#Prepare the computation of linear and non-linear optic properties #of GaAs crystal : ground-state with few bands, #then non-SCF with a larger number of bands, then ddk for different directions #Note that the k point sampling shoud be finer for significant results. The cut-off energy is also too low. ndtset 6 #First dataset : SC run with kpoints in the IBZ iscf1 3 nband1 42 nstep1 200 nbdbuf1 0 prtden1 1 getden1 0 getwfk1 0 ! Usual file handling data #Second dataset : NSC run with large number of bands, and points in the IBZ iscf2 -2 nband2 68 ! This number of bands might be too low for non-linear optics and real part of linear optics nstep2 200 getwfk2 1 getden2 1 ! Usual file handling data #Third dataset : NSC run with large number of bands, and points in the the full BZ iscf3 -2 nband3 68 ! This number of bands might be too low for non-linear optics and real part of linear optics nstep3 200 getwfk3 2 getden3 1 ! Usual file handling data #Fourth dataset : ddk response function along axis 1 iscf4 -3 nband4 68 ! This number of bands might be too low for non-linear optics and real part of linear optics nstep4 1 nline4 0 nqpt4 1 qpt4 0.0d0 0.0d0 0.0d0 rfdir4 1 0 0 rfelfd4 2 getwfk4 3 #Fifth dataset : ddk response function along axis 2 iscf5 -3 nband5 68 ! This number of bands might be too low for non-linear optics and real part of linear optics nstep5 1 nline5 0 nqpt5 1 qpt5 0.0d0 0.0d0 0.0d0 rfdir5 0 1 0 rfelfd5 2 getwfk5 3 Sixth dataset : ddk response function along axis 3 iscf6 -3 nband6 68 ! This number of bands might be too low for non-linear optics and real part of linear optics nstep6 1 nline6 0 nqpt6 1 qpt6 0.0d0 0.0d0 0.0d0 rfdir6 0 0 1 rfelfd6 2 getwfk6 3 ######################################################################### #Data common to all datasets############################################# ######################################################################### nsym 0 kptopt 0 nkpt 1 kpt 0.0d0 0.0d0 0.0d0 acell 43 44 38 rprim 1.0 0.0 0.0 0.0 1.0 0.0 0.0 0.0 1.0 #Definition of the atom types ntypat 3 znucl 6 7 1 #Definition of the atoms natom 24 typat 1 1 1 1 1 1 1 1 1 1 1 1 3 3 3 3 3 3 3 3 3 3 2 2 tolwfr 1.e-20 nbdbuf 2 #Definition of the planewave basis set ecut 5 # Maximal kinetic energy cut-off, in Hartre diemac 1.5 diemix 0.5 xcart 0.12610908E+02 0.69923842E+01 0.10268339E+02 0.15207306E+02 0.74174076E+01 0.10386263E+02 0.16167274E+02 0.98948730E+01 0.10484650E+02 0.14489426E+02 0.11953405E+02 0.10343192E+02 0.11894070E+02 0.11510622E+02 0.10175298E+02 0.10942651E+02 0.90405743E+01 0.10160446E+02 0.18112287E+02 0.13367950E+02 0.15093961E+02 0.17969181E+02 0.15296873E+02 0.16887708E+02 0.19363503E+02 0.17526713E+02 0.16588913E+02 0.20959827E+02 0.17804747E+02 0.14499162E+02 0.21158066E+02 0.15864730E+02 0.12730375E+02 0.19691041E+02 0.13660835E+02 0.12973277E+02 0.89148169E+01 0.87156412E+01 0.10023436E+02 0.16544236E+02 0.58533533E+01 0.10372034E+02 0.15204634E+02 0.13878773E+02 0.10327155E+02 0.10597717E+02 0.13104246E+02 0.10043308E+02 0.11890805E+02 0.50646308E+01 0.10204072E+02 0.16761223E+02 0.15060892E+02 0.18538351E+02 0.22094006E+02 0.19508725E+02 0.14280691E+02 0.22468742E+02 0.15993571E+02 0.11149587E+02 0.17030923E+02 0.11640529E+02 0.15354660E+02 0.19238302E+02 0.19020122E+02 0.17999518E+02 0.18892502E+02 0.10035037E+02 0.10276291E+02 0.20327037E+02 0.11703030E+02 0.11172947E+02 ####################################################################