1970
DOI: 10.1016/0375-9601(70)90066-6
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The scattering of long wavelength phonons by current carriers in INSB

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Cited by 14 publications
(9 citation statements)
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“…As was shown experimentally in [20], the intense phonon scattering in this type of crystals is not caused by impurities or imperfections of the lattice but is rather due to charge carriers which a t p > lo1' ~m -~ can be regarded as free ones [18] in the temperature range under investigation. I n this kind of crystals the effective mass of charge carriers (holes) is large, and the mechanism of phonon scattering by charge carriers (11) plays the decisive role accounting for great differences in the phonon thermal conductivity of n-and p-InSb revealed by the experiments.…”
Section: Indium Antimonide Of P-typementioning
confidence: 95%
“…As was shown experimentally in [20], the intense phonon scattering in this type of crystals is not caused by impurities or imperfections of the lattice but is rather due to charge carriers which a t p > lo1' ~m -~ can be regarded as free ones [18] in the temperature range under investigation. I n this kind of crystals the effective mass of charge carriers (holes) is large, and the mechanism of phonon scattering by charge carriers (11) plays the decisive role accounting for great differences in the phonon thermal conductivity of n-and p-InSb revealed by the experiments.…”
Section: Indium Antimonide Of P-typementioning
confidence: 95%
“…The calculated κ natural given by the different lattice constants for each indium-V compound are compared in Figure 7. Figure 7 shows the calculated κ L vs. temperature for the indium-V compounds with experimental data for InP (black circles [59], squares [60], diamond [61], and triangle [62]), InAs (red circles [63], squares [64], diamond [65], and triangles [66]), and InSb (blue circles [56], squares [67], and triangles [68]). The isotope effect is small in the indium-V compounds so we show only the calculated κ natural in Figure 7.…”
Section: Indium-v Compoundsmentioning
confidence: 99%
“…Experimental data is shown for κ L of GaSb (black circles [56]), GaAs (green circles [47] and green triangles [48]), and GaP (red circles [51] and red triangles [52]). InP (black circles [59], squares [60], diamond [61], and triangle [62]), InAs (red circles [63], squares [64], diamond [65], and triangles [66]), and InSb (blue circles [56], squares [67], and triangles [68]). The dashed black curve corresponds to κ natural for InP with harmonic and anharmonic IFCs determined using the lattice constant from energy minimization, a InP =5.79Å.…”
Section: Figure Captionsmentioning
confidence: 99%
“…The same conclusion was reached thanks to a detailed study of the heat conductivity in InSb as a function of the doping and of the compensation [35]. This consideration will be of primary importance in further measurements to follow, where the T pulses will serve as calibrators of the heat-pulse signals.…”
mentioning
confidence: 61%
“…Let us remark that in heat-conductivity measurements, where the mean phonon frequency is tuned by varying the temperature, the Fermi-surface cut-off does not usually show [35], except, to a certain extent, in heavily doped p-type samples [37]. Here Fig.…”
mentioning
confidence: 99%