I have two silicon in an unit cell, for a test calculation. Each silicon as 12 electrons in the pseudopotential (1s is frozen). I have done the partial density of states (PDOS) calculation using DFT with QUANTUM ESPRESSO. What I need to know is, I have been suggested to do the following two tasks (which instructs like):
- Take your PDOS summed over the different atomic orbitals (2s, 2p, 3s, 3p, 3d), and summed over energies up to the Fermi level (i.e. all the occupied states)
- Then subtract this from the total number of electrons in the unit cell. It will find the number of electrons that are not in those atomic orbitals (this is the ultimate goal of the task).
Could you please suggest me how to solve these two to get the number of electrons that are not in those atomic orbitals (any process or modification of input files or steps or resource links would be greatly appreciated)?
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Note (optional, in case it gives more insight): I got the Fermi energy value as 21.653 eV from the DOS calculation. My DOS input code:
&DOS
prefix='silicon'
outdir='.',
DeltaE=0.2,
Emin=-119.233,
Emax=109.567,
fildos='si.dos',
/
And my PDOS input was
&projwfc
prefix='silicon'
outdir='./'
degauss=0.2
DeltaE=0.2
filpdos='si.pdos.dat'
/
From DOS calculation, the output data obtained is like this (shown portion to get idea):
# E (eV) dos(E) Int dos(E) EFermi = 21.653 eV
-119.233 0.1148E-84 0.2295E-85
-119.033 0.1148E-84 0.4591E-85
-118.833 0.1148E-84 0.6886E-85
And from the PDOS calculation, the output data files from one atom are (shown portions to get ideas):
For 2s:
# E (eV) ldos(E) pdos(E)
-119.233 0.379E-04 0.379E-04
-119.033 0.589E-04 0.589E-04
-118.833 0.907E-04 0.907E-04
For 2p:
# E (eV) ldos(E) pdos(E) pdos(E) pdos(E)
-119.233 0.174E-08 0.580E-09 0.580E-09 0.580E-09
-119.033 0.271E-08 0.902E-09 0.902E-09 0.902E-09
-118.833 0.416E-08 0.139E-08 0.139E-08 0.139E-08
For 3s:
# E (eV) ldos(E) pdos(E)
-119.233 0.327E-06 0.327E-06
-119.033 0.511E-06 0.511E-06
-118.833 0.788E-06 0.788E-06
and for 3p:
# E (eV) ldos(E) pdos(E) pdos(E) pdos(E)
-119.233 0.149E-05 0.498E-06 0.498E-06 0.498E-06
-119.033 0.232E-05 0.773E-06 0.773E-06 0.773E-06
-118.833 0.356E-05 0.119E-05 0.119E-05 0.119E-05