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dc.contributor.authorDyksik, M.
dc.contributor.authorMotyka, M.
dc.contributor.authorWeih, R.
dc.contributor.authorHöfling, S.
dc.contributor.authorKamp, M.
dc.contributor.authorSęk, G.
dc.contributor.authorMisiewicz, J.
dc.date.accessioned2017-01-25T10:30:14Z
dc.date.available2017-01-25T10:30:14Z
dc.date.issued2017-02
dc.identifier249000207
dc.identifiercd5721a0-48b1-4875-ab11-b1122dd3c7be
dc.identifier85009781784
dc.identifier000394357200013
dc.identifier.citationDyksik , M , Motyka , M , Weih , R , Höfling , S , Kamp , M , Sęk , G & Misiewicz , J 2017 , ' Carrier transfer between confined and localized states in type II InAs/GaAsSb quantum wells ' , Optical and Quantum Electronics , vol. 49 , no. 2 , 59 . https://doi.org/10.1007/s11082-017-0891-0en
dc.identifier.issn1572-817X
dc.identifier.otherBibtex: urn:416655387eb811fa28264f809839e94d
dc.identifier.urihttps://hdl.handle.net/10023/10168
dc.descriptionThe work has been supported from iCspec project, which received funding from the European Commission’s Horizon 2020 Research and Innovation Programme under grant agreement No. 636930, and also by the National Science Centre of Poland within Grant No. 2014/15/B/ST7/04663.en
dc.description.abstractTemperature-resolved photoluminescence studies were performed on tensely-strained AlSb/InAs/GaAsSb W-shaped type II quantum wells. They revealed two emission bands: one at lower energy of localized origin resulting from carrier trapping states at interfaces and dominates at low-temperature; and one corresponding to the fundamental optical transition in the type II quantum well. With the temperature increase to 170—200 K the low-energy emission is quenched and the high-energy band dominates and its intensity increases, indicating carrier transfer processes between the respective states at elevated temperatures. In addition, the integrated photoluminescence intensity was measured as a function of excitation power. At high excitation regime the emission intensity of the low-energy emission band saturated, indicating low density of states, thus confirming its localized nature. The depth of the localization potential at the InAs/GaAsSb interface was determined to be 13—15 meV.
dc.format.extent8
dc.format.extent704418
dc.language.isoeng
dc.relation.ispartofOptical and Quantum Electronicsen
dc.subjectFourier-transform infrared spectroscopyen
dc.subjectType II quantum wellsen
dc.subjectPhotoluminescence quenchingen
dc.subjectCarrier transferen
dc.subjectLocalized statesen
dc.subjectQC Physicsen
dc.subjectNDASen
dc.subject.lccQCen
dc.titleCarrier transfer between confined and localized states in type II InAs/GaAsSb quantum wellsen
dc.typeJournal articleen
dc.contributor.institutionUniversity of St Andrews. School of Physics and Astronomyen
dc.contributor.institutionUniversity of St Andrews. Condensed Matter Physicsen
dc.identifier.doi10.1007/s11082-017-0891-0
dc.description.statusPeer revieweden


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