XANES in Diamond: Difference between revisions

From VASP Wiki
No edit summary
No edit summary
Line 2: Line 2:


== Task ==
== Task ==
Calculation of the XANES in diamond using the supercell core-hole method.
Calculation of the XANES K-edge in diamond using the supercell core-hole method.


== Input ==


=== {{FILE|POSCAR}} ===
cubic diamond
3.567
0.5 0.5 0.0
0.0 0.5 0.5
0.5 0.0 0.5
2
direct
0.0 0.0 0.0
0.25 0.25 0.25


*We will not use this structure as input but rather use it to construct a super cell from it that is actually used in the calculations.


=== {{FILE|INCAR}} ===
{{TAGBL|System}} = DIAMOND
{{TAGBL|ALGO}} = FAST
{{TAGBL|ISMEAR}} = 0; {{TAGBL|SIGMA}} = 0.1;
{{TAGBL|ICORELEVEL}} = 2
{{TAGBL|CLNT}} = 1
{{TAGBL|CLN}} = 1
{{TAGBL|CLL}} = 0
{{TAGBL|CLZ}} = 1.0
{{TAGBL|CH_LSPEC}} = .TRUE.
{{TAGBL|CH_SIGMA}} = 0.5
{{TAGBL|NBANDS}} = 300
{{TAGBL|LREAL}} = A
*To promote a core electron into the conduction bands and hence create the core-hole {{TAG|ICORELEVEL}}=2 has to be set. This corresponds to the final state approximation
*{{TAG|CLNT}}=1 selects the first atom species in the {{TAG|POSCAR}} file.
*{{TAG|CLN}}=1 selects main quantum number 1 (hence K-edge).
*{{TAG|CLL}}=0 selects angular quantum number 0 (s).
*{{TAG|CLZ}}=1.0 selects the charge of the core hole. By setting this number to a fractional value we can mimick different screening of the electrons. Since this purely exploits error cancellation and the physical background of non-integer charges is not defined well, it should be only used with caution.
*By setting {{TAG|CH_LSPEC}}=''.TRUE.'' we enable the calculation of matrix elements between core and conduction states and the calculation of the core electron absorption spectrum.
*The broadening of the core electron absorption spectrum is controlled by the tag {{TAG|CH_SIGMA}}. Usually it is good practice to set this value low and broaden the spectrum in post processing.
*We have to set {{TAG|NBANDS}} to a larger value to consider enough conduction band states in the calculation.
*Since super cells are used the calculation of the projection operators in real space is much faster, hence {{TAG|LREAL}}=''A'' is set.
== Download ==
== Download ==



Revision as of 15:21, 12 April 2018

Task

Calculation of the XANES K-edge in diamond using the supercell core-hole method.

Input

POSCAR

cubic diamond

3.567
0.5 0.5 0.0
0.0 0.5 0.5
0.5 0.0 0.5
2

direct

0.0 0.0 0.0
0.25 0.25 0.25
  • We will not use this structure as input but rather use it to construct a super cell from it that is actually used in the calculations.

INCAR

System = DIAMOND
ALGO = FAST
ISMEAR = 0; SIGMA = 0.1;
ICORELEVEL = 2
CLNT = 1
CLN = 1
CLL = 0
CLZ = 1.0
CH_LSPEC = .TRUE.
CH_SIGMA = 0.5
NBANDS = 300
LREAL = A
  • To promote a core electron into the conduction bands and hence create the core-hole ICORELEVEL=2 has to be set. This corresponds to the final state approximation
  • CLNT=1 selects the first atom species in the POSCAR file.
  • CLN=1 selects main quantum number 1 (hence K-edge).
  • CLL=0 selects angular quantum number 0 (s).
  • CLZ=1.0 selects the charge of the core hole. By setting this number to a fractional value we can mimick different screening of the electrons. Since this purely exploits error cancellation and the physical background of non-integer charges is not defined well, it should be only used with caution.
  • By setting CH_LSPEC=.TRUE. we enable the calculation of matrix elements between core and conduction states and the calculation of the core electron absorption spectrum.
  • The broadening of the core electron absorption spectrum is controlled by the tag CH_SIGMA. Usually it is good practice to set this value low and broaden the spectrum in post processing.
  • We have to set NBANDS to a larger value to consider enough conduction band states in the calculation.
  • Since super cells are used the calculation of the projection operators in real space is much faster, hence LREAL=A is set.

Download

Back to the main page.