Equilibrium volume of Si in the RPA: Difference between revisions

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=== Step 4 ===
*Obtain DFT "virtual" orbitals (empty states).
*The following {{TAG|INCAR}} file is used in this step (INCAR.DIAG):
{{TAGBL|ALGO}} = Exact
{{TAGBL|NBANDS}} = 64
{{TAGBL|NELM}} = 1
{{TAGBL|LOPTICS}} = .TRUE.
{{TAGBL|ISMEAR}} = 0 ; {{TAGBL|SIGMA}} = 0.05
*In this step one needs to set {{TAG|LOPTICS}}=''.TRUE.'' to have VASP calculate the derivative of the orbitals w.r.t. the Bloch wavevector (stored in the {{TAG|WAVEDER}} file). These are needed to correctly describe the long-wavelength limit of the dielectric screening.
*We use exact diagonalization ({{TAG|ALGO}}=''Exact'') and keep 64 bands after diagonalization ({{TAG|NBANDS}}=64).
*This calculations needs the orbitals ({{TAG|WAVECAR}} file) written in Step 3.
----
----
== Used INCAR Tags ==
== Used INCAR Tags ==

Revision as of 10:07, 3 April 2018

Task

Calculation of the equilibrium lattice constant of Si in the RPA (ACFDT).

Input

POSCAR

system Si
  5.8
0.5 0.5 0.0
0.0 0.5 0.5
0.5 0.0 0.5
2
cart
0.00 0.00 0.00
0.25 0.25 0.25

Calculation

The workflow of RPA total energy calculations consists of five consecutive steps:

  • Step 1: a “standard” DFT groundstate calculation with a “dense” mesh of k-points.
  • Step 2: compute the Hartree-Fock energy using the orbitals of Step 1. Needs WAVECAR file from step 1.
  • Step 3: a “standard” DFT groundstate calculation with “coarse” mesh of k-points.
  • Step 4: obtain DFT “virtual” orbitals (empty states). Needs WAVECAR file from step 3.
  • Step 5: the RPA correlation energy (ACFDT) calculation. Needs WAVECAR and WAVEDER files from step 4.

In case of metallic systems there is an additional step between Steps 4 and 5, that is beyond the scope of this example.

All of the calculation steps are prepared in the script doall.sh.

Step 1

  • DFT groundstate calculation with a “dense” mesh of k-points
  • The following INCAR file is used (INCAR.DFT):
ISMEAR = 0 ; SIGMA = 0.05
EDIFF = 1E-8
  • The following KPOINTS file is used (KPOINTS.12):
12x12x12
 0
G
 12 12 12
  0  0  0

Step 2

  • Compute the Hartree-Fock energy using the DFT orbitals (WAVECAR) of Step 1.
  • The INCAR file INCAR.EXX is used in this step:
ALGO = EIGENVAL ; NELM = 1
LWAVE = .FALSE.
LHFCALC = .TRUE.
AEXX = 1.0 ; ALDAC = 0.0 ; AGGAC = 0.0
NKRED = 2
ISMEAR = 0 ; SIGMA = 0.05
KPAR = 8
NBANDS = 4
  • NKRED=2 is used for the downsample the k-space representation of the Fock-potential to save time.
  • Using NBANDS=4 only occupied states are considered to save time.

Step 3

  • DFT groundstate calculation with a “coarse” mesh of k-points.
  • The following INCAR file is used (INCAR.DFT):
ISMEAR = 0 ; SIGMA = 0.05
EDIFF = 1E-8
  • The following coarse KPOINTS file is used (KPOINTS.12):
6x6x6
 0
G
  6  6  6
  0  0  0

Step 4

  • Obtain DFT "virtual" orbitals (empty states).
  • The following INCAR file is used in this step (INCAR.DIAG):
ALGO = Exact
NBANDS = 64
NELM = 1
LOPTICS = .TRUE.
ISMEAR = 0 ; SIGMA = 0.05 
  • In this step one needs to set LOPTICS=.TRUE. to have VASP calculate the derivative of the orbitals w.r.t. the Bloch wavevector (stored in the WAVEDER file). These are needed to correctly describe the long-wavelength limit of the dielectric screening.
  • We use exact diagonalization (ALGO=Exact) and keep 64 bands after diagonalization (NBANDS=64).
  • This calculations needs the orbitals (WAVECAR file) written in Step 3.

Used INCAR Tags

AEXX, AGGAC, ALDAC, ALGO, EDIFF, ISMEAR, KPAR, LHFCALC, LOPTICS, LWAVE, NBANDS, NELM, NKRED, NOMEGA, SIGMA, SYSTEM

Download

Si_ACFDT_vol.tgz

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