Examples¶
Introduction¶
AMP2includes several examples (for Si, Ge and NiO) in AMP2/examples/.
Execute AMP2¶
Before running examples, please set the configuration to be suitable for your system. (See Installation and execution) Then, you can execute AMP2 using shell script as following.
sh run.sh
Calculation results¶
When the calculation is finished, Sub-directory is generated in Done path. (Ex. /Done/Si) In the Sub-directory/Results, you can obtain optimized structure, band gap, band structure, density of states, dielectric constant and effective mass of hole and electron.
Si¶
Si is a typical example of semiconductor. Therefore, we calculate all properties supported by AMP2in this example.
Optimized structure (/Results/POSCAR_rlx_GGA)
relaxed poscar 1.000000000 0.0 2.73243086189 2.73243086189 2.73243086189 -0.0 2.73243086189 2.73243086189 2.73243086189 0.0 Si 2 Selective dynamics Direct 0.5 0.5 0.5 T T T ! Si1 0.75 0.75 0.75 T T T ! Si1Band gap (/Results/band_gap_GGA.log)
Band gap: 0.612 eV (Indirect) VBM: 0.0 0.0 0.0 : 5.649 eV CBM: 0.4166667 0.0 0.4166667 : 6.261 eV nVBM: 4 spin: 1 nCBM: 5 spin: 1Band structure (/Results/band_GGA.png and /Results/band_GGA.pdf)
Band gap from HSE@PBE (/Results/band_hybrid_GGA.log)
Band gap: 1.187 eV (Indirect) VBM: 0.0 0.0 0.0 : 5.289 eV CBM: 0.4166667 0.0 0.4166667 : 6.477 eV nVBM: 4 spin: 1 nCBM: 5 spin: 1Corrected band structure (/Results/band_GGA_corrected.png and /Results/band_GGA_corrected.pdf)
Density of states (/Results/dos_GGA.log)
Dielectric constant (/Results/dielectric_GGA.log)
Dielectric tensor (electronic contribution): 12.936 0.000 -0.000 0.000 12.936 0.000 -0.000 0.000 12.936 Dielectric tensor (ionic contribution): 0.000 0.000 0.000 0.000 -0.000 -0.000 0.000 -0.000 0.000 Dielectric constant diagonalization (electronic): 12.936 12.936 12.936 Dielectric constant diagonalization (ionic): 0.000 -0.000 0.000 Averaged static dielectric constant: 12.936Effective mass of hole (/effective_mass_hole_GGA.log)
hole -0.266 -0.000 -0.000 -0.000 -0.266 -0.000 -0.000 -0.000 -0.266 Diagonalized effective mass: -0.266 -0.266 -0.266Effective mass of electron (/Results/effective_mass_hole_GGA.log)
electron 0.287 0.000 0.000 0.000 0.287 0.000 0.000 0.000 0.287 Diagonalized effective mass: 0.287 0.287 0.287
Ge¶
Ge is a well-known semiconductor with metallic band structure in conventional DFT schemes like LDA and PBE. In AMP2, however, we can obtain the reliable band gap and band structure due to the band gap correction scheme. In this example, we calculate corrected band structure.
Band gap (/Results/band_gap_GGA.log)
This system is metallic. ! If it is not hybrid calculation, additional search is required for hybrid calculation.Band structure (/Results/band_GGA.png and /Results/band_GGA.pdf)
Band gap from HSE@PBE (/Results/band_hybrid_GGA.log)
Band gap: 0.161 eV (Direct) VBM: 0.0 0.0 0.0 : 2.875 eV CBM: 0.0 0.0 0.0 : 3.036 eV nVBM: 4 spin: 1 nCBM: 5 spin: 1Corrected band structure (/Results/band_GGA_corrected.png and /Results/band_GGA_corrected.pdf)
NiO¶
NiO is one of the antiferromagnetic materials. In this example, we show the most stable magnetic spin ordering for NiO and its electronic configurations (band strucrue and density of states).
Optimized structure (/Results/POSCAR_rlx_GGA)
relaxed poscar 1.000000000 1.47786935879 0.853248272122 4.82278497551 -1.47786935879 0.853248272122 4.82278497551 0.0 -1.70649654425 4.82278497551 Ni O 2 2 Selective dynamics Direct 0.5 0.5 0.5 T T T ! Ni1_up -0.0 -0.0 0.0 T T T ! Ni1_down 0.750000037602 0.750000037602 0.750000037602 T T T ! O1 0.249999962398 0.249999962398 0.249999962398 T T T ! O1Band gap (/Results/band_gap_GGA.log)
Band gap: 3.433 eV (Indirect) VBM: 0.5 0.5 0.5 : 6.242 eV CBM: 0.0 0.0 0.0 : 9.675 eV nVBM: 16 spin: 1 nCBM: 17 spin: 2Band structure (/Results/band_GGA.png and /Results/band_GGA.pdf)
Density of states (/Results/dos_GGA.log)