[Wien] mixed occupancy
Rocquefelte
Xavier.Rocquefelte at cnrs-imn.fr
Thu Mar 13 13:35:35 CET 2008
Dear Julia,
As all DFT code Wien2k can only work on a clearly defined atomic
structure in the 3D space. As a consequence, each crystallographic sites
are fully occupied.
When a partial occupancy is observed experimentally, one solution
consists to create a supercell (which will be lower in symmetry) that
will allow the distribution of Cu1 and Sn1 on this site.
By such an approach you will create an atomic order and for this reason
it is usually necessary to consider different models in order to check
that the order does not perturb the property you are looking for.
Another approach "the virtual crystal approximation" consists to mix two
atoms in one in a given proportion. Then you don't need to create a
supercell and you have an effective treatment of the partial occupancy.
However, I don't think that such an approach will be valid in the
present case, because of the strong difference between Cu and Sn atoms.
Regards
Xavier
Julia Messel a écrit :
> Dear wien users,
>
> is it possible to consider for s.o.f.'s < 1 and mixed occupancy in struct
> file? I create a struct-file out of a cif-file, which contains the position
> x=0.32445 y=0.25 z=0.49864 shared by 0.728 Cu1 and 0.272 Sn1, but wien2k does
> not accept this.
>
> Thanking you in anticipation,
>
> Julia
>
>
> SOF
> Cu1 Cu Uani 0.32445(10) 0.25 0.49864(12) 0.0156(4) 4 0.728(12)
> Sn1 Sn Uani 0.3245 0.25 0.4986 0.0156(4) 4 0.272(12)
> Sn2 Sn Uani 0.67730(12) 0.21643(12) 0.40562(14) 0.0370(6) 8 0.5
> P1 P Uani 0.1799(3) 0.25 0.3511(3) 0.0199(10) 4 1
> P2 P Uani 0.4699(3) 0.25 0.3449(3) 0.0168(10) 4 1
> P3 P Uani 0.07948(16) 0.0796(2) 0.4183(2) 0.0148(6) 8 1
> P4 P Uani 0.43279(16) 0.0835(2) 0.2108(2) 0.0142(7) 8 1
> P5 P Uani 0.31577(17) 0.0781(2) 0.8318(2) 0.0160(6) 8 1
> P6 P Uani 0.35655(16) 0.0532(2) 0.6295(2) 0.0202(7) 8 1
> P7 P Uani 0.03056(16) 0.0780(2) 0.8522(2) 0.0144(6) 8 1
> P8 P Uani 0.4126(2) 0.25 0.9038(3) 0.0145(10) 4 1
> P9 P Uani 0.0583(2) 0.25 0.7201(3) 0.0150(10) 4 1
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