1969
DOI: 10.1103/physrev.182.802
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Carrier-Concentration Dependence of Electron-Phonon Scattering in Te-Doped GaSb at Low Temperature

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Cited by 36 publications
(18 citation statements)
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“…In undoped films, τ D1 is associated with electron-LO-phonon interactions (τ e-LO = 1.68 ps), which remains unchanged with the pump power (with n), thus reflecting the fact that the rate of polar Fröhlich electron-LO-phonon interaction (1/τ e-LO ) is independent of the carrier density [4]. One exception can occur for a degenerate electron gas in heavily doped semiconductors due to the energy band nonparabolicity, which mainly appears in low-temperature measurements [28]. In contrast, τ R in undoped samples is associated with electron-electron interactions and hence slightly decreases with increasing n (figure 3) since the electron-electron scattering rate (1/τ R ) varies with carrier density as n 2/3 and as n in 3D and 2D structures, respectively [29].…”
Section: Resultsmentioning
confidence: 97%
“…In undoped films, τ D1 is associated with electron-LO-phonon interactions (τ e-LO = 1.68 ps), which remains unchanged with the pump power (with n), thus reflecting the fact that the rate of polar Fröhlich electron-LO-phonon interaction (1/τ e-LO ) is independent of the carrier density [4]. One exception can occur for a degenerate electron gas in heavily doped semiconductors due to the energy band nonparabolicity, which mainly appears in low-temperature measurements [28]. In contrast, τ R in undoped samples is associated with electron-electron interactions and hence slightly decreases with increasing n (figure 3) since the electron-electron scattering rate (1/τ R ) varies with carrier density as n 2/3 and as n in 3D and 2D structures, respectively [29].…”
Section: Resultsmentioning
confidence: 97%
“…The classical treatment of this problem in semiconductors was provided by Ziman [3,14,15], where simplified models for the phonon dispersion, the electronic structure, and the interaction matrix elements were used for a closed-form analytic formula with limited accuracy and applicability (only valid at low temperatures in degenerate semiconductors). Ensuing experiments in semiconductors also suffered from the difficulty of separating the EPI from other scattering mechanisms of phonons, and thus remained qualitative and/ or limited to very low temperatures [16][17][18][19][20][21][22][23][24][25][26][27][28]. Again the common wisdom was that the EPI would only be important on the phonon transport at low temperatures, partly due to the fact that most of the studies analyzed samples with carrier concentrations below 10 18 cm −3 .…”
mentioning
confidence: 99%
“…Another interesting perspective, which goes beyond the scope of this work, concerns the investigation of the impact of a modified interaction with phonons induced by collective effects on the thermal conductivity of the doped semiconductor. Indeed it has been shown experimentally and theoretically that electron-phonon interaction can modify both the electronic and lattice contribution to the thermal conductivity [34,35].…”
Section: Discussionmentioning
confidence: 99%