pwmat:demo:dipole1
目录
Transition dipole moment calculation exclude local field
Transition dipole moment calculaton in CsPbI3.
There are four steps, the first step is “SCF” calculation, the second is “NONSCF” calculation, the third is “DOS” calculation, and the fourth step is to process the data with TDM.x tool.
First Step: “SCF” calculation
Input files
atom.config
5 LATTICE 6.39011884 0.00000000 0.00000000 0.00000000 6.39011884 0.00000000 0.00000000 0.00000000 6.39011884 POSITION 55 0.50000000 0.50000000 0.50000000 1 1 1 82 0.00000000 0.00000000 0.00000000 1 1 1 53 0.00000000 0.00000000 0.50000000 1 1 1 53 0.50000000 0.00000000 0.00000000 1 1 1 53 0.00000000 0.50000000 0.00000000 1 1 1
etot.input
4 1 JOB = SCF IN.PSP1 = Cs.SG15.PBE.UPF IN.PSP2 = Pb-d.SG15.PBE.UPF IN.PSP3 = I.SG15.PBE.UPF IN.ATOM = atom.config CONVERGENCE = difficult Ecut = 50 Ecut2 = 100 MP_N123 = 5 5 5 0 0 0
Cs.SG15.PBE.UPF, Pb-d.SG15.PBE.UPF, I.SG15.PBE.UPF
Calculations
- You can submit PWmat tasks in different ways:
mpirun -np 4 PWmat | tee output
Run the command directly
#!/bin/bash #PBS -N SCF #PBS -l nodes=1:ppn=4 #PBS -q batch #PBS -l walltime=100:00:00 ulimit -s unlimited cd $PBS_O_WORKDIR mpirun -np 4 PWmat | tee output
Submit the task with a pbs script
Second Step: “NONSCF” calculation
Input files
atom.config
5 LATTICE 6.39011884 0.00000000 0.00000000 0.00000000 6.39011884 0.00000000 0.00000000 0.00000000 6.39011884 POSITION 55 0.50000000 0.50000000 0.50000000 1 1 1 82 0.00000000 0.00000000 0.00000000 1 1 1 53 0.00000000 0.00000000 0.50000000 1 1 1 53 0.50000000 0.00000000 0.00000000 1 1 1 53 0.00000000 0.50000000 0.00000000 1 1 1
etot.input
4 1 JOB = NONSCF IN.PSP1 = Cs.SG15.PBE.UPF IN.PSP2 = Pb-d.SG15.PBE.UPF IN.PSP3 = I.SG15.PBE.UPF IN.ATOM = atom.config Ecut = 50 Ecut2 = 100 IN.VR = T IN.KPT = T
- How to get IN.VR and IN.KPT, please refer to the example Bandstructure calculation.
- The file gen.kpt:
BAND # COMMENT line 20 # number of k-points between X and R 0.000 0.500 0.000 X # reciprocal coordinates; label 'X' for X point 0.500 0.500 0.500 R 20 0.500 0.500 0.500 R 0.500 0.500 0.000 M 20 0.500 0.500 0.000 M 0.000 0.000 0.000 G 20 0.000 0.000 0.000 G 0.500 0.500 0.500 R
Cs.SG15.PBE.SOC.UPF, Pb-d.SG15.PBE.SOC.UPF, I.SG15.PBE.UPF
Calculations
- You can submit PWmat tasks in different ways:
mpirun -np 4 PWmat | tee output
Run the command directly
#!/bin/bash #PBS -N SCF #PBS -l nodes=1:ppn=4 #PBS -q batch #PBS -l walltime=100:00:00 ulimit -s unlimited cd $PBS_O_WORKDIR mpirun -np 4 PWmat | tee output
Submit the task with a pbs script
Third Step: “DOS” calculation
Input files
atom.config
5 LATTICE 6.39011884 0.00000000 0.00000000 0.00000000 6.39011884 0.00000000 0.00000000 0.00000000 6.39011884 POSITION 55 0.50000000 0.50000000 0.50000000 1 1 1 82 0.00000000 0.00000000 0.00000000 1 1 1 53 0.00000000 0.00000000 0.50000000 1 1 1 53 0.50000000 0.00000000 0.00000000 1 1 1 53 0.00000000 0.50000000 0.00000000 1 1 1
etot.input
4 1 JOB = DOS IN.PSP1 = Cs.SG15.PBE.UPF IN.PSP2 = Pb-d.SG15.PBE.UPF IN.PSP3 = I.SG15.PBE.UPF IN.ATOM = atom.config Ecut = 50 Ecut2 = 100 Ecutp = 100 IN.WG = T IN.KPT = T
- Read IN.WG from previous NONSCF calculation OUT.WG.
- You also need copy OUT.EIGEN and OUT.FERMI from previous NONSCF calculation.
- IN.KPT is the same as previous NONSCF calculation.
Cs.SG15.PBE.SOC.UPF, Pb-d.SG15.PBE.SOC.UPF, I.SG15.PBE.UPF
Calculations
- You can submit PWmat tasks in different ways:
mpirun -np 4 PWmat | tee output
Run the command directly
#!/bin/bash #PBS -N SCF #PBS -l nodes=1:ppn=4 #PBS -q batch #PBS -l walltime=100:00:00 ulimit -s unlimited cd $PBS_O_WORKDIR mpirun -np 4 PWmat | tee output
Submit the task with a pbs script
Fourth Step: run TDM.x
Input files
TDM.input
0 #flag: possible values 0, 1. 0: no nonlocal potential; 1: nonlocal potential is taken into account 37 38 #i,j: TDM between j and j state.
- flag 0: TDM.x will read TDM.input, OUT.WG, OUT.EIGEN and OUT.GKK.
- flag 1: TDM.x will read TDM.input and OUT.momentK._ (_ represents multiple files)
- After run TDM.x, you will get transition_moment file:
ikpt X-component Y-component Z-component Total(e^2*bohr^2) X-real X-imag Y-real Y-imag Z-real Z-imag 1 0.7198E-11 0.2949E+02 0.4606E-11 0.2949E+02 -0.1739E-05 0.2043E-05 0.1961E+01 0.5064E+01 -0.6900E-06 0.2032E-05 2 0.6357E-12 0.2951E+02 0.3241E-11 0.2951E+02 -0.5834E-06 0.5435E-06 0.2084E+01 -0.5017E+01 0.6696E-06 0.1671E-05 3 0.1115E-10 0.2962E+02 0.4501E-11 0.2962E+02 0.2978E-05 -0.1510E-05 -0.5258E+01 -0.1404E+01 0.9306E-06 -0.1907E-05 ... ... ... 83 0.1498E+02 0.1315E+01 0.7419E+01 0.2371E+02 0.5129E+00 -0.3836E+01 -0.1307E+00 0.1139E+01 -0.3821E+00 0.2697E+01 84 0.2322E+02 0.5479E+01 0.7938E+01 0.3663E+02 0.3863E+01 0.2879E+01 -0.2275E+01 -0.5526E+00 -0.1589E+01 -0.2327E+01 85 0.3655E+02 0.4251E+01 0.2792E+01 0.4359E+02 -0.5741E+01 -0.1895E+01 0.1737E+01 0.1111E+01 0.4033E+00 0.1622E+01
pwmat/demo/dipole1.txt · 最后更改: 2024/02/04 17:50 由 pengge
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