1998
DOI: 10.1002/(sici)1521-3951(199812)210:2<873::aid-pssb873>3.0.co;2-5
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Resonant States in Strained Semiconductors

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Cited by 12 publications
(13 citation statements)
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“…17, 18 However, if a resonant state exists with energy less than ប 0 , then under an applied electric field a carrier will charge the resonant state before its energy reaches ប 0 . In our earlier letter 5 we have proved that such process provides a new mechanism of carrier population inversion, which explains the origin of far-infrared lasing from strained p-Ge. 4 The detailed analysis, which was not given in Ref.…”
Section: Kinetics Of Resonant Statesmentioning
confidence: 81%
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“…17, 18 However, if a resonant state exists with energy less than ប 0 , then under an applied electric field a carrier will charge the resonant state before its energy reaches ប 0 . In our earlier letter 5 we have proved that such process provides a new mechanism of carrier population inversion, which explains the origin of far-infrared lasing from strained p-Ge. 4 The detailed analysis, which was not given in Ref.…”
Section: Kinetics Of Resonant Statesmentioning
confidence: 81%
“…We will first outline briefly the model studied in Ref. 5. It includes a drain D at E k ϭប 0 , which describes the process of removal of holes in the energy region E k уប 0 due to emission of optical phonons, and a source S at small k within the energy interval between zero and ⑀ 0 Ӷប 0 , which presents the generation of holes removed by drain.…”
Section: Kinetics Of Resonant Statesmentioning
confidence: 99%
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“…We will demonstrate in quantitative details that our suggested mechanism is realistic. Based on a uniaxially strained p-Ge in which shallow acceptors induce resonant states [4,5], a terahertz laser has been fabricated recently [6], and the radiation emission is due to optical transitions between the resonant states and the localized acceptor (Ga) states. Up to now, the mechanism of lasing has remained a puzzle.…”
mentioning
confidence: 99%
“…In p-Ge, t r is shorter than t k , and t r ഠ 2 3 10 26 s [5]. The value ofh͞G was obtained earlier [4,5] ash͞G ഠ 2 3 10 213 s, and our numerical calculation (shown later) gives the transient time t E ഠ 10 211 s for reaching stationary nonequilibrium distribution. Thus, the necessary condition for lasing is satisfied, and we neglect the radiation transition processes in the kinetic equations for f k and for the population of the impurity state f r .…”
mentioning
confidence: 99%