abinit/tests/v7/Input/t10.abi

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# Nickel ferromagnetic fcc structure. ONCVPSP pseudo with valence density.
ecut 25
nband 12
nsppol 2
spinat 0. 0. 4.
# Treat core charge in G-space (default for NC is real-space)
nc_xccc_gspace 1
# Write psps% data in netcdf format.
prtpsps 1
# Structural relaxation with densfor_pred
ionmov 2
optcell 2
densfor_pred 6
ecutsm 0.5
dilatmx 1.02
ntime 2
# SCF cycle
nstep 50
tolvrs 1.0d-9
# K-point sampling and smearing
occopt 7
tsmear 0.0075
ngkpt 6 6 6
nshiftk 4
shiftk 1/2 1/2 1/2
1/2 0.0 0.0
0.0 1/2 0.0
0.0 0.0 1/2
# Crystalline structure.
ntypat 1
acell 3*3.52 angstrom
rprim 0.0 1/2 1/2
1/2 0.0 1/2
1/2 1/2 0.0
natom 1
typat 1
xred 0.0 0.0 0.0
znucl 28
pp_dirpath "$ABI_PSPDIR"
pseudos "Ni-psval-icmod3.psp8"
#%%<BEGIN TEST_INFO>
#%% [setup]
#%% executable = abinit
#%% [files]
#%% files_to_test=t10.abo, tolnlines=5, tolabs=1.00e-3, tolrel=2.00e-2, fld_options=-easy
#%% [paral_info]
#%% max_nprocs = 8
#%% [extra_info]
#%% authors = M. Giantomassi
#%% keywords = NC, psp8
#%% description =
#%% Nickel ferromagnetic fcc structure with an ONCVPSP pseudo containing valence density.
#%% We test several improvements that are available when the NC file contains the PS valence charge.
#%% More specifically, we test the initialization of the density from atomic quantities (initro.F90),
#%% the correction to the forces due to the residuals and the extrapolation of the density
#%% for structural relaxations (well, xred is fixed by symmetry).
#%% We also test the treatment of the core charge in G-space in the case of GS calculations
#%% By default, abinit handles XCCC in real space, here we use nc_xccc_gspace==1 to treat it
#%% in G-space using the same approach as the one used in PAW.
#%% topics = GeoOpt
#%%<END TEST_INFO>