完整後設資料紀錄
DC 欄位語言
dc.contributor.authorChang, TCen_US
dc.contributor.authorYeh, WKen_US
dc.contributor.authorMei, YJen_US
dc.contributor.authorTsai, WCen_US
dc.contributor.authorChen, YFen_US
dc.date.accessioned2019-04-02T05:58:28Z-
dc.date.available2019-04-02T05:58:28Z-
dc.date.issued1996-10-01en_US
dc.identifier.issn0306-8919en_US
dc.identifier.urihttp://dx.doi.org/10.1007/BF00326202en_US
dc.identifier.urihttp://hdl.handle.net/11536/149337-
dc.description.abstractOrdered (Ord-SL) and disordered (Dis-SL) Si-SiGe superlattices are grown using ultrahigh vacuum chemical vapour deposition (UHVCVD). The results of cross-sectional transmission electron microscopy (XTEM) and high-resolution double crystal x-ray diffraction (HRXRD) indicate that high quality Si-SiGe superlattices can be achieved. Well-defined band-edge excitonic luminescence is observed for the Si0.86Ge0.14-Si superlattice. Stronger phosoluminescence (PL) is observed for the Si-SiGe disordered superlattice compared with the corresponding Si-SiGe ordered superlattice. Furthermore, PL peak energy of the Dis-SL shifts to lower value with respect to the peak position of the corresponding Ord-SL. The stronger intensity of the no-phonon (NP) peak and the red shift of the PL peak are possibly a result of two probable mechanisms: (i) the tunnelling effect and (ii) the formation of localized states.en_US
dc.language.isoen_USen_US
dc.titlePhotoluminescence from ordered and disordered Si-SiGe superlatticesen_US
dc.typeArticleen_US
dc.identifier.doi10.1007/BF00326202en_US
dc.identifier.journalOPTICAL AND QUANTUM ELECTRONICSen_US
dc.citation.volume28en_US
dc.citation.spage1295en_US
dc.citation.epage1303en_US
dc.contributor.department電子工程學系及電子研究所zh_TW
dc.contributor.departmentDepartment of Electronics Engineering and Institute of Electronicsen_US
dc.identifier.wosnumberWOS:A1996VM79500009en_US
dc.citation.woscount0en_US
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