[Wien] MAE calculation
Torsten Andersen
thor at physik.uni-kl.de
Thu Feb 17 13:52:27 CET 2005
Dear Wien-User,
first of all, I do not think it is a problem with Gmax. But since every
little detail can be important when you want to calculate MAE, you
should consider:
1) Did you optimize your structure?
2) Do you get the same result if you directly calculate the last of the
runsp_lapw mentioned below (and skip the two first ones)?
3) What do you get in between your "hard" and "easy" axes?
Also, I am not so sure whether you can trust results for the MAE that
are less than 1 meV.
And, of course, no method is perfect, so it could be an artefact of the
method.
You might want to try to increase R*Kmax to about 9-10. Watch the
changes in the total energy as a function of R*Kmax.
Best regards,
Torsten Andersen.
yasuharu_shiraishi at fujifilm.co.jp wrote:
> Dear wien-users,
> I calculate MAE of bilayer transition metal phase(FeNi) with s-o
> calculation. But It is strange that total energy of easy axis is higher
> than that of hard axis. So I want to ask three questions.
> First, according to User Guide, Kmax should be about 3.5 in APW+lo, so
> I use R*Kmax 8.0, but I do not know how to define Gmax. So I want to know
> how to define it. Second, I want to know how to define energy of Local
> Orbital in APW+lo of Fe and Ni which are defined as El in case.in1 file.
> Third, I want to know how to define energy El of Local Orbital correction
> for s-o interaction in case.inso file. I use same energy El in case.in1
> file which represend for energy of Local Orbital in APW+lo. Best regard.
>
> (a)My calculation parameters is as follows
>
> k = 10000
> R*Kmax = 8.0 Gmax = 14.0(default) Emax =10.0
> coordinate of Fe is (0 0 0) and Ni is (0.5 0.5 0.5) symmetry is P
> Rmt (Fe=2.3, Ni=2.3)
>
> (b)Total energy of FeNi is as follows
>
> FeNi(easy axis [0. 0. 1.]) Total energy -5577.963872
> FeNi(hard axis [1. 1. 0.]) Total energy -5577.963888
>
> (c)My case.in1 file is as follows
>
> WFFIL (WFPRI, SUPWF)
> 8.00 10 4 (R-MT*K-MAX; MAX L IN WF, V-NMT
> 0.30 5 0 (GLOBAL E-PARAMETER WITH n OTHER CHOICES, global
> APW/LAPW)
> 0 0.30 0.000 CONT 1
> 0 -6.46 0.005 STOP 1
> 1 0.30 0.000 CONT 1
> 1 -3.96 0.005 STOP 1 (I also use -3.96 for case.inso file)
> 2 0.30 0.010 CONT 1
> 0.30 5 0 (GLOBAL E-PARAMETER WITH n OTHER CHOICES, global
> APW/LAPW)
> 0 0.30 0.000 CONT 1
> 0 -7.89 0.005 STOP 1
> 1 0.30 0.000 CONT 1
> 1 -4.95 0.005 STOP 1 (I also use -4.95 for case.inso file)
> 2 0.30 0.010 CONT 1
> K-VECTORS FROM UNIT:4 -10.0 10.0 emin/emax window
>
> (d)My case.in2 file is as follows
>
> TOT (TOT,FOR,QTL,EFG,FERMI)
> -9.0 34.0 0.50 0.05 EMIN, NE, ESEPERMIN,
> ESEPER0
> TETRA 0.000 (GAUSS,ROOT,TEMP,TETRA,ALL eval)
> 0 0 2 0 4 0 4 4 6 0 6 4
> 0 0 2 0 4 0 4 4 6 0 6 4
> 14. GMAX
> FILE FILE/NOFILE write recprlist
>
> (e)My case.inso file is as follows
>
> WFFIL
> 4 1 0 llmax,ipr,kpot
> -10.0000 10.0000 emin,emax (output energy window)
> 0. 0. 1.(or (1. 1. 0.)) direction of magnetization (lattice
> vectors)
> 2 number of atoms for which RLO is added
> 1 -3.96 0.005 STOP atom number,e-lo,de (case.in1), repeat NX
> times
> 2 -4.95 0.005 STOP
> 0 0 number of atoms for which SO is switch off;
> atoms
>
> (f)My procedure of calculation is as follows
>
> init_lapw
> initso_lapw(direction of M is (0, 0, 1,) or (1, 1, 0,))
> x dstart (because symmetry changes)
> x dstart -up
> x dstart -dn
> runsp_lapw -i 512 -cc 0.000001
> save_lapw case_nrel
> runsp_lapw -so -i 512 -cc 0.000001
> save_lapw case_nrel
> runsp_lapw -so -orb -i 512 -cc 0.000001
> x lapwdm -up -so -c
>
>
>
>
>
>
>
> _______________________________________________
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> Wien at zeus.theochem.tuwien.ac.at
> http://zeus.theochem.tuwien.ac.at/mailman/listinfo/wien
>
--
Dr. Torsten Andersen TA-web: http://deep.at/myspace/
AG Hübner, Department of Physics, Kaiserslautern University
http://cmt.physik.uni-kl.de http://www.physik.uni-kl.de/
Symposium on Excited-state properties of solids, Mannheim 2005:
See: http://cmt.physik.uni-kl.de/XSM05/
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