[CP2K-user] [CP2K:17673] Bad convergence performance for the MXene system
Thomas Kühne
tkuehne at gmail.com
Wed Sep 14 07:38:26 UTC 2022
Dear Justin,
please sent the output, i.e. in particular during the OT loop for better assistance.
Typical, hints may be:
(i) set EPS_DEFAULT to 1.0E-12
(ii) reduce MAX_SCF in the inner OT loop to s.th. more reasonable than 40-50.
(iii) reduce stepsize to 0.1 or lower
(iv) use different PRECONDITIONER such as FULL_ALL to together with
ENERGY_GAP 0.0001
(v) use CG instead of DIIS
Best,
Thomas Kühne
> Am 25.08.2022 um 09:47 schrieb zhouk... at gmail.com <zhoukedoit at gmail.com>:
>
> Here is the input and structure file.
>
> 在2022年8月25日星期四 UTC+8 15:45:28<zhouk... at gmail.com> 写道:
> Dear all,
>
> Now I am simulation the MXene (Ti3C2O2)+water system. But SCF can not converge.
> The initial structure is from the MD simulation using VASP (PBE+D3) and thus the problem is not from bad positions of atoms.
>
> Can anyone give me some suggestions?
>
> Best,
> Justin
> -----------------------------------------------------------------
> &FORCE_EVAL
> ! the electronic structure part of CP2K is named Quickstep
> METHOD Quickstep
> STRESS_TENSOR ANALYTICAL
> &DFT
> BASIS_SET_FILE_NAME ./BASIS_MOLOPT
> POTENTIAL_FILE_NAME ./POTENTIAL
> WFN_RESTART_FILE_NAME ./MX-RESTART.wfn
> &MGRID
> CUTOFF [Ry] 400
> &END
> &QS
> ! use the GPW method (i.e. pseudopotential based calculations with the Gaussian and Plane Waves scheme).
> METHOD GPW
> ! default threshold for numerics ~ roughly numerical accuracy of the total energy per electron,
> ! sets reasonable values for all other thresholds.
> EPS_DEFAULT 1.0E-10
> ! used for MD, the method used to generate the initial guess.
> EXTRAPOLATION ASPC
> EXTRAPOLATION_ORDER 4
> &END
>
> &POISSON
> PERIODIC XYZ ! the default, gas phase systems should have 'NONE' and a wavelet solver
> &END
> &PRINT
> ! output atomic charge
> &MULLIKEN
> ! FILENAME ${SYSTEM}
> &EACH
> MD 10
> &END EACH
> &END MULLIKEN
> ! output others
> &END
> ! use the OT METHOD for robust and efficient SCF, suitable for all non-metallic systems.
> &SCF
> SCF_GUESS RESTART !!!#####ATOMIC ! can be used to RESTART an interrupted calculation
> MAX_SCF 1000
> EPS_SCF 1.0E-7
> &OUTER_SCF ! repeat the inner SCF cycle 10 times
> MAX_SCF 10
> EPS_SCF 1.0E-7
> &END
>
> &OT ON
> MINIMIZER DIIS
> &END OT
>
>
>
> &END SCF
>
> ! specify the exchange and correlation treatment
> &XC
> ! use a PBE functional
> &XC_FUNCTIONAL PBE
> &END XC_FUNCTIONAL
> ! adding Grimme's D3 correction (by default without C9 terms)
> &VDW_POTENTIAL
> POTENTIAL_TYPE PAIR_POTENTIAL
> &PAIR_POTENTIAL
> PARAMETER_FILE_NAME dftd3.dat
> TYPE DFTD3
> REFERENCE_FUNCTIONAL PBE
> &END
> &END VDW_POTENTIAL
>
> &XC_GRID
> XC_SMOOTH_RHO NN50
> XC_DERIV NN50_SMOOTH
> &END
>
> &END XC
> &END DFT
>
>
> ! description of the system
> &SUBSYS
> &CELL
> ! unit cells that are orthorhombic are more efficient with CP2K
> ABC [angstrom] 12.0944890976000003 10.4741353988999997 16.2000007629000002
> &END CELL
>
> ! atom coordinates can be in the &COORD section,
> ! or provided as an external file.
> &TOPOLOGY
> COORD_FILE_NAME MX-wt.xyz
> COORD_FILE_FORMAT XYZ
> &END
>
> ! MOLOPT basis sets are fairly costly,
> ! but in the 'DZVP-MOLOPT-SR-GTH' available for all elements
> ! their contracted nature makes them suitable
> ! for condensed and gas phase systems alike.
>
> &KIND C
> BASIS_SET DZVP-MOLOPT-SR-GTH
> POTENTIAL GTH-PBE
> &END KIND
> &KIND Ti
> BASIS_SET DZVP-MOLOPT-SR-GTH
> POTENTIAL GTH-PBE
> &END KIND
> &KIND H
> BASIS_SET DZVP-MOLOPT-SR-GTH
> POTENTIAL GTH-PBE
> &END KIND
> &KIND O
> BASIS_SET DZVP-MOLOPT-SR-GTH
> POTENTIAL GTH-PBE
> &END KIND
> &KIND Li
> BASIS_SET DZVP-MOLOPT-SR-GTH
> POTENTIAL GTH-PBE
> &END KIND
> &END SUBSYS
> &END FORCE_EVAL
>
> -----------------------
>
>
>
>
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> <eq.inp><MX-wt.xyz>
==============================
Thomas D. Kühne
Dynamics of Condensed Matter
Chair of Theoretical Chemistry
University of Paderborn
Warburger Str. 100
D-33098 Paderborn
Germany
thomas.kuehne at upb.de
+49/(0)5251/60-5726
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