<div dir="ltr">Dear Dr. Juerg,<div><br></div><div>Thank you very much.</div><div>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.</div><div>Is there any reference or tutorial you would like to suggest on optimize the basis set?</div><div><br></div><div>Best,</div><div><br></div><div>Yi Wang<br><br><blockquote class="gmail_quote" style="margin: 0;margin-left: 0.8ex;border-left: 1px #ccc solid;padding-left: 1ex;">Hi
<br>
<br>my guess would be
<br>1) basis set
<br>2) pseudopotential
<br>
<br>regards
<br>
<br>Juerg
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<br>Juerg Hutter <wbr> Phone : ++41 44 635 4491
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<br>Date: 05/16/2016 03:33PM
<br>Subject: [CP2K:7758] magnetization of bcc-Fe
<br>
<br>Hi everyone,
<br>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.
<br>Many thanks for any suggestion.
<br>
<br>
<br>&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
<br>
<br>
<br>Yi Wang--------------------------<wbr>-----Yi WangPh.D student, Nanjing University of Sci. & Tech.
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