DOI: 10.1007/978-1-4020-8425-6_10
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Picosecond Carrier Dynamics in Narrow-Gap Semiconductors studied by Terahertz Radiation Pulses

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Cited by 7 publications
(4 citation statements)
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“…Previous monochromatic investigations of wide-bandgap compositions of Hg 1−x Cd x Te in the near-IR spectral range succeeded in extracting average collective relaxation times on the order of 0.5 to 2 ps (25). A spectrally integrated pump-probe study of a narrow-bandgap composition (x = 0.2) in the terahertz spectral range arrived at a similar conclusion (26).…”
Section: Introductionmentioning
confidence: 71%
“…Previous monochromatic investigations of wide-bandgap compositions of Hg 1−x Cd x Te in the near-IR spectral range succeeded in extracting average collective relaxation times on the order of 0.5 to 2 ps (25). A spectrally integrated pump-probe study of a narrow-bandgap composition (x = 0.2) in the terahertz spectral range arrived at a similar conclusion (26).…”
Section: Introductionmentioning
confidence: 71%
“…It must be noted that the free carrier influence on the THz generation strongly depends on their energy relaxation time. Thus in narrow band-gap semiconductors the THz generation is almost unaffected due to ∆t (ps) a relatively large electron mass during the first few picoseconds after the photoexcitation [20].…”
Section: Resultsmentioning
confidence: 99%
“…However, experiments have shown that average THz power radiated from the surfaces of InSb and Cd 1−x Hg x Te with x = 0, 0.2 and 0.3 is more than two orders of magnitude smaller than from the surface of InAs [143,148]. The reduced efficiency of THz emission from InSb was explained by photoexcited electron transfer to subsidiary conduction band L valleys with a large electron effective mass [143], whereas in the case of Cd 1−x Hg x Te the main reason for weak THz emission is, most probably, large non-parabolicity of the conduction band [149].…”
Section: Inas and Other Narrow-gap Semiconductorsmentioning
confidence: 98%