# * Born effective charges ndtset 3 # Set 1 : Initial self-consistent run iscf1 5 kptopt1 1 tolvrs1 1.0d-18 #need excellent convergence of GS quantities for RF runs # Set 2 : Calculate the ddk wf's - needed for piezoelectric tensor and # Born effective charges in dataset 3 getwfk2 -1 iscf2 -3 #this option is needed for ddk kptopt2 2 #use time-reversal symmetry only for k points nqpt2 1 #one wave vector will be specified qpt2 0 0 0 #need to specify gamma point rfelfd2 2 #set for ddk wf's only rfdir2 1 1 1 #full set of directions needed tolwfr2 1.0d-20 #only wf convergence can be monitored here # Set 3 : response-function calculations for all needed perturbations getddk3 -1 getwfk3 -2 iscf3 5 kptopt3 2 #use time-reversal symmetry only for k points nqpt3 1 qpt3 0 0 0 rfphon3 1 #do atomic displacement perturbation rfatpol3 1 4 #do for all atoms rfstrs3 3 #do strain perturbation rfdir3 1 1 1 #the full set of directions is needed tolvrs3 1.0d-10 #need reasonable convergence of 1st-order quantities #Common input variables #Total enrgy of CuInSe (I42d group) #Definition of the unit cell acell 3*7.692047091691874 # This is equivalent to 10.61 10.61 10.61 rprim 1.0 0.0 0.0 # In lessons 1 and 2, these primitive vectors 0.0 1.0 0.0 # (to be scaled by acell) were 1 0 0 0 1 0 0 0 1 0.5 0.5 0.9329012766836911 # that is, the default. #Definition of the atom types ntypat 3 # There are two types of atom znucl 13 5 7 # 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, type 1 is the Aluminum, # type 2 is the Arsenic. #Definition of the atoms natom 8 # There are two atoms typat 1 1 2 2 3 3 3 3 # The first is of type 1 (Al), the second is of type 2 (As). xred # This keyword indicate that the location of the atoms # will follow, one triplet of number for each atom 6.9388939039E-18 -2.0816681712E-17 -1.3877787808E-17 -2.5000000000E-01 2.5000000000E-01 5.0000000000E-01 5.0000000000E-01 5.0000000000E-01 -1.3877787808E-17 2.5000000000E-01 -2.5000000000E-01 5.0000000000E-01 1.8173101317E-01 1.2500000000E-01 2.5000000000E-01 -4.3173101317E-01 -3.7500000000E-01 2.5000000000E-01 -1.2500000000E-01 4.3173101317E-01 -2.5000000000E-01 3.7500000000E-01 -1.8173101317E-01 -2.5000000000E-01 #Gives the number of band, explicitely (do not take the default) #nband 16 # For an insulator (if described correctly as an insulator # by DFT), there is no need to include conduction bands # in response-function calculations #Exchange-correlation functional ixc 1 # LDA Teter Pade parametrization #Definition of the planewave basis set ecut 5.0 # Maximal kinetic energy cut-off, in Hartree #Definition of the k-point grid #kptrlatt -4 4 4 # In cartesian coordinates, this grid is simple cubic, and # 4 -4 4 # actually corresponds to the so-called 8x8x8 Monkhorst-Pack grid. # 4 4 -4 # It might as well be obtained through the use of # ngkpt, nshiftk and shiftk . kptopt 1 #nkptopt 1 nshiftk 1 shiftk 0.50 0.50 0.50 0.5 0.0 0.0 0.0 0.5 0.0 0.0 0.0 0.5 ngkpt 4 4 3 #Definition of the SCF procedure nstep 150 # Maximal number of SCF cycles diemac 9.0 # Although this is not mandatory, it is worth to #toldfe 1.0d-6 # precondition the SCF cycle. The model dielectric # function used as the standard preconditioner # is described in the "dielng" input variable section. # The dielectric constant of AlAs is smaller that the one of Si (=12).