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Excited Acceptor States in II–VI and III–V Semiconductors
35
Citations
32
References
1990
Year
SemiconductorsIi-vi SemiconductorElectrical EngineeringEngineeringPhysicsExcited Acceptor StatesCubic CorrectionApplied PhysicsQuantum MaterialsRadial EquationsSemiconductor MaterialElectronic Excited StateElectronic StructureOptoelectronicsLipari Spherical ModelCompound SemiconductorSemiconductor Nanostructures
Abstract Higher excited states of acceptors in CdTe, ZnTe, and GaAs are obtained by using the Baldereschi and Lipari spherical model including the cubic correction and the central‐cell effect. This is done by solving the coupled radial equations by the finite‐element method with Arnoldi's algorithm, which gives several (≈ 20) low‐lying states simultaneously. The procedure permits to determine very accurately the host band‐structure parameters. In the case of II–VI compounds, the Luttinger parameters γ 1 = 5.30, γ 2 = 1.62, γ 3 = 2.10 and the dielectric constant ϵ 0 = 9.3 for CdTe and, γ 1 = 3.80, γ 2 = 0.86, γ 3 = 1.32 and ϵ 0 = 9.4 for ZnTe are obtained. For GaAs, γ 1 = 7.20, γ 2 = 2.15, γ 3 = 3.05, and ϵ 0 = 12.49 are obtained.
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