Time-dependent theory of hot electrons using the discrete Boltzmann equation

G. S. Canright and G. D. Mahan
Phys. Rev. B 36, 1025 – Published 15 July 1987
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Abstract

The discrete Boltzmann equation may be applied to the time evolution of the electron distribution for spatially homogeneous systems in which optical-phonon scattering is dominant. We describe the time-dependent solution for both pulsed and steady excitation (e.g., via photoexcitation). The results for the latter case may be compared with experimental hot-electron luminescence spectra under steady photoexcitation. The agreement is generally good, but sensitive in detail to the method used to calculate recombination rates.

  • Received 6 February 1987

DOI:https://doi.org/10.1103/PhysRevB.36.1025

©1987 American Physical Society

Authors & Affiliations

G. S. Canright and G. D. Mahan

  • Solid State Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37830 and Department of Physics, The University of Tennessee, Knoxville, Tennessee 37996

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Issue

Vol. 36, Iss. 2 — 15 July 1987

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