Electron-phonon coupling in semiconductors at high electronic temperatures

被引:2
|
作者
Medvedev N. [1 ,2 ]
机构
[1] Institute of Physics, Czech Academy of Sciences, Na Slovance 2, Prague, 182 21
[2] Institute of Plasma Physics, Czech Academy of Sciences, Za Slovankou 3, Prague 8
关键词
Aluminum compounds - Boltzmann equation - Distribution functions - Electrons - Gallium arsenide - II-VI semiconductors - Layered semiconductors - Molecular dynamics - Phonons - Silicon carbide - Titanium dioxide - Wide band gap semiconductors - Zinc oxide - Zinc sulfide;
D O I
10.1103/PhysRevB.108.144305
中图分类号
学科分类号
摘要
A nonperturbative dynamical coupling approach based on tight-binding molecular dynamics is used to evaluate the electron-ion (electron-phonon) coupling parameter in irradiated semiconductors as a function of the electronic temperature up to ∼25000K. The method accounts for arbitrary electronic distribution function via the Boltzmann equation, enabling a comparative analysis of various models: fully equilibrium electronic distribution, band-resolved local equilibria (distinct temperatures and chemical potentials of electrons in the valence and the conduction band), and a full nonequilibrium distribution. It is demonstrated that the nonequilibrium produces the electron-phonon coupling parameter different by at most ∼35% from its equilibrium counterpart for identical deposited energy density, allowing us to use the coupling parameter as a function of the single electronic equivalent (or kinetic) temperature. The following 14 semiconductors are studied here: group IV: Si, Ge, SiC; group III-V: AlAs, AlP, GaP, GaAs, GaSb; oxides: ZnO, TiO2, Cu2O; layered PbI2; ZnS and B4C. © 2023 American Physical Society.
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