It is NOT necessary to use your own case.cf file.

There are standard options for case.inq to obtain the j1/2-3/2
Use QSPLIT=0 (or -1).

On 11/20/2013 04:57 AM, acta3...@chiba-u.jp wrote:
Dear WIEN2k users,

I am intersted in materials with strong spin-orbit coupling and now
trying
to calculate the electronic structure of Sr2IrO4 without spin
polarization.

Using wien2k but without using wannier, I want to reproduce the PDOS
projected onto Jeff=1/2 and 3/2, as was done in Fig.5.15 on page 87 of
Ref: http://hal.archives-ouvertes.fr/docs/00/59/10/68/PDF/MainThese.pdf

The mailing-list suggests the use of case.cf, so I am using the files
case.struct, case.inso, case.cf, and case.inq attached below.
Using these files, I have done the following:

1. x qtl -so
2. emacs Sr2IrO4_I4mmm_undistorted.qtl
    line 6 is changed from
    JATOM  2  MULT= 1  ISPLIT= 6   projected DOS, user own unitary
transformation
    to
    JATOM  2  MULT= 1  ISPLIT= 6   tot,d,j3/2p3/2,j3/2m3/2,j3/2p1/2,j3/
2m1/2,j1/2p1/2,j1/2m1/2,z2up,z2dn,x2y2up,x2y2dn,
3. x tetra

However, the results did not agree with those of the above Reference.
For example, no denegeracy in PDOS occurs between |Jeff=3/2,Jz=-3/2> and
|Jeff=3/2,Jz=+3/2>.

The states of Jeff=3/2 and 1/2 are written as
|Jeff=3/2,Jz=-3/2>=(|dyz,dn>-i|dxz,dn>)/sqrt(2)
|Jeff=3/2,Jz=+3/2>=(-|dyz,dn>-i|dxz,dn>)/sqrt(2)
|Jeff=3/2,Jz=-1/2>=(|dyz,up>-i|dxz,up>+2|dxy,dn>)/sqrt(6)
|Jeff=3/2,Jz=+1/2>=(-|dyz,dn>-i|dxz,dn>+2|dxy,up>)/sqrt(6)
|Jeff=1/2,Jz=-1/2>=(|dyz,up>-i|dxz,up>-|dxy,dn>)/sqrt(3)
|Jeff=1/2,Jz=+1/2>=(|dyz,dn>+i|dxz,dn>+|dxy,up>)/sqrt(3)

I am wondering what is wrong....

I am using version 13.1 of wien2k, and OS is ubuntu12.04LTS.

Thanks for your help.

--
Tatsuya Toriyama
Dept. of Phys.,
Japan, Chiba-univ.


------Sr2IrO4_I4mmm_undistorted.struct-----------------------
Sr2IrO4_I4mmm_undistorted
B   LATTICE,NONEQUIV.ATOMS:  4139_I4/mmm
MODE OF CALC=RELA unit=bohr
   7.314185  7.314185 24.063584 90.000000 90.000000 90.000000
ATOM  -1: X=0.00000000 Y=0.00000000 Z=0.35308382
           MULT= 2          ISPLIT=-2
       -1: X=0.00000000 Y=0.00000000 Z=0.64691618
Sr         NPT=  781  R0=0.00001000 RMT=    2.2700   Z: 38.0
LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000
                      0.0000000 1.0000000 0.0000000
                      0.0000000 0.0000000 1.0000000
ATOM  -2: X=0.00000000 Y=0.00000000 Z=0.00000000
           MULT= 1          ISPLIT=-2
Ir         NPT=  781  R0=0.00000500 RMT=    2.0000   Z: 77.0
LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000
                      0.0000000 1.0000000 0.0000000
                      0.0000000 0.0000000 1.0000000
ATOM  -3: X=0.00000000 Y=0.50000000 Z=0.00000000
           MULT= 2          ISPLIT= 8
       -3: X=0.50000000 Y=0.00000000 Z=0.00000000
O          NPT=  781  R0=0.00010000 RMT=    1.6400   Z:  8.0
LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000
                      0.0000000 1.0000000 0.0000000
                      0.0000000 0.0000000 1.0000000
ATOM  -4: X=0.00000000 Y=0.00000000 Z=0.16316250
           MULT= 2          ISPLIT=-2
       -4: X=0.00000000 Y=0.00000000 Z=0.83683750
O          NPT=  781  R0=0.00010000 RMT=    1.6400   Z:  8.0
LOCAL ROT MATRIX:    1.0000000 0.0000000 0.0000000
                      0.0000000 1.0000000 0.0000000
                      0.0000000 0.0000000 1.0000000
   16      NUMBER OF SYMMETRY OPERATIONS
  1 0 0 0.00000000
  0-1 0 0.00000000
  0 0-1 0.00000000
        1
  0-1 0 0.00000000
  1 0 0 0.00000000
  0 0-1 0.00000000
        2
-1 0 0 0.00000000
  0-1 0 0.00000000
  0 0-1 0.00000000
        3
  0 1 0 0.00000000
  1 0 0 0.00000000
  0 0-1 0.00000000
        4
  0-1 0 0.00000000
-1 0 0 0.00000000
  0 0-1 0.00000000
        5
  1 0 0 0.00000000
  0 1 0 0.00000000
  0 0-1 0.00000000
        6
  1 0 0 0.00000000
  0-1 0 0.00000000
  0 0 1 0.00000000
        7
  0-1 0 0.00000000
  1 0 0 0.00000000
  0 0 1 0.00000000
        8
  0 1 0 0.00000000
-1 0 0 0.00000000
  0 0-1 0.00000000
        9
-1 0 0 0.00000000
  0 1 0 0.00000000
  0 0-1 0.00000000
       10
-1 0 0 0.00000000
  0-1 0 0.00000000
  0 0 1 0.00000000
       11
  0 1 0 0.00000000
  1 0 0 0.00000000
  0 0 1 0.00000000
       12
  0-1 0 0.00000000
-1 0 0 0.00000000
  0 0 1 0.00000000
       13
  1 0 0 0.00000000
  0 1 0 0.00000000
  0 0 1 0.00000000
       14
  0 1 0 0.00000000
-1 0 0 0.00000000
  0 0 1 0.00000000
       15
-1 0 0 0.00000000
  0 1 0 0.00000000
  0 0 1 0.00000000
       16
------Sr2IrO4_I4mmm_undistorted.inso-------------------------
WFFIL
  4  1  0                      llmax,ipr,kpot
  -10.0000   1.50000           emin,emax (output energy window)
    0.  0.  1.                 direction of magnetization (lattice
vectors)
  0                            number of atoms for which RLO is added
  0                            number of atoms for which SO is switch off;
  atoms
------Sr2IrO4_I4mmm_undistorted.cf2--------------------------
  0.00000  0.00000  0.00000 0.00000  0. 0.  1. 0.  0.00000  0.00000  0.
00000  0.00000  0. 0.  0. 0.  0.00000 0.00000  0.00000 0.00000 j3/2jz+3/
2
  0.00000  0.00000  0.00000 0.00000  0. 0.  0. 0.  0.00000  0.00000  0.
00000  0.00000  1. 0.  0. 0.  0.00000 0.00000  0.00000 0.00000 j3/2jz-3/
2
  0.00000 -0.57735  0.00000 0.00000  0. 0.  0. 0.  0.00000  0.57735  0.
00000  0.00000  0. 0.  0. 0.  0.57735 0.00000  0.00000 0.00000 j3/2jz+1/
2
  0.00000  0.00000  0.57735 0.00000  0. 0.  0. 0.  0.00000  0.00000  0.
00000 -0.57735  0. 0.  0. 0.  0.00000 0.00000  0.00000 0.57735 j3/2jz-1/
2
  0.00000  0.40825  0.00000 0.00000  0. 0.  0. 0.  0.00000 -0.40825  0.
00000  0.00000  0. 0.  0. 0.  0.81650 0.00000  0.00000 0.00000 j1/2jz+1/
2
  0.00000  0.00000 -0.81650 0.00000  0. 0.  0. 0.  0.00000  0.00000  0.
00000 -0.40825  0. 0.  0. 0.  0.00000 0.00000  0.00000 0.40825 j1/2jz-1/
2
  0.00000  0.00000  0.00000 0.00000  1. 0.  0. 0.  0.00000  0.00000  0.
00000  0.00000  0. 0.  0. 0.  0.00000 0.00000  0.00000 0.00000 z2u
  0.00000  0.00000  0.00000 0.00000  0. 0.  0. 0.  0.00000  0.00000  0.
00000  0.00000  0. 0.  1. 0.  0.00000 0.00000  0.00000 0.00000 z2d
  0.70711  0.00000  0.00000 0.00000  0. 0.  0. 0.  0.70711  0.00000  0.
00000  0.00000  0. 0.  0. 0.  0.00000 0.00000  0.00000 0.00000 x2y2u
  0.00000  0.00000  0.00000 0.00000  0. 0.  0. 0.  0.00000  0.00000  0.
70711  0.00000  0. 0.  0. 0.  0.00000 0.00000  0.70711 0.00000 x2y2d
------Sr2IrO4_I4mmm_undistorted.inq---------------------------
-9.0   3.0           Emin  Emax
    4                 number of atoms
    1  -2  0  0       iatom,qsplit,symmetrize,locrot
3   0  1  2          nL, l-values
    2   6  0  0       iatom,qsplit,symmetrize,locrot
1   2                nL, l-values
    3  -2  0  0       iatom,qsplit,symmetrize,locrot
2   0  1             nL, l-values
    4  -2  0  0       iatom,qsplit,symmetrize,locrot
2   0  1             nL, l-values
--------------------------------------------------------------



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--

                                      P.Blaha
--------------------------------------------------------------------------
Peter BLAHA, Inst.f. Materials Chemistry, TU Vienna, A-1060 Vienna
Phone: +43-1-58801-165300             FAX: +43-1-58801-165982
Email: bl...@theochem.tuwien.ac.at WWW: http://info.tuwien.ac.at/theochem/
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