abinit/tests/tutorial/Input/tgw1_2.abi

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# Crystalline silicon
# Calculation of the GW corrections
# Dataset 1: ground state calculation
# Dataset 2: calculation of the WFK file for only Gamma point
# Dataset 3: calculation of the screening (epsilon^-1 matrix for W)
ndtset 3
# Definition of the k-point grid
ngkpt 2 2 2
nshiftk 1
shiftk 0.0 0.0 0.0
istwfk *1 # Option needed for special k-points like Gamma
# Dataset1: usual self-consistent ground-state calculation
nband1 6
tolvrs1 1.0e-10
# Dataset2: calculation of WFK file
# Definition of the SCF procedure
iscf2 -2 # Non self-consistent calculation
getden2 -1 # Read previous density file
tolwfr2 1.0d-12 # Still get it converged
nband2 260
nbdbuf2 40
# Dataset3: Calculation of the screening (epsilon^-1 matrix)
optdriver3 3
getwfk3 -1
nband3 60
ecuteps3 6.0
ppmfrq3 16.7 eV # It is easier (and safer) to let ABINIT compute and use the Drude plasma frequency,
# instead of selecting a value by hand. This would be done thanks to the default value ppmfrq 0.0 .
# Definition of the unit cell: fcc
acell 3*10.26 # Experimental lattice constants
rprim 0.0 0.5 0.5 # FCC primitive vectors (to be scaled by acell)
0.5 0.0 0.5
0.5 0.5 0.0
# Definition of the atom types
ntypat 1 # There is only one type of atom
znucl 14 # The keyword "znucl" refers to the atomic number of the
# possible type(s) of atom. The pseudopotential(s)
# mentioned in the "files" file must correspond
# to the type(s) of atom. Here, the only type is Silicon.
pp_dirpath "$ABI_PSPDIR"
pseudos "Psdj_nc_sr_04_pbe_std_psp8/Si.psp8"
# Definition of the atoms
natom 2 # There are two atoms
typat 1 1 # They both are of type 1, that is, Silicon.
xred # Reduced coordinate of atoms
0.0 0.0 0.0
0.25 0.25 0.25
# Definition of the planewave basis set (at convergence 16 Rydberg 8 Hartree)
ecut 8.0 # Maximal kinetic energy cut-off, in Hartree
# Definition of the SCF procedure
nstep 20 # Maximal number of SCF cycles
diemac 12.0 # Although this is not mandatory, it is worth to
# precondition the SCF cycle. The model dielectric
# function used as the standard preconditioner
# is described in the "dielng" input variable section.
# Here, we follow the prescription for bulk silicon.
##############################################################
# This section is used only for regression testing of ABINIT #
##############################################################
#%%<BEGIN TEST_INFO>
#%% [setup]
#%% executable = abinit
#%% test_chain = tgw1_2.abi, tgw1_3.abi, tgw1_4.abi, tgw1_5.abi
#%% [files]
#%% files_to_test =
#%% tgw1_2.abo, tolnlines= 70, tolabs= 1.010e-03, tolrel= 1.000e+00
#%% [shell]
#%% post_commands =
#%% ww_cp tgw1_2o_DS2_WFK tgw1_3o_DS2_WFK;
#%% ww_cp tgw1_2o_DS3_SCR tgw1_3o_DS3_SCR;
#%% ww_cp tgw1_2o_DS2_WFK tgw1_4o_DS2_WFK;
#%% ww_cp tgw1_2o_DS2_WFK tgw1_5o_DS2_WFK;
#%% [paral_info]
#%% max_nprocs = 1
#%% [extra_info]
#%% authors = V. Olevano, F. Bruneval, M. Giantomassi
#%% keywords = GW
#%% description =
#%% Crystalline silicon
#%% Calculation of the GW corrections
#%% Dataset 1: ground state calculation
#%% Dataset 2: calculation of the WFK file for only Gamma point
#%% Dataset 3: calculation of the screening (epsilon^-1 matrix for W)
#%%<END TEST_INFO>