# beta-SiC # ndtset 6 # DATASET 1 : density + WFK nband1 20 # DATASET 2 : SCR symchi2 1 optdriver2 3 awtr2 1 nband2 20 ecuteps2 5. ecutwfn2 16 inclvkb2 2 getwfk2 -1 gwcomp2 0 # DATASET 3 : SIG optdriver3 4 symsigma3 1 nband3 20 ecutsigx3 8. ecutwfn3 16 getwfk3 -2 getscr3 -1 gwcomp3 0 nkptgw3 2 kptgw3 0. 0. 0. 0.5 0.5 0. bdgw3 2 4 5 5 gw_icutcoul3 3 # old deprecated value of icutcoul, only used for legacy # DATASET 4 : SIG optdriver4 4 symsigma4 1 nband4 20 ecutsigx4 8. ecutwfn4 8. getwfk4 -3 getscr4 -2 gwcomp4 1 # Switching on the closure trick gwencomp4 1.2 nkptgw4 2 kptgw4 0. 0. 0. 0.5 0.5 0. bdgw4 2 4 5 5 gw_icutcoul4 3 # old deprecated value of icutcoul, only used for legacy # DATASET 5 : SCR symchi5 1 optdriver5 3 awtr5 1 nband5 20 ecuteps5 5. ecutwfn5 16 inclvkb5 2 getwfk5 -4 gwcomp5 1 # Switching on the closure trick gwencomp5 1.2 # DATASET 6 : SIG symsigma6 1 optdriver6 4 nband6 20 ecutsigx6 8. ecutwfn6 16 getwfk6 -5 getscr6 -1 gwcomp6 1 # Switching on the closure trick gwencomp6 1.2 nkptgw6 2 kptgw6 0. 0. 0. 0.5 0.5 0. bdgw6 2 4 5 5 gw_icutcoul6 3 # old deprecated value of icutcoul, only used for legacy #### Common to all datasets #### # # printing options prtden 0 #prtwf 0 prtvol 1 enunit 1 # atomic types natom 2 ntypat 2 znucl 14 6 typat 1 2 # k-points parameters ngkpt 4 4 4 shiftk 0. 0. 0. istwfk 8*1 # cut-off ecut 12. # SCF parameters #toldfe 1.d-7 tolwfr 1.d-9 nstep 50 #geometry acell 3*8.155 rprim 0. 0.5 0.5 0.5 0. 0.5 0.5 0.5 0. # atomic positions xred 0.0000 0.0000 0.0000 0.2500 0.2500 0.2500 # XC potential ixc 7 pp_dirpath "$ABI_PSPDIR" pseudos "PseudosTM_pwteter/14si.pspnc, PseudosTM_pwteter/6c.pspnc" #%% #%% [setup] #%% executable = abinit #%% [files] #%% files_to_test = #%% t69.out, tolnlines = 15, tolabs = 1.010e-03, tolrel = 7.000e-03, fld_options = -medium #%% [paral_info] #%% max_nprocs = 8 #%% [extra_info] #%% authors = M. Giantomassi #%% keywords = NC, GW #%% description = #%% Beta-SiC #%% Calculation of the GW corrections with extrapolar approximation and in-core solution. #%% Similar to t65, the main difference is that symmetries are used both in chi0 and sigma and also #%% the extrapolar term is symmetrized. Using a larger G-sphere for wavefunctions wrt t65 in order to #%% reduce the number of G1-G2 vectors falling outside the "ecutwfn" sphere (see completchi0_deltapart.F90). #%% topics = GW #%%