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Isotropic exciton effective mass and scattering by acoustic phonons

2 Isotropic exciton effective mass and scattering by acoustic phonons [Pg.415]

Using the Fermi s golden rule, the probabilities of absorption and emission of a phonon by the exciton system read [Pg.415]

At sufficiently low temperatures, when the thermal energy ksT is much smaller than the exciton bandwidth, most excitons at thermodynamic equilibrium are concentrated in the vicinity of the exciton band minimum in wavevector space. If this minimum corresponds to k = 0 and we assume for simplicity that the excitons have an isotropic effective mass m, we have [Pg.415]

Moreover, under these conditions the relation k a -C 1 (a is the lattice constant) is satisfied for the overhelming majority of excitons. [Pg.415]

The conservation of energy for the absorption and emission processes can now be written as [Pg.416]




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Acoustic phonon

Acoustic phonons

Acoustic scattering

By Mass

Effective phonons

Exciton

Exciton effects

Exciton/excitonic

Excitons

Excitons effective mass

Mass effects

Phonons scattering

Scattering effects

Scattering phonon

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