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dc.contributor.authorFENG, MSen_US
dc.contributor.authorFANG, CSAen_US
dc.contributor.authorCHEN, HDen_US
dc.date.accessioned2014-12-08T15:03:04Z-
dc.date.available2014-12-08T15:03:04Z-
dc.date.issued1995-11-15en_US
dc.identifier.issn0254-0584en_US
dc.identifier.urihttp://hdl.handle.net/11536/1650-
dc.description.abstractPhotoluminescence characteristics of heavily carbon-, beryllium- and zinc-doped GaAs were studied in this investigation. The band-to-acceptor (e,A) transition was identified via various doping concentrations from 10(17) to 10(20) cm(-3) and the temperature from 20 to 300 K. As a result the (e,A) peak was found to be a dominant peak at 20 K instead of the band-to-band (B,B) peak at p> 1 x 10(19) cm(-3). The (e,A) peak was also observed at 300 K and enhanced with the increasing carrier concentration at p> 2.8 x 10(18) cm(-3). Bandgap shrinkage of these samples was qualitatively obtained. When p> 1 x 10(19) cm(-3), the impurity band merges with the valence band and the binding energy of the acceptor is equal to zero. Consequently, the bandgap can be taken as the energy between the conduction-band minimum and the top of the impurity band.en_US
dc.language.isoen_USen_US
dc.subjectPHOTOLUMINESCENCEen_US
dc.subjectSPECTROSCOPYen_US
dc.subjectBANDGAP SHRINKAGEen_US
dc.subjectGAASen_US
dc.titleBANDGAP SHRINKAGE OF DEGENERATE P-TYPE GAAS BY PHOTOLUMINESCENCE SPECTROSCOPYen_US
dc.typeArticleen_US
dc.identifier.journalMATERIALS CHEMISTRY AND PHYSICSen_US
dc.citation.volume42en_US
dc.citation.issue2en_US
dc.citation.spage143en_US
dc.citation.epage147en_US
dc.contributor.department材料科學與工程學系zh_TW
dc.contributor.department電控工程研究所zh_TW
dc.contributor.departmentDepartment of Materials Science and Engineeringen_US
dc.contributor.departmentInstitute of Electrical and Control Engineeringen_US
dc.identifier.wosnumberWOS:A1995TB85700011-
dc.citation.woscount3-
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