NiO LSDA+U: Difference between revisions
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*The sample outpue for the on site occupancies in the {{TAG|OUTCAR}} file should look like the following (the meaning of the columns after the second equality sign is given below): | *The sample outpue for the on site occupancies in the {{TAG|OUTCAR}} file should look like the following (the meaning of the columns after the second equality sign is given below): | ||
atom = 1 type = 1 1 = 2 | atom = 1 type = 1 1 = 2 | ||
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o = 1.0248 v = -0.0032 0.0016 -1.0000 0.0016 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 | o = 1.0248 v = -0.0032 0.0016 -1.0000 0.0016 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 | ||
o = 1.0248 v = 0.0000 0.0027 0.0000 -0.0027 1.0000 0.0000 0.0000 0.0000 0.0000 0.0000 | o = 1.0248 v = 0.0000 0.0027 0.0000 -0.0027 1.0000 0.0000 0.0000 0.0000 0.0000 0.0000 | ||
<math>\qquad \qquad \qquad \qquad \qquad \qquad d_{xy}^{\uparrow} \qquad d_{yz}^{\uparrow} \qquad \quad d_{z^{2}-r^{2}}^{\uparrow} \qquad d_{xz}^{\uparrow} \qquad d_{z^{2}-y^{2}}^{\uparrow} \qquad d_{xy}^{\downarrow} \qquad \quad d_{yz}^{\downarrow} \qquad \quad d_{z^{2}-r^{2}}^{\downarrow} \qquad d_{xz}^{\downarrow} \qquad d_{z^{2}-y^{2}}^{\downarrow}</math> | |||
*Just for comparison when U=0 and J=0 (i.e. just LSDA) the on site occupancies are as follows: | |||
o = 0.3462 v = 0.0000 0.0000 0.0000 0.0000 0.0000 -0.0048 0.0028 0.9951 0.0020 -0.0986 | |||
o = 0.3462 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.0005 0.0039 -0.0986 -0.0044 -0.9951 | |||
o = 0.9491 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.5774 0.5774 0.0000 0.5774 0.0000 | |||
o = 0.9495 v = 0.0000 0.0000 0.0000 0.0000 0.0000 -0.0588 0.7347 -0.0004 -0.6759 0.0059 | |||
o = 0.9495 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.8144 -0.3563 0.0059 -0.4581 0.0004 | |||
o = 0.9527 v = 0.0477 -0.0256 0.9974 -0.0221 -0.0420 0.0000 0.0000 0.0000 0.0000 0.0000 | |||
o = 0.9527 v = 0.0020 0.0403 0.0420 -0.0423 0.9974 0.0000 0.0000 0.0000 0.0000 0.0000 | |||
o = 0.9598 v = 0.5774 0.5774 0.0000 0.5774 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 | |||
o = 0.9599 v = -0.1186 0.7577 0.0085 -0.6391 -0.0579 0.0000 0.0000 0.0000 0.0000 0.0000 | |||
o = 0.9599 v = 0.8064 -0.3005 -0.0570 -0.5059 -0.0085 0.0000 0.0000 0.0000 0.0000 0.0000 | |||
<math>\qquad \qquad \qquad \qquad \qquad \qquad d_{xy}^{\uparrow} \qquad d_{yz}^{\uparrow} \qquad \quad d_{z^{2}-r^{2}}^{\uparrow} \qquad d_{xz}^{\uparrow} \qquad d_{z^{2}-y^{2}}^{\uparrow} \qquad d_{xy}^{\downarrow} \qquad \quad d_{yz}^{\downarrow} \qquad \quad d_{z^{2}-r^{2}}^{\downarrow} \qquad d_{xz}^{\downarrow} \qquad d_{z^{2}-y^{2}}^{\downarrow}</math> | <math>\qquad \qquad \qquad \qquad \qquad \qquad d_{xy}^{\uparrow} \qquad d_{yz}^{\uparrow} \qquad \quad d_{z^{2}-r^{2}}^{\uparrow} \qquad d_{xz}^{\uparrow} \qquad d_{z^{2}-y^{2}}^{\uparrow} \qquad d_{xy}^{\downarrow} \qquad \quad d_{yz}^{\downarrow} \qquad \quad d_{z^{2}-r^{2}}^{\downarrow} \qquad d_{xz}^{\downarrow} \qquad d_{z^{2}-y^{2}}^{\downarrow}</math> | ||
Revision as of 10:25, 13 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 antiferromagnetic NiO in the LSDA+U (Dudarev's approach).
Input
POSCAR
AFM NiO 4.17 1.0 0.5 0.5 0.5 1.0 0.5 0.5 0.5 1.0 2 2 Cartesian 0.0 0.0 0.0 1.0 1.0 1.0 0.5 0.5 0.5 1.5 1.5 1.5
INCAR
SYSTEM = NiO ISTART = 0 ISPIN = 2 MAGMOM = 2.0 -2.0 2*0 ENMAX = 250.0 EDIFF = 1E-3 ISMEAR = -5 AMIX = 0.2 BMIX = 0.00001 AMIX_MAG = 0.8 BMIX_MAG = 0.00001 LORBIT = 11 LDAU = .TRUE. LDAUTYPE = 2 LDAUL = 2 -1 LDAUU = 8.00 0.00 LDAUJ = 0.95 0.00 LDAUPRINT = 2 LMAXMIX = 4 ! Important: mix paw occupancies up to L=4
- Switching on LSDA+U using Dudarev's approach (LDAUTYPE=2).
- LDAUL selects the l quantum number for which on site interaction is added (-1 = no on site interaction).
- The U and J parameters have to be specified.
- Print occupation matrices in the OUTCAR file (LDAUPRINT=2.
- L, U, and J must be specified for all atomic types!
KPOINTS
k-points 0 gamma 4 4 4 0 0 0
Calculation
- The sample outpue for the on site occupancies in the OUTCAR file should look like the following (the meaning of the columns after the second equality sign is given below):
atom = 1 type = 1 1 = 2 onsite density matrix ... ... occupancies and eigenvectors o = 0.1696 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.0013 -0.0006 -0.9999 -0.0007 -0.0104 o = 0.1696 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 -0.0011 -0.0104 0.0011 0.9999 o = 0.9770 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.7787 -0.1766 0.0015 -0.6020 0.0005 o = 0.9770 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.2456 -0.7972 0.0005 0.5516 -0.0015 o = 0.9770 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.5774 0.5774 0.0000 0.5774 0.0000 o = 0.9803 v = -0.0193 0.7166 0.0001 -0.6972 -0.0039 0.0000 0.0000 0.0000 0.0000 0.0000 o = 0.9803 v = 0.8163 -0.3914 -0.0039 -0.4249 -0.0001 0.0000 0.0000 0.0000 0.0000 0.0000 o = 0.9803 v = 0.5774 0.5774 0.0000 0.5774 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 o = 1.0248 v = -0.0032 0.0016 -1.0000 0.0016 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 o = 1.0248 v = 0.0000 0.0027 0.0000 -0.0027 1.0000 0.0000 0.0000 0.0000 0.0000 0.0000
- Just for comparison when U=0 and J=0 (i.e. just LSDA) the on site occupancies are as follows:
o = 0.3462 v = 0.0000 0.0000 0.0000 0.0000 0.0000 -0.0048 0.0028 0.9951 0.0020 -0.0986 o = 0.3462 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.0005 0.0039 -0.0986 -0.0044 -0.9951 o = 0.9491 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.5774 0.5774 0.0000 0.5774 0.0000 o = 0.9495 v = 0.0000 0.0000 0.0000 0.0000 0.0000 -0.0588 0.7347 -0.0004 -0.6759 0.0059 o = 0.9495 v = 0.0000 0.0000 0.0000 0.0000 0.0000 0.8144 -0.3563 0.0059 -0.4581 0.0004 o = 0.9527 v = 0.0477 -0.0256 0.9974 -0.0221 -0.0420 0.0000 0.0000 0.0000 0.0000 0.0000 o = 0.9527 v = 0.0020 0.0403 0.0420 -0.0423 0.9974 0.0000 0.0000 0.0000 0.0000 0.0000 o = 0.9598 v = 0.5774 0.5774 0.0000 0.5774 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 o = 0.9599 v = -0.1186 0.7577 0.0085 -0.6391 -0.0579 0.0000 0.0000 0.0000 0.0000 0.0000 o = 0.9599 v = 0.8064 -0.3005 -0.0570 -0.5059 -0.0085 0.0000 0.0000 0.0000 0.0000 0.0000
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