Hi,

Fermi energy is not really defined in an insulator/semiconductor; at 0 temperature any value in the gap a is good fermi energy, but better to talk about the chemical potential. At temperature is raised, it would be approximately start in the middle of the gap, and move away from that depending on how the conduction and valence DOS are. Maybe read the Ashcroft Mermin chapter on homogeneous semiconductors (27, I think).

A typical good choice for smearing (0.02 Ry, 0.15 A^-1 density of k-points) would give you the fermi energy in the middle of the gap, approximately, if you use gaussian smearing in an insulator. mv and mp should not be used for an insulator/semiconductor.

Also, mv has positive occupations, so something seems wrong with your plot - are you sure you are not using mp?

                        nicola

On 27/06/2020 14:56, 후신 부지드 wrote:
Dear QE users,


I tried to search a solution for this problem and looked to the previous posts but didn't work with me



I made scf calculation for bulk SnS2 with dft-d3 using occupations= 'tetrahedra' I get the the fermi level Ef on top of the valence band as reported in the literature,

but when I try to use smearing the Ef will shifts about 1 eV to locate in the middle of the gap

I tried gaussian smearing and fd using a huge k points, but eventhough the energy converges to the value in tertahedra case, the Ef always shifts by ~ 1eV.

The only exception is mv smearing with 0.01 degauss it gives the right Ef, (but it has a tail with finite dos which is not seen in the gaussian case with wrong Ef, pls see the attached image) and when I try mv with 0.005 degauss it also show wrong Ef even with huge k points.


Does anyone know why I'm getting this shift in Ef even though the energy is converged and the kpoint is large enough


Here is the input file for tetrahedra and smearing:



Tetrahedra:


&control
     calculation = 'scf'
     restart_mode='from_scratch'
     prefix = 'tet'
     outdir = '/home/outdir'
     pseudo_dir = '/home/pseudo'
     verbosity = 'high'
/

&system

     ibrav = 0,
     nat   = 6,
     ntyp  = 2,
     ecutwfc=80
     ecutrho=560
     vdw_corr = 'dft-d3'
     occupations='tetrahedra'
     nbnd=52
     lda_plus_u=.true.
     Hubbard_U(1)=9.0,
     Hubbard_U(2)=9.0,

/

&electrons
     conv_thr=1e-6
/

ATOMIC_SPECIES
  Sn    118.71000  Sn.pbe-dn-kjpaw_psl.1.0.0.UPF
  S      32.06600  S.pbe-n-kjpaw_psl.1.0.0.UPF

ATOMIC_POSITIONS (angstrom)

Sn      -0.000001900   2.129228760   7.368473930
Sn       1.843967305   1.064612836   1.474204489
S        1.843967305   1.064612836   8.846101191
S       -0.000001900   2.129228760   2.951831855
S       -0.000000000  -0.000000000  -0.005322640
S       -0.000000000   0.000000000   5.888946695

CELL_PARAMETERS (angstrom)

  3.687930810   0.000000000  -0.000000000
-1.843965405   3.193841769  -0.000000000
-0.000000000  -0.000000000  11.788538670
K_POINTS (automatic)
  20 20 6 0 0 0



Smearing



&control
     calculation = 'scf'
     restart_mode='from_scratch'
     prefix = 'smea'
     outdir = '/home/outdir'
     pseudo_dir = '/home/pseudo'
     verbosity = 'high'
/

&system

     ibrav = 0,
     nat   = 6,
     ntyp  = 2,
     ecutwfc=80
     ecutrho=560
     vdw_corr = 'dft-d3'
     occupations='smearing',smearing='gaussian',degauss=0.01
     lda_plus_u=.true.
     Hubbard_U(1)=9.0,
     Hubbard_U(2)=9.0,
/

&electrons
     conv_thr=1e-6
/

ATOMIC_SPECIES
  Sn    118.71000  Sn.pbe-dn-kjpaw_psl.1.0.0.UPF
  S      32.06600  S.pbe-n-kjpaw_psl.1.0.0.UPF

ATOMIC_POSITIONS (angstrom)

Sn      -0.000001900   2.129228760   7.368473930
Sn       1.843967305   1.064612836   1.474204489
S        1.843967305   1.064612836   8.846101191
S       -0.000001900   2.129228760   2.951831855
S       -0.000000000  -0.000000000  -0.005322640
S       -0.000000000   0.000000000   5.888946695

CELL_PARAMETERS (angstrom)

  3.687930810   0.000000000  -0.000000000
-1.843965405   3.193841769  -0.000000000
-0.000000000  -0.000000000  11.788538670
K_POINTS (automatic)
  32 32 10 0 0 0


Houcine BOUZID
Sungkyunkwan University,


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--
----------------------------------------------------------------------
Prof Nicola Marzari, Chair of Theory and Simulation of Materials, EPFL
Director, National Centre for Competence in Research NCCR MARVEL, EPFL
http://theossrv1.epfl.ch/Main/Contact http://nccr-marvel.ch/en/project
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