abinit/tests/v7/Input/t57.abi

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# C in diamond structure; Very rough 2x2x2 special point grid; low ecut.
# Only 1 random q-points
ndtset 3
elph2_imagden 0.1 eV
ngkpt 3*2
#This should not change with convergence studies
nshiftk 1
shiftk 0.0 0.0 0.0
qptopt 0
# Ground state density
getwfk1 0
getden1 0
prtden1 1
nqpt1 0
ieig2rf1 0
rfphon1 0
smdelta1 0
# Non self-consistent calculation with an abritrary q point
getden2 -1
ieig2rf2 0
smdelta2 0
rfphon2 0
iscf2 -2
qpt2 0.11 0.0 0.0
wtq2 0.1 # Random weigth value for testing purposes.
# Computation at an other q point
getwfk3 -2
getwfq3 -1
qpt3 0.11 0.0 0.0
wtq3 0.1 # Random weigth value for testing purposes.
# Common input variables, to be superceded in some cases
nqpt 1
ieig2rf 4
smdelta 1
kptopt 3 # Need full k-point set for finite q response
rfphon 1 # Do phonon response
# Cell dependant parameters
acell 3*6.6709983131
rprim 0 .5 .5 .5 0 .5 .5 .5 0
nsym 1 # To be on the safe side. The implementation of symmetry should be perform.
natom 2
typat 1 1
xred 3*0.0 3*0.25
nband 10
ntypat 1
znucl 6
diemac 6
ecut 10
enunit 2
nstep 50
tolwfr 1.0d-8
istwfk *1
pp_dirpath "$ABI_PSPDIR"
pseudos "PseudosTM_pwteter/6c.pspnc"
#%%<BEGIN TEST_INFO>
#%% [setup]
#%% executable = abinit
#%% [shell]
#%% post_commands =
#%% [files]
#%% files_to_test =
#%% t57.abo, tolnlines = 7, tolabs = 1.1e-3, tolrel = 2.0e-4, fld_options = -medium
#%% [paral_info]
#%% max_nprocs = 2
#%% [extra_info]
#%% authors = S. Ponc\'e
#%% keywords = NC, DFPT, EPH_OLD
#%% description =
#%% Diamond. The wtq variable is introduced to be able to reproduce the q-point
#%% weight obtained with ngqpt and qptopt.
#%% The main reason being that the initialization of large q-point (same for k-point) grid
#%% is extremely slow. Inputing manually the qpt and wtq in the input file avoid such
#%% inefficient initialization.
#%% topics = TDepES
#%%<END TEST_INFO>