Fcc Ni (revisited): Difference between revisions
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*The example output for the spin up and down DOS shows an exchange splitting of approximately 0.5 eV: | *The example output for the spin up and down DOS shows an exchange splitting of approximately 0.5 eV: | ||
[[File:Fig fccNi revised 1.png|700px]] | [[File:Fig fccNi revised 1.png|700px]] | ||
*Proper initialization of magnetic moments is ver important: | |||
**Too small initial magnetic moments will/may lead to nonmagnetic solution (by starting with an initial moment of 0.0 we arrive only to a magnetic of 0.002). | |||
**Badly initialized calculations take longer to converge. | |||
**Coexistence of low- and high spin solutions. | |||
== Download == | == Download == |
Revision as of 10:06, 12 June 2017
Overview > fcc Ni (revisited) > NiO > NiO LSDA+U > Spin-orbit coupling in a Ni monolayer > Spin-orbit coupling in a Fe monolayer >constraining local magnetic moments > List of tutorials
Task
Calculation of the partial DOS of spin-polarized fcc Ni, a ferromagnet.
Input
POSCAR
fcc: -10.93 0.5 0.5 0.0 0.0 0.5 0.5 0.5 0.0 0.5 1 Cartesian 0 0 0
INCAR
SYSTEM = Ni fcc bulk ISTART = 0 ISPIN = 2 MAGMOM = 1.0 ISMEAR = -5 VOSKOWN = 1 LORBIT = 11
- Spin-polarized calculation with initial magnetic moment of 1 µB.
- Interpolation scheme of Vosko, Wilk and Nusair is used (see VOSKOWN=1).
- lm-decomposed DOSCAR is created.
- Tetrahedron method with Blöchl's corrections used for k-mesh integration.
KPOINTS
k-points 0 Gamma 11 11 11 0 0 0
Calculation
- The output for the magnetic moments in the OSZICAR should look like the following:
N E DAV: 1 0.139935173959E+02 0.13994E+02 -0.35801E+03 2338 0.828E+02 DAV: 2 -0.623612680591E+01 -0.20230E+02 -0.19281E+02 2282 0.123E+02 DAV: 3 -0.643764005251E+01 -0.20151E+00 -0.19906E+00 2536 0.140E+01 DAV: 4 -0.643786482872E+01 -0.22478E-03 -0.22442E-03 2344 0.459E-01 DAV: 5 -0.643786514671E+01 -0.31798E-06 -0.31687E-06 1832 0.173E-02 0.793E+00 ... DAV: 9 -0.545953126374E+01 0.48409E-02 -0.96206E-03 2946 0.839E-01 0.847E-02 DAV: 10 -0.545946513577E+01 0.66128E-04 -0.77007E-05 1364 0.126E-01 1 F= -.54594651E+01 E0= -.54594651E+01 d E =0.000000E+00 mag= 0.5781
- The l decomposed parts of the magnetic moment are written in the OUTCAR file:
magnetization (x)
# of ion s p p tot ---------------------------------------- 1 -0.007 -0.026 0.625 0.591
- The example output for the spin up and down DOS shows an exchange splitting of approximately 0.5 eV:
- Proper initialization of magnetic moments is ver important:
- Too small initial magnetic moments will/may lead to nonmagnetic solution (by starting with an initial moment of 0.0 we arrive only to a magnetic of 0.002).
- Badly initialized calculations take longer to converge.
- Coexistence of low- and high spin solutions.
Download
To the list of examples or to the main page