Physical review. B, Solid state · 1972 · 1.5K citations · 18 references
Natural SciencesMaterials SciencePhysicsCondensed Matter PhysicsSemiconductor MaterialsSpectroscopyAmorphous MaterialsAmorphous SemiconductorsAmorphous SolidsOptical Properties Of SemiconductorsOptical Properties Of SolidsSemiconductor PhysicsBand GapElectronic Density Of StatesElectronic Structure Of Amorphous MaterialsLight ScatteringMobility GapOptical Band GapOptical Properties Of Amorphous MaterialsOptical Transitions
Optical absorption measurements near the absorption edge are presented for three bulk semiconductor glasses: ${\mathrm{As}}_{2}$${\mathrm{S}}_{3}$, ${\mathrm{Ge}}_{33}$${\mathrm{As}}_{12}$${\mathrm{Se}}_{55}$, and ${\mathrm{Ge}}_{28}$${\mathrm{Sb}}_{12}$${\mathrm{Se}}_{60}$. The weak absorption tails observed below the exponential part of the edge also follow an exponential law, and they are not due to a light-scattering artifact. We associate them with localized states in the band gap. The results are interpreted in terms of a model in which optical transitions occur between localized states below the mobility edge and extended states of the opposite band.
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The electrical properties of liquid mercury
N. F. Mott · Philosophical magazine · 1966 · 371 citations