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dc.contributor.authorLow, Ten_US
dc.contributor.authorLi, MFen_US
dc.contributor.authorShen, Cen_US
dc.contributor.authorYeo, YCen_US
dc.contributor.authorHou, YTen_US
dc.contributor.authorZhu, CXen_US
dc.contributor.authorChin, Aen_US
dc.contributor.authorKwong, DLen_US
dc.date.accessioned2014-12-08T15:38:31Z-
dc.date.available2014-12-08T15:38:31Z-
dc.date.issued2004-09-20en_US
dc.identifier.issn0003-6951en_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.1788888en_US
dc.identifier.urihttp://hdl.handle.net/11536/26372-
dc.description.abstractElectron mobility in strained silicon and various surface oriented germanium ultrathin-body (UTB) metal-oxide semiconductor field-effect transistors (MOSFETs) with sub-10-nm-body thickness are systematically studied. For biaxial tensile strained-Si UTB MOSFETs, strain effects offer mobility enhancement down to a body thickness of 3 nm, below which strong quantum confinement effect renders further valley splitting via application of strain redundant. For Ge channel UTB MOSFETs, electron mobility is found to be highly dependent on surface orientation. Ge<100> and Ge<110> surfaces have low quantization mass that leads to a lower mobility than that of Si in aggressively scaled UTB MOSFETs. (C) 2004 American Institute of Physics.en_US
dc.language.isoen_USen_US
dc.titleElectron mobility in Ge and strained-Si channel ultrathin-body metal-oxide semi conductor field-effect transistorsen_US
dc.typeArticleen_US
dc.identifier.doi10.1063/1.1788888en_US
dc.identifier.journalAPPLIED PHYSICS LETTERSen_US
dc.citation.volume85en_US
dc.citation.issue12en_US
dc.citation.spage2402en_US
dc.citation.epage2404en_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:000224145300083-
dc.citation.woscount16-
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