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dc.contributor.authorBarman, B.en_US
dc.contributor.authorTsai, Y.en_US
dc.contributor.authorScrace, T.en_US
dc.contributor.authorMurphy, J. R.en_US
dc.contributor.authorCartwright, A. N.en_US
dc.contributor.authorPientka, J. M.en_US
dc.contributor.authorZutic, I.en_US
dc.contributor.authorMcCombe, B. D.en_US
dc.contributor.authorPetrou, A.en_US
dc.contributor.authorSellers, I. R.en_US
dc.contributor.authorOszwaldowski, R.en_US
dc.contributor.authorPetukhov, A.en_US
dc.contributor.authorFan, W. C.en_US
dc.contributor.authorChou, W. C.en_US
dc.contributor.authorYang, C. S.en_US
dc.date.accessioned2019-04-03T06:47:36Z-
dc.date.available2019-04-03T06:47:36Z-
dc.date.issued2014-01-01en_US
dc.identifier.isbn978-1-62841-194-2en_US
dc.identifier.issn0277-786Xen_US
dc.identifier.urihttp://dx.doi.org/10.1117/12.2064339en_US
dc.identifier.urihttp://hdl.handle.net/11536/135274-
dc.description.abstractWe used time resolved photoluminescence (TRPL) spectroscopy to compare the properties of magnetic polarons in two related, spatially indirect, II-VI epitaxially grown quantum dot systems. In sample A (ZnMnTe/ZnSe), the photoexcited holes are confined in the magnetic ZnMnTe quantum dots (QDs), while the electrons remain in the surrounding non-magnetic ZnSe matrix. In sample B (ZnTe/ZnMnSe) on the other hand, the holes are confined in the non-magnetic ZnTe QDs and the electrons move in the magnetic ZnMnSe matrix. The magnetic polaron formation energies, E-MP, in these samples were measured from the temporal red-shift of the excitonic emission peak. The magnetic polarons in the two samples exhibit distinct characteristics. In sample A, the magnetic polaron is strongly bound with E-MP = 35 meV. Furthermore, E-MP has unconventionally weak dependence of on both temperature T and magnetic field B-appl. In contrast, magnetic polarons in sample B show conventional characteristics with E-MP decreasing with increasing temperature and increasing external magnetic field. We attribute the difference in magnetic polaron properties between the two types of QDs to the difference in the location of the Mn ions in the respective structures.en_US
dc.language.isoen_USen_US
dc.subjectmagnetic quantum dotsen_US
dc.subjectmagnetic polaron dynamicsen_US
dc.subjectexchange interactionen_US
dc.titleConventional vs Unconventional Magnetic Polarons: ZnMnTe/ZnSe and ZnTe/ZnMnSe Quantum Dotsen_US
dc.typeProceedings Paperen_US
dc.identifier.doi10.1117/12.2064339en_US
dc.identifier.journalSPINTRONICS VIIen_US
dc.citation.volume9167en_US
dc.citation.spage0en_US
dc.citation.epage0en_US
dc.contributor.department交大名義發表zh_TW
dc.contributor.departmentNational Chiao Tung Universityen_US
dc.identifier.wosnumberWOS:000343860800014en_US
dc.citation.woscount0en_US
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