O atom spinpolarized: Difference between revisions
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| {{Template:At_and_mol - Tutorial}} | |||
| == Task == | |||
| Performing a spin polarized calculation for a single oxygen atom in a cubic box to get the correct magnetic moment of the atom. | |||
| == Input == | |||
| === {{FILE|POSCAR}} === | |||
|   O atom in a box |   O atom in a box | ||
|    1.0          ! universal scaling parameters |    1.0          ! universal scaling parameters | ||
| Line 21: | Line 17: | ||
|    0 0 0 |    0 0 0 | ||
| === {{FILE|INCAR}} === | |||
|  {{TAGBL|SYSTEM}} = O atom in a box | |||
|  {{TAGBL|ISMEAR}} = 0  ! Gaussian smearing | |||
|  {{TAGBL|ISPIN}} =  2  ! spin polarized calculation | |||
| === {{FILE|KPOINTS}} === | |||
|  Gamma-point only | |||
|   0 | |||
|  Monkhorst Pack | |||
|   1 1 1 | |||
|   0 0 0 | |||
| == Calculation == | |||
| *The O atom is an open shell system with 2 unpaired electrons. | |||
| *Starting from the previous chapter add {{TAG|ISPIN}}=2 to the {{TAG|INCAR}} file remove the {{TAG|WAVECAR}} file and restart VASP. | |||
| *The following example output is obtained (stdout): | |||
|  running on    8 total cores | |||
|  distrk:  each k-point on    8 cores,    1 groups | |||
|  distr:  one band on    1 cores,    8 groups | |||
|  using from now: INCAR      | |||
|  vasp.5.4.1 05Feb16 (build Aug 22 2016 16:46:23) complex                         | |||
|  POSCAR found :  1 types and       1 ions | |||
|  scaLAPACK will be used | |||
|  LDA part: xc-table for Pade appr. of Perdew | |||
|  POSCAR, INCAR and KPOINTS ok, starting setup | |||
|  WARNING: small aliasing (wrap around) errors must be expected | |||
|  FFT: planning ... | |||
|  WAVECAR not read | |||
|  entering main loop | |||
|  N       E                     dE             d eps       ncg     rms          rms(c) | |||
|  DAV:   1     0.389725012498E+02    0.38973E+02   -0.10098E+03    32   0.259E+02 | |||
|  DAV:   2     0.317912429240E+01   -0.35793E+02   -0.35786E+02    64   0.438E+01 | |||
|  DAV:   3    -0.119085682530E+01   -0.43700E+01   -0.36686E+01    32   0.328E+01 | |||
|  DAV:   4    -0.126198272139E+01   -0.71126E-01   -0.69189E-01    32   0.508E+00 | |||
|  DAV:   5    -0.126284205021E+01   -0.85933E-03   -0.85925E-03    48   0.504E-01    0.653E+00 | |||
|  DAV:   6     0.164008071667E+00    0.14269E+01   -0.32208E+00    32   0.894E+00    0.151E+00 | |||
|  ...    ...      ...                  | |||
|  DAV:  13    -0.167302579657E+01   -0.25698E-03   -0.13177E-05    32   0.203E-02    0.956E-03 | |||
|  DAV:  14    -0.167302926747E+01   -0.34709E-05   -0.34771E-06    32   0.116E-02 | |||
|  1 F= -.16730293E+01 E0= -.15958981E+01  d E =-.154262E+00  mag=     1.9999 | |||
|  writing wavefunctions | |||
|  E-fermi : -7.1152 XC(G=0): -0.7730 alpha+bet : -0.1463 | |||
| *Eigenstates for spin up and spin down are calculated "separately". In LSDA they interact only via the effective local potential spin-up and spin-down potential.  | |||
| *In the {{TAG|OUTCAR}} file one can see two spin components: | |||
|  spin component 1 | |||
|  k-point     1 :       0.0000    0.0000    0.0000 | |||
|   band No.  band energies     occupation | |||
|       1     -25.0878      1.00000 | |||
|       2     -10.0830      1.00000 | |||
|       3     -10.0830      1.00000 | |||
|       4     -10.0830      1.00000 | |||
|       5      -0.4932      0.00000 | |||
|       6       1.8213      0.00000 | |||
|       7       1.8303      0.00000 | |||
|       8       1.8303      0.00000 | |||
|  spin component 2 | |||
|  k-point     1 :       0.0000    0.0000    0.0000 | |||
|   band No.  band energies     occupation | |||
|       1     -21.8396      1.00000 | |||
|       2      -7.0543      0.33333 | |||
|       3      -7.0543      0.33333 | |||
|       4      -7.0543      0.33333 | |||
|       5      -0.3594      0.00000 | |||
|       6       1.9830      0.00000 | |||
|       7       1.9830      0.00000 | |||
|       8       1.9830      0.00000 | |||
| The spin component 1 has two more electrons corresponding to a magnetization of <math> 2\mu_{B} </math>. | |||
| == Download == | == Download == | ||
| [ | [[Media:Oatomspin.tgz|Oatomspin.tgz]] | ||
| {{Template:At_and_mol}} | |||
| [[Category:Examples]] | [[Category:Examples]] | ||
Latest revision as of 14:16, 14 November 2019
Overview > O atom > O atom spinpolarized > O atom spinpolarized low symmetry > O dimer > CO > CO vibration >  CO partial DOS > H2O >
 H2O vibration > H2O molecular dynamics > Further things to try  > List of tutorials
Task
Performing a spin polarized calculation for a single oxygen atom in a cubic box to get the correct magnetic moment of the atom.
Input
POSCAR
O atom in a box 1.0 ! universal scaling parameters 8.0 0.0 0.0 ! lattice vector a(1) 0.0 8.0 0.0 ! lattice vector a(2) 0.0 0.0 8.0 ! lattice vector a(3) 1 ! number of atoms cart ! positions in cartesian coordinates 0 0 0
INCAR
SYSTEM = O atom in a box ISMEAR = 0 ! Gaussian smearing ISPIN = 2 ! spin polarized calculation
KPOINTS
Gamma-point only 0 Monkhorst Pack 1 1 1 0 0 0
Calculation
- The O atom is an open shell system with 2 unpaired electrons.
- Starting from the previous chapter add ISPIN=2 to the INCAR file remove the WAVECAR file and restart VASP.
- The following example output is obtained (stdout):
running on 8 total cores distrk: each k-point on 8 cores, 1 groups distr: one band on 1 cores, 8 groups using from now: INCAR vasp.5.4.1 05Feb16 (build Aug 22 2016 16:46:23) complex POSCAR found : 1 types and 1 ions scaLAPACK will be used LDA part: xc-table for Pade appr. of Perdew POSCAR, INCAR and KPOINTS ok, starting setup WARNING: small aliasing (wrap around) errors must be expected FFT: planning ... WAVECAR not read entering main loop N E dE d eps ncg rms rms(c) DAV: 1 0.389725012498E+02 0.38973E+02 -0.10098E+03 32 0.259E+02 DAV: 2 0.317912429240E+01 -0.35793E+02 -0.35786E+02 64 0.438E+01 DAV: 3 -0.119085682530E+01 -0.43700E+01 -0.36686E+01 32 0.328E+01 DAV: 4 -0.126198272139E+01 -0.71126E-01 -0.69189E-01 32 0.508E+00 DAV: 5 -0.126284205021E+01 -0.85933E-03 -0.85925E-03 48 0.504E-01 0.653E+00 DAV: 6 0.164008071667E+00 0.14269E+01 -0.32208E+00 32 0.894E+00 0.151E+00 ... ... ... DAV: 13 -0.167302579657E+01 -0.25698E-03 -0.13177E-05 32 0.203E-02 0.956E-03 DAV: 14 -0.167302926747E+01 -0.34709E-05 -0.34771E-06 32 0.116E-02 1 F= -.16730293E+01 E0= -.15958981E+01 d E =-.154262E+00 mag= 1.9999 writing wavefunctions E-fermi : -7.1152 XC(G=0): -0.7730 alpha+bet : -0.1463
- Eigenstates for spin up and spin down are calculated "separately". In LSDA they interact only via the effective local potential spin-up and spin-down potential.
- In the OUTCAR file one can see two spin components:
spin component 1
  
k-point     1 :       0.0000    0.0000    0.0000
 band No.  band energies     occupation
     1     -25.0878      1.00000
     2     -10.0830      1.00000
     3     -10.0830      1.00000
     4     -10.0830      1.00000
     5      -0.4932      0.00000
     6       1.8213      0.00000
     7       1.8303      0.00000
     8       1.8303      0.00000
spin component 2
  
k-point     1 :       0.0000    0.0000    0.0000
 band No.  band energies     occupation
     1     -21.8396      1.00000
     2      -7.0543      0.33333
     3      -7.0543      0.33333
     4      -7.0543      0.33333
     5      -0.3594      0.00000
     6       1.9830      0.00000
     7       1.9830      0.00000
     8       1.9830      0.00000
The spin component 1 has two more electrons corresponding to a magnetization of [math]\displaystyle{ 2\mu_{B} }[/math].
