# Rhombohedral Bi treated as a semiconductor # 2x2x2 grid, automatically generated, unlike with # Test_v3#2 . Should give exactly the same results. # Execute only datasets 8 and 10. ndtset 2 jdtset 8 10 #Dataset 8 : GS with spin-orbit tolvrs8 1.0d-20 kptopt8 1 #Dataset 10 : RF with spin-orbit nqpt10 1 qpt10 3*0.0d0 rfphon10 1 getwfk10 8 kptopt10 2 toldfe10 1.1d-12 nstep10 15 #Common data acell 3*9.0d0 angdeg 3*57.25d0 ecut 2.0d0 natom 2 nband 10 ngkpt 2 2 2 nspinor 2 nstep 20 ntypat 1 rfatpol 1 1 rfdir 1 0 0 typat 1 1 xred 3*0.231d0 3*-0.231d0 znucl 83.d0 pp_dirpath "$ABI_PSPDIR" pseudos "PseudosHGH_pwteter/83bi.5.hgh" #%% #%% [setup] #%% executable = abinit #%% [files] #%% files_to_test = #%% t14.out, tolnlines = 6, tolabs = 2.000e-01, tolrel = 3.000e-01, fld_options = -easy #%% [paral_info] #%% max_nprocs = 2 #%% [extra_info] #%% authors = Unknown #%% keywords = NC, DFPT #%% description = #%% Bi A7 structure (2 atoms per unit cell), #%% using the HGH pseudopotential, within LDA. #%% Fixed cell dimensions. Treated as a semi-conductor #%% Test the response to atomic displacements, #%% with spin-orbit. Should give the same answer #%% than test 2, except that the k point grid is now #%% defined automatically. #%% Dataset 8 : frozen-phonon with spin-orbit #%% Dataset 10 : RF with spin-orbit. #%% The agreement is as good as without #%% spin-orbit ! Frozen-phonon 2DTE=2.48156, #%% RF 2DTE=2.48156 . #%% Warning : the output file of this test #%% is machine-dependent, although the final #%% result is not. This is because the #%% degeneracy of the GS wavefunctions with #%% different spin orientation has not been broken. #%%