1981
DOI: 10.1016/0038-1098(81)90431-2
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Cooling of hot electron-hole plasmas in the presence of screened electron-phonon interactions

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Cited by 115 publications
(34 citation statements)
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“…Through the fitting process described above we can determine the electron and hole densities (their quasi-Fermi energies) and temperature as a function of time. We can therefore calculate the dynamic change in the average energy per carriers using the expression: [27][28][29]…”
Section: Carrier Thermalizationmentioning
confidence: 99%
“…Through the fitting process described above we can determine the electron and hole densities (their quasi-Fermi energies) and temperature as a function of time. We can therefore calculate the dynamic change in the average energy per carriers using the expression: [27][28][29]…”
Section: Carrier Thermalizationmentioning
confidence: 99%
“…the piezoelectric and deformation-potential interaction) is the main process for hot-carrier cooling. Although the rapid carrier cooling in the first few picoseconds suggested LO-phonon bottleneck [27,28] or carrier-LOphonon screening [29][30][31] may not be effective. It is possible that the fast decay of the LO-phonon leads to a nonequilibrium built up of the acoustic-phonon population (the LO-phonon lifetime was measured to be 4.5 ps at 20 K [32] and should be considerably smaller at room temperature).…”
Section: Resultsmentioning
confidence: 96%
“…The absence of a quasi-equilibrium is the result of a competition between radiative recombination and relaxation to the lower energy states. Since at this lattice temperature the average kinetic energy of the photoexcited carriers is low, the main relaxation processes correspond to carrier scatttering with acoustical phonons via both the piezoelectric interaction and the acoustical deformation potential [16]. Relaxation by emission of acoustical phonon is expected to be strongly reduced in the energy range of the localized states.…”
Section: Methodsmentioning
confidence: 99%