2007
DOI: 10.1021/nl070386c
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Photon Storage with Nanosecond Switching in Coupled Quantum Well Nanostructures

Abstract: Photon storage with nanosecond switching was implemented with indirect excitons in coupled quantum well nanostructures. The storage and release of photons was controlled by the gate voltage pulses. The nanosecond write and readout times were much shorter than the storage time, which reached microseconds. Furthermore, the presented control of excitons on a time scale much shorter than the exciton lifetime demonstrates the feasibility of studying excitons in in situ controlled electrostatic traps.

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Cited by 40 publications
(49 citation statements)
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“…3(a)] can be converted into IXs and stored in the EXAT source electrode. Alternatively, stored IXs can be reconverted to photons by selecting an appropriate source voltage to reduce the IX recombination lifetime [34]. The EXAT source can act, therefore, as a voltage-tunable location for photon-to-exciton interconversion as well as for IX storage.…”
Section: Acoustic Exciton Multiplexer-exammentioning
confidence: 99%
“…3(a)] can be converted into IXs and stored in the EXAT source electrode. Alternatively, stored IXs can be reconverted to photons by selecting an appropriate source voltage to reduce the IX recombination lifetime [34]. The EXAT source can act, therefore, as a voltage-tunable location for photon-to-exciton interconversion as well as for IX storage.…”
Section: Acoustic Exciton Multiplexer-exammentioning
confidence: 99%
“…This situation is equivalent to the case of exciton storage in coupled quantum wells. 25,26,48 Furthermore, virtually all of the tetrapods must have such trap sites since, at low excitation density, the relative fluorescence quenching tends towards 100% [ Fig. 1(c)].…”
Section: B the Role Of Localized Trap Statesmentioning
confidence: 99%
“…After a pump pulse creating 2D dipolar excitons in a QW they thermalize locally quite fast 12,13 . The excitons can then cool down to low temperatures 14 due to the interaction with the semiconductor lattice 15 , as their lifetime is sufficiently long 10,16 . Disorder (due to impurities and interface roughness) 17,18 , inevitably present in semiconductors, is screened by the interexcitonic interactions 19 and is usually weak in wide single QWs 10,20 .…”
Section: Introductionmentioning
confidence: 99%