[CP2K:7764] magnetization of bcc-Fe
Ralph Koitz
ralph... at gmail.com
Tue May 17 11:31:57 UTC 2016
Hi
> Is there any reference or tutorial you would like to suggest on optimize
> the basis set?
>
> Here is a talk about PP and basis set optimizations with cp2k:
https://www.cp2k.org/_media/events:2015_cecam_tutorial:ling_basis_pseudo.pdf
by S. Ling at the 2015 cp2k tutorial. Hope that helps.
Thorough testing of pseudos and basis sets is advisable before using them
in production runs.
Best,
Ralph
> Best,
>
> Yi Wang
>
> Hi
>>
>> my guess would be
>> 1) basis set
>> 2) pseudopotential
>>
>> regards
>>
>> Juerg
>> --------------------------------------------------------------
>> Juerg Hutter Phone : ++41 44 635 4491
>> Institut für Chemie C FAX : ++41 44 635 6838
>> Universität Zürich E-mail: hut... at chem.uzh.ch
>> Winterthurerstrasse 190
>> CH-8057 Zürich, Switzerland
>> ---------------------------------------------------------------
>>
>> -----cp... at googlegroups.com wrote: -----To: cp2k <cp... at googlegroups.com>
>>
>> From: wan... at gmail.com
>> Sent by: cp... at googlegroups.com
>> Date: 05/16/2016 03:33PM
>> Subject: [CP2K:7758] magnetization of bcc-Fe
>>
>> Hi everyone,
>> I'm using the new cp2k 3.0 version with its k points sampling method to
>> model the bcc-Fe.I hope the magnetization per atom can be properly modeled,
>> so that I may use it for large cells with point defect, where distribution
>> of magnetization per atom will be explored.I used the following input,
>> which produces a magnetization of 3.6 muB/atom, which is larger than
>> experiments and other simulations of around 2.2 muB/atom. (Similar in the
>> case of fcc-Ni, which is 0.63 muB/atom > 0.52 muB/atom in exp)Is it rather
>> a problem of cutoff and k points or the problem of potential and basis
>> sets?I'm quite new to cp2k, wish this question is not too naive.
>> Many thanks for any suggestion.
>>
>>
>> &GLOBAL PROJECT bcc-Fe RUN_TYPE ENERGY_FORCE PRINT_LEVEL LOW &FM
>> TYPE_OF_MATRIX_MULTIPLICATION DBCSR_MM FORCE_BLOCK_SIZE T &END FM
>> &DBCSR MM_DRIVER AUTO &END DBCSR FFTW_PLAN_TYPE MEASURE&END
>> GLOBAL&FORCE_EVAL METHOD Quickstep &SUBSYS &KIND Fe ELEMENT Fe
>> BASIS_SET DZVP-MOLOPT-SR-GTH POTENTIAL GTH-PBE-q16 &END KIND
>> &CELL A -1.43 1.43 1.43 B 1.43 -1.43 1.43 C 1.43
>> 1.43 -1.43 PERIODIC XYZ &END CELL &COORD Fe 0.000000000
>> 0.000000000 0.000000000 &END COORD &END SUBSYS &DFT
>> BASIS_SET_FILE_NAME BASIS_MOLOPT POTENTIAL_FILE_NAME GTH_POTENTIALS
>> SPIN_POLARIZED T MULTIPLICITY 3 RELAX_MULTIPLICITY 0.
>> &PRINT &HIRSHFELD ON REFERENCE_CHARGE MULLIKEN &END
>> HIRSHFELD &END PRINT &QS METHOD GPW EPS_DEFAULT 1.0E-14
>> EXTRAPOLATION USE_GUESS &END QS &MGRID NGRIDS 5 CUTOFF
>> 500 REL_CUTOFF 100 &END MGRID &XC &XC_FUNCTIONAL PBE
>> &END XC_FUNCTIONAL &END XC &SCF SCF_GUESS ATOMIC EPS_SCF
>> 2.0E-7 MAX_SCF 300 &DIAGONALIZATION ON ALGORITHM
>> STANDARD &END DIAGONALIZATION &MIXING T METHOD
>> BROYDEN_MIXING NSKIP 4 N_SIMPLE_MIX 4 ALPHA
>> 0.08 BETA 0.25 NBUFFER 12 &END MIXING ADDED_MOS 6
>> 6 CHOLESKY INVERSE_DBCSR MAX_DIIS 6 &SMEAR T METHOD
>> FERMI_DIRAC ELECTRONIC_TEMPERATURE [K] 300 &END SMEAR &END
>> SCF &KPOINTS SCHEME MONKHORST-PACK 12 12 12 FULL_GRID T
>> &END KPOINTS &END DFT &PRINT &FORCES ON &END FORCES &END PRINT&END
>> FORCE_EVAL
>>
>>
>> Yi Wang-------------------------------Yi WangPh.D student, Nanjing
>> University of Sci. & Tech.
>>
>>
>>
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--
Ralph Koitz
ralph... at gmail.com
+41 78 600 2093
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