Equilibrium volume of Si in the RPA: Difference between revisions

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


=== Step 1 ===
=== Step 1: DFT groundstate calculation with a “dense” mesh of k-points ===
*DFT groundstate calculation with a “dense” mesh of k-points
 
*The following {{TAG|INCAR}} file is used (INCAR.DFT):
*The following {{TAG|INCAR}} file is used (INCAR.DFT):
  {{TAGBL|ISMEAR}} = 0 ; {{TAGBL|SIGMA}} = 0.05
  {{TAGBL|ISMEAR}} = 0 ; {{TAGBL|SIGMA}} = 0.05
  {{TAGBL|EDIFF}} = 1E-8
  {{TAGBL|EDIFF}} = 1E-8
*The following {{TAG|KPOINTS}} file is used (KPOINTS.12):
*The following {{TAG|KPOINTS}} file is used (KPOINTS.12):
  12x12x12
  12x12x12
Line 44: Line 45:
   0  0  0
   0  0  0


=== Step 2 ===
=== Step 2: Compute the Hartree-Fock energy using the DFT orbitals===
*Compute the Hartree-Fock energy using the DFT orbitals ({{TAG|WAVECAR}}) of Step 1.
 
*To Compute the Hartree-Fock energy using the DFT orbitals we need the ({{TAG|WAVECAR}}) of Step 1.
 
*The {{TAG|INCAR}} file INCAR.EXX is used in this step:
*The {{TAG|INCAR}} file INCAR.EXX is used in this step:
  {{TAGBL|ALGO}} = EIGENVAL ; {{TAGBL|NELM}} = 1
  {{TAGBL|ALGO}} = EIGENVAL ; {{TAGBL|NELM}} = 1

Revision as of 16:33, 24 June 2019

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

  • To Compute the Hartree-Fock energy using the DFT orbitals we need the (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.

Step 5

  • The RPA correlation energy (ACFDT) calculation.
  • The following INCAR file is used in this step (INCAR.ACFDT):
ALGO = ACFDT
NBANDS = 64
ISMEAR = 0 ; SIGMA = 0.05
  • In OUTCAR.ACFDT.X.X one finds the RPA correlation energy, e.g.:
       cutoff energy      smooth cutoff    RPA   correlation   Hartree contr. to MP2
---------------------------------------------------------------------------------
            163.563            130.851       -10.7869840331      -19.0268026572
            155.775            124.620       -10.7813600055      -19.0200457142
            148.357            118.685       -10.7744584182      -19.0118291822
            141.292            113.034       -10.7659931963      -19.0017871991
            134.564            107.651       -10.7555712745      -18.9894197881
            128.156            102.525       -10.7428704760      -18.9742991317
            122.054             97.643       -10.7273118140      -18.9556871679
            116.241             92.993       -10.7085991597      -18.9331679971
linear regression
converged value                              -10.9079580568      -19.1711146204
  • Take the “converged value”, in this case: EC(RPA) = -10.9079580568eV (an approximate “infinite basis set” limit).
  • This calculations needs the orbitals (WAVECAR file) and the derivative of the orbitals w.r.t. the Bloch wavevectors (WAVEDER file) written in Step 4.
  • The RPA total energy is calculated as the, E(RPA)=EC(RPA)+EXX sum of the RPA correlation energy of step 5 EC(RPA) and the Hartree fock energy EXX. To get the Hartree fock energy grep “free energy” in the OUTCAR.EXX.* file (there are two spaces between free and energy).
  • The sample output for the total energy vs volume curves for DFT and RPA should look like the following:


Download

Si_ACFDT_vol.tgz

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