Thanks Dr. Blaha,
One more doubt. Doping in 333SC in present work resulted
break in multiplicity of a doped site from single site (m=4) in undoped SC
to two sites (each with m=2) in doped SC. I was expecting same EFGs at two
sites (assuming same local chemical environment) as
If sgroup has given you two impurity atom sites, then their environment is
different as that is what sgroup (and other code such as nn) looks at.
Hence their EFG is different. If their environment was truly the same then
sgroup would have merged them to one, with perhaps a change in cell..
How
Hi,
In principle, mBJ can not be applied to systems with vacuum or an
interface (see section "Modified Becke-Johnson potential (mBJ) for band
gaps" in the user's guide). An alternative is to use lmBJ as you did,
but convergence was not possible. Another possibility is to use mBJ, but
by
That's perfectly ok.
You have to distinguish between a lattice (which describes the
periodicity) and a spacegroup (which includes possible point symmetry
operations like rotations,...)
If you put atoms randomly into a cubic box, the lattice is still cubic,
but the spacegroup will be P1.
Hello everyone,
I am doing SCF calculation for impurity atom (single atom)
doped 3x3x3 supercell(SC) calculation. I knw that doping of impurity atom
in SC breaks its symmetry. To know the space group of impurity atom doped
SC, x sgroup was performed and new case.struct file is
Dear ,
*) You mentioned that the first bulk MoS2 calculation worked also with hf, but
the second one not. What is the difference between them ?
No difference between them
*)Did you use the init_hf script properly ?
I think yes. I do : 1) pbe calculation + save_lapw
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