1984
DOI: 10.1016/0375-9601(84)90220-2
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Electron energy relaxation due to 2TA phonons in n-GaAs and n-InP

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Cited by 4 publications
(2 citation statements)
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“…So we have used in our calculations a value of 19.4 meV for the 2TA phonon energy and for p a value of 0.5. The two-phonon deformation potential parameter D was varied to obtain the best fit with the data in the temperature range 20 K < T e < 40 K. The value so obtained D = 2.0 × 10 3 eV may be compared with the value of 3.0 × 10 3 eV used in explaining the energy relaxation time data in bulk n-GaAs [23]. Any uncertainty about the p value only alters the fitted D value as these two quantities enter the energy loss expression in the form D p 1/2 .…”
Section: Resultsmentioning
confidence: 99%
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“…So we have used in our calculations a value of 19.4 meV for the 2TA phonon energy and for p a value of 0.5. The two-phonon deformation potential parameter D was varied to obtain the best fit with the data in the temperature range 20 K < T e < 40 K. The value so obtained D = 2.0 × 10 3 eV may be compared with the value of 3.0 × 10 3 eV used in explaining the energy relaxation time data in bulk n-GaAs [23]. Any uncertainty about the p value only alters the fitted D value as these two quantities enter the energy loss expression in the form D p 1/2 .…”
Section: Resultsmentioning
confidence: 99%
“…Ganguly and Ngai [21] have formulated an effective Hamiltonian for the interaction between electrons and two-phonons. Employing this formalism the energy loss rates are satisfactorily explained in InSb [22], GaAs [23] by Kubakaddi and co-workers and in GaSb [19] by Obditsch and Kahlert. Free carrier absorption in InSb [21] and mobility in Si [11] are also explained employing electron scattering by two-phonons.…”
Section: Two-phonon Processes In Bulk Semiconductorsmentioning
confidence: 92%