# Aluminum diatomic molecule for tests of dielectric matrix. # Note : use a shifted geometry, in order to have non-symmorphic # rotations. acell 18 11 11 diecut 1.4 diegap 0.1d0 dielam 0.0d0 diemac 1.0d0 diemix 0.2d0 ecut 2.0 enunit 2 intxc 1 iprcel 28 iscf 2 istatr 9 ixc 0 kptopt 0 kpt 0.25 0.25 0.25 natom 2 nband 20 nkpt 1 nstep 30 nsym 4 ntypat 1 occopt 1 prtvol 10 rprim 1 0 0 0 1 0 0 0 1 symrel 1 0 0 0 1 0 0 0 1 1 0 0 0 1 0 0 0 -1 1 0 0 0 -1 0 0 0 1 1 0 0 0 -1 0 0 0 -1 tnons 3*0.0d0 9*0.0d0 0.3333333333333333d0 0.0d0 0.0d0 0.3333333333333333d0 0.0d0 0.0d0 0.3333333333333333d0 0.0d0 0.0d0 0.3333333333333333d0 0.0d0 0.0d0 toldfe 1.0d-12 typat 1 1 wtk 1 3*1 xcart 0.0 0.0 0.0 6.0 0.0 0.0 znucl 13.0 pp_dirpath "$ABI_PSPDIR" pseudos "PseudosGTH_pwteter/13al.pspgth" #%% #%% [setup] #%% executable = abinit #%% test_chain = t51.in, t52.in #%% [files] #%% files_to_test = #%% t51.out, tolnlines = 0, tolabs = 0.000e+00, tolrel = 0.000e+00 #%% [paral_info] #%% max_nprocs = 1 #%% [extra_info] #%% keywords = NC #%% authors = Unknown #%% description = #%% Al2 molecule, inversion point shifted from the origin, ixc=0, #%% kpt=1/4 1/4 1/4, nsym=4. #%% Large number of bands (20 instead of 3). #%% 8 first SCF steps with simple mixing algorithm, mixing factor 1/5. #%% Slow convergence. #%% Computation of the hermitian dielectric matrix at the 8th step. #%% The inverse of the dielectric matrix is then used as preconditioning. #%% A factor of 20 is gained on each step. Largest eigenvalue value of the #%% dielectric matrix is 5.712 (a mixing factor of 1/3 would have #%% been enough, but 1/5 is faster). A second eigenvalue is close : 5.531 . #%%