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dc.contributor.authorCHYAN, YFen_US
dc.contributor.authorCHANG, CYen_US
dc.contributor.authorSZE, SMen_US
dc.contributor.authorLIN, MJen_US
dc.contributor.authorLIAO, Ken_US
dc.contributor.authorREIF, Ren_US
dc.date.accessioned2014-12-08T15:03:51Z-
dc.date.available2014-12-08T15:03:51Z-
dc.date.issued1994-08-01en_US
dc.identifier.issn0038-1101en_US
dc.identifier.urihttp://dx.doi.org/10.1016/0038-1101(94)90160-0en_US
dc.identifier.urihttp://hdl.handle.net/11536/2381-
dc.description.abstractWe derived an analytical model, focused on injected charge storage, for electron current density J(n), hole current density J(ps), current gain beta, and forward transit time tau(f), for heavily doped base and emitter with non-uniform band structures. This model can apply in high-level injection regions before the onset of the Kirk effect. By comparing with those results obtained from Sukuki's low-level injection model, it is observed that a new high-level injection term, proportional to the square of the hole current density, appears in the injected hole concentration in the polycrystalline silicon emitter and this term vanishes in the limit of low-level injection. As bias increases, J(n) and J(ps) of high-level injection model are less than those of the low-level injection model. In addition. for low-level injection model, beta, tau(f), the base transit time tau(b), the crystalline silicon emitter transit time tau(se), and the polycrystalline silicon emitter transit time tau(pe) keep constant for all injection region. However, for high-level injection model, beta and tau(b) decreases as bias increases, while tau(se) and tau(pe) increase with increasing bias. Tau(f) reaches a minimum and then increases. We conclude that the high-level injection model offers significant information for device operations at various electron current levels.en_US
dc.language.isoen_USen_US
dc.titleANALYTICAL MODELING OF POLYCRYSTALLINE SILICON EMITTER BIPOLAR-TRANSISTORS UNDER HIGH-LEVEL INJECTIONen_US
dc.typeArticleen_US
dc.identifier.doi10.1016/0038-1101(94)90160-0en_US
dc.identifier.journalSOLID-STATE ELECTRONICSen_US
dc.citation.volume37en_US
dc.citation.issue8en_US
dc.citation.spage1521en_US
dc.citation.epage1529en_US
dc.contributor.department電控工程研究所zh_TW
dc.contributor.departmentInstitute of Electrical and Control Engineeringen_US
dc.identifier.wosnumberWOS:A1994NN24900009-
dc.citation.woscount14-
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