#Test the use of a double loop, up to a dataset number that is beyond 1000 (last one is 1022). # Computation of the band structure. # First, a SCF density computation, then a non-SCF band structure calculation. ndtset 204 udtset 102 2 # Translate the atoms from one dataset to the next one xred:? # This keyword indicate that the location of the atoms # will follow, one triplet of number for each atom 0.0 0.0 0.0 # Triplet giving the REDUCED coordinate of atom 1. 1/4 1/4 1/4 # Triplet giving the REDUCED coordinate of atom 2. xred+? 6*0.0001 chksymbreak 0 #Definition of the planewave basis set ecut 4.0 #ecut:? 4.0 # Starting kinetic energy cut-off, in Hartree #ecut+? 0.1 # Increment of kinetic energy cut-off, in Hartree getwfk11 0 getwfk -2 #Dataset 1 : usual self-consistent calculation kptopt?1 1 # Option for the automatic generation of k points, # taking into account the symmetry nshiftk?1 4 shiftk?1 0.5 0.5 0.5 # These shifts will be the same for all grids 0.5 0.0 0.0 0.0 0.5 0.0 0.0 0.0 0.5 ngkpt?1 1 1 1 prtden?1 1 # Print the density, for use by dataset 2 toldfe?1 1.0d-6 # This value is way too large for most realistic studies of materials #Dataset 2 : the band structure iscf?2 -2 getden?2 -1 kptopt?2 -1 nband?2 8 ndivk?2 2 # 2 divisions of the segment kptbounds?2 0.5 0.0 0.0 # L point 0.0 0.0 0.0 # Gamma point tolwfr?2 1.0d-12 enunit?2 1 # Will output the eigenenergies in eV #Definition of the unit cell acell 3*10.217 # This is equivalent to 10.217 10.217 10.217 rprim 0.0 0.5 0.5 # FCC primitive vectors (to be scaled by acell) 0.5 0.0 0.5 0.5 0.5 0.0 #Definition of the atom types ntypat 1 # There is only one type of atom znucl 14 # The keyword "znucl" refers to the atomic number of the # possible type(s) of atom. The pseudopotential(s) # mentioned in the "files" file must correspond # to the type(s) of atom. Here, the only type is Silicon. #Definition of the atoms natom 2 # There are two atoms typat 1 1 # They both are of type 1, that is, Silicon. #Definition of the SCF procedure nstep 10 # Maximal number of SCF cycles diemac 12.0 # Although this is not mandatory, it is worth to # precondition the SCF cycle. The model dielectric # function used as the standard preconditioner # is described in the "dielng" input variable section. # Here, we follow the prescription for bulk silicon. #timopt 1 pp_dirpath "$ABI_PSPDIR" pseudos "PseudosTM_pwteter/14si.pspnc" #%% #%% [setup] #%% executable = abinit #%% [files] #%% files_to_test = #%% t34.out, tolnlines = 0, tolabs = 0.0, tolrel = 0.0, fld_options = #%% [paral_info] #%% max_nprocs = 1 #%% [extra_info] #%% authors = Unknown #%% keywords = #%% description = #%% Crystalline silicon. Diamond structure. #%% Quick test of the use of datasets with a numbering beyond 1000 (the last one is 1022). #%% (Tests 35-40 are for response-function) #%%