1987
DOI: 10.1103/physrevlett.59.696
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Time-resolved Raman scattering in GaAs quantum wells

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Cited by 220 publications
(42 citation statements)
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“…It was therefore thought that there is a considerable advantage in working in this frequency range since LO phonon emission-which represents the competing non-radiative loss mechanism-should be eliminated. However, recent experimental work on wide quantum wells has yielded a range of intersubband lifetimes, from 200 ps ͑characteristic of the acoustic phonon scattering regime͒ 2 to approximately 1 ps ͑implying incomplete suppression of LO phonon scattering͒. 3 Determination of intersubband lifetimes is therefore an important aspect in the successful design of both a terahertz emitter and a laser.…”
Section: Introductionmentioning
confidence: 99%
“…It was therefore thought that there is a considerable advantage in working in this frequency range since LO phonon emission-which represents the competing non-radiative loss mechanism-should be eliminated. However, recent experimental work on wide quantum wells has yielded a range of intersubband lifetimes, from 200 ps ͑characteristic of the acoustic phonon scattering regime͒ 2 to approximately 1 ps ͑implying incomplete suppression of LO phonon scattering͒. 3 Determination of intersubband lifetimes is therefore an important aspect in the successful design of both a terahertz emitter and a laser.…”
Section: Introductionmentioning
confidence: 99%
“…As the well width decreases the effect of the MQW potential on the zone-folded acoustic phonon modes enhances and leads to an increase of the acoustic-phonon contribution to the intra-impurity scattering rate. For intersubband scattering of electrons in the GaAs MQWs, the acoustic-phonon contribution to the intersubband scattering rate is inversely proportional to the square of the well width [10]. A similar dependence of the overlap between the localized impurity states and the acoustic phonon modes could also explain the monotonically decreasing 2p excited state lifetime with well width.…”
Section: Resultsmentioning
confidence: 95%
“…This is a consequence of the quenching of the LO-phonon emission when the ISB transition energy is below the LO-phonon energy, which is well documented, for example, in GaAs/ AlGaAs QWs. [23][24][25][26][27] This huge increase of the ISB relaxation time opens great prospects for efficient nitride ISB devices at long wavelengths.…”
Section: ͑9͒mentioning
confidence: 99%
“…Typical ISB relaxation times in GaAs quantum wells range from ϳ0.3-2 ps for mid-infrared transitions ͑LO-phonon emission͒ to ϳ100-400 ps for far-infrared transitions ͑acoustic phonon emission͒. [23][24][25][26][27] GaN, with a LOphonon energy E LO = 92 meV compared with 36 meV for GaAs, opens interesting opportunities in this context. Nowadays the maturity of the plasma-assisted molecular-beam epitaxy ͑PAMBE͒ of GaN / AlGaN heterostructures renders feasible the realization of band-engineered structures required to observe and exploit these ISB effects.…”
Section: Introductionmentioning
confidence: 98%