2009
DOI: 10.1103/physrevb.80.155331
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Kinetics of the inner ring in the exciton emission pattern in coupled GaAs quantum wells

Abstract: We report on the kinetics of the inner ring in the exciton emission pattern. The formation time of the inner ring following the onset of the laser excitation is found to be about 30 ns. The inner ring was also found to disappear within 4 ns after the laser termination. The latter process is accompanied by a jump in the photoluminescence (PL) intensity. The spatial dependence of the PL-jump indicates that the excitons outside of the region of laser excitation, including the inner ring region, are efficiently co… Show more

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Cited by 49 publications
(122 citation statements)
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“…The photoexcited electrons recombine within the inner ring [42,43]. Therefore, in the area of external and LBS rings with no photoexcited electrons coherence forms spontaneously; it is not affected by coherence of the optical pumping.…”
Section: Methodsmentioning
confidence: 99%
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“…The photoexcited electrons recombine within the inner ring [42,43]. Therefore, in the area of external and LBS rings with no photoexcited electrons coherence forms spontaneously; it is not affected by coherence of the optical pumping.…”
Section: Methodsmentioning
confidence: 99%
“…In this work, the area of study is beyond the inner ring, which is formed by indirect excitons traveling away from the optical excitation spot [37,42,43]. The photoexcited electrons recombine within the inner ring [42,43].…”
Section: Methodsmentioning
confidence: 99%
“…7,9,17,18,26,28,29 For a strong laser excitation, the density of generated excitons is high so that they can effectively screen the disorder potential, delocalize, and travel and cool to the lattice temperature outside the laser excitation spot thus forming the inner ring. 7,9,17,18,26,28,29 Figures 1 The external ring can also be seen beyond the inner ring; the external ring radius (that is the distance to the excitation line for the studied case of line excitation) quickly increases with the excitation power. E pump = E probe = 1960 meV.…”
Section: A Experimentsmentioning
confidence: 99%
“…10,13,24,27 A set of exciton transport phenomena was observed, including the transistor effect for excitons, 14,15,19,21 localizationdelocalization transition in random potentials 7,9,10,13,17,22 and in static and moving lattices, 18,23,29 and the inner ring in emission patterns. 7,9,17,18,26,28,29,32 The studies of the latter form the subject of this work.…”
Section: Introductionmentioning
confidence: 99%
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