000000
0.0432486046 -0.0017104621 1.0388865857 1.0000000000
0.0057696324 1.0000000000
3 2 2 1 1
0.0973000000 1.0000000000
In my experience, REL_CUTOFF=50 Ry is a good choice for static cell
calculations and REL_CUTOFF=80 Ry is a good choice for dynamic cell
calculations. Both figures are based on experience with condensed phase
simulation. This leads to CUTOFFs of ~600 Ry and ~1000 Ry for liquid water
for NVT and NPT simulations, respectively. The devs had a recent paper on
accurate simulations of liquid water which draws similar conclusions when
not using smoothing.
-T
On Thursday, October 10, 2019 at 8:13:29 AM UTC-3, Akshay Malik wrote:
>
> Dear all,
> I am trying to do cutoff-convergence for my system but it is only
> converging up to two digits after the decimal point.
> Please suggest some method by which I can get converged energy up to 6
> decimals.
>
> # Grid cutoff vs total energy
> # Date: Thu Oct 10 16:37:32 IST 2019
> # PWD: /home/space/cp2k/cutoff-convergence
> # REL_CUTOFF = 60
> # Cutoff (Ry) | Total Energy (Ha) | NG on grid 1 | NG on grid 2 | NG on
> grid 3 | NG on grid 4
> 50.00 -1337.8915343935 668903 50882 240 0
> 100.00 -1351.0266889654 1216132 286203 11290 0
> 150.00 -1351.6349634609 1071797 364690 75938 1200
> 200.00 -1351.6825629692 975942 418150 115933 3600
> 250.00 -1351.6992612267 875755 439820 192650 5400
> 300.00 -1351.6990099247 791971 424161 286203 11290
> 350.00 -1351.6961310939 735698 431201 323555 23171
> 400.00 -1351.6944391280 687700 428173 341928 55824
> 450.00 -1351.6933108152 644645 427152 364690 77138
> 500.00 -1351.6931016574 603223 441589 368145 100668
>
> I am using this cp2k file section for calculating energy:
> &FORCE_EVAL
> METHOD Quickstep
> &DFT
> BASIS_SET_FILE_NAME GTH_BASIS_SETS
> POTENTIAL_FILE_NAME GTH_POTENTIALS
> &MGRID
> NGRIDS 4
> CUTOFF LT_cutoff
> REL_CUTOFF LT_rel_cutoff
> &END MGRID
> &QS
> EPS_DEFAULT 1.0E-10
> &END QS
> &SCF
> SCF_GUESS ATOMIC
> EPS_SCF 1.0E-6
> MAX_SCF 1
> ADDED_MOS 10
> CHOLESKY INVERSE
> &SMEAR ON
> METHOD FERMI_DIRAC
> ELECTRONIC_TEMPERATURE [K] 333
> &END SMEAR
> &DIAGONALIZATION
> ALGORITHM STANDARD
> &END DIAGONALIZATION
> &MIXING
> METHOD BROYDEN_MIXING
> ALPHA 0.4
> BETA 0.5
> NBROYDEN 8
> &END MIXING
> &END SCF
> &XC
> &XC_FUNCTIONAL BLYP
> &END
> &END
> &END DFT
>
>
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