Electron-phonon coupling in semiconductors at high electronic temperatures
arXiv:2307.13554 · doi:10.1103/PhysRevB.108.144305
Abstract
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 ~25,000 K. 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 potential 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 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.
References in corpus (8)
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- Stainless steel in an electronically excited state
- Ultrafast X-ray interaction with photovoltaic materials: Thermal and nonthermal responses