Photon Absorption Models in Nanostructured Semiconductor Solar Cells and Devices by Antonio Luque & Alexander Virgil Mellor

Author:Antonio Luque & Alexander Virgil Mellor
Language: eng
Format: epub
Publisher: Springer International Publishing, Cham

(3.42)

where E BScb is the energy of the cb bound state, which is negative for the cases in study (as well as ) and is not further developed. Contrarily, we fully develop the energy of the initial VB bound state, which may belong to the hh or to the lh bands (so states have too low energy as to give E line within the host bandgap). The initial-state k components have discrete permitted values, and they are labeled with their correspondent nx, ny, nz quantum numbers.

When the wavefunction is extended in one of its variables, E line is denoted in a more informative way: the subscript includes the extended variables outside the bracket and the QNs of the bound parts inside the bracket. According to this nomenclature, and taking into account the energy-wavevector relationship for extended states of Eq. (2.​41), these equations are

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