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MedeA®-Electronics provides the ability to calculate the electronic properties of solids that involve the electronic states in a narrow energy range about the Fermi energy, that is, those states that can be thermally activated or activated by doping. These electronic states govern the response of the material to external electric fields or temperature gradients, which produce electric and heat currents. Properties of prime interest are effective masses, electrical conductivity and thermoelectric power which complement the calculation of accurate electronic band structures using MedeA® VASP - all of which are accessible from MedeA®-Electronics.
The combination of electronic band structures obtained from MedeA®‑VASP and the properties predicted by MedeA®‑Electronics gives users a toolbox for the comprehensive analysis and understanding of the electronic properties of desired materials.
MedeA®‑Electronics is fully integrated into the MedeA® Environment allowing it to take advantage of the robust MedeA® JobServer and TaskServer Infastructure. Calculations are efficiently managed across the desired number of CPU cores.
| Γ-point Effective Mass of Si | Zeghbroeck | IOFFE | MedeA® |
|---|---|---|---|
| Electrons | measured | measured | calculated |
| Longitudinal | 0.98 | 0.98 | 0.96 |
| Transverals | 0.19 | 0.19 | 0.19 |
| DOS Mass | 1.08 | 1.08 | 1.08 |
| Conductivity Mass | 0.26 | 0.26 | 0.26 |
| Heavy Hole | 0.49 | 0.49 | * |
| Light Hole | 0.16 | 0.16 | 0.18 |
| Split-off Band | 0.29 | 0.24 | 0.23 |
Calculated effective masses of both hole and electron states nearly perfectly agree with experimental data.
*Principle difficulties in measuring and calculating the Γ-point heavy-hole mass are easily traced to the strong anisotropy of the respective band close to this point shown in the isoenergy surfaces above.