[CP2K:7764] magnetization of bcc-Fe
hut... at chem.uzh.ch
hut... at chem.uzh.ch
Tue May 17 11:36:28 UTC 2016
Hi
regarding the delta test: if you check the Abinit HGHk values
you find for Fe a value of 5.15 meV/atom.
regards
Juerg
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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
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-----cp... at googlegroups.com wrote: -----To: cp2k <cp... at googlegroups.com>
From: wang... at gmail.com
Sent by: cp... at googlegroups.com
Date: 05/17/2016 01:19PM
Subject: Re: [CP2K:7764] magnetization of bcc-Fe
Dear Dr. Juerg,
Thank you very much.The potential seems has been used by the BigDFT team for the delta parameter calculation on deltacodesdft website, with a small error of 2.7 meV/atom compared with Wien2k. According to the results of deltacodesdft, the potential may perform same well in different codes. So I guess maybe the basis is not suitable for bcc-Fe.Is there any reference or tutorial you would like to suggest on optimize the basis set?
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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