Please use this identifier to cite or link to this item: https://doi.org/10.1109/16.737470
DC FieldValue
dc.titleA Modified Lucky Electron Model for Impact lonization Rate in NMOSFET's at 77 K
dc.contributor.authorLing, C.H.
dc.contributor.authorSee, L.K.
dc.date.accessioned2014-10-07T02:55:44Z
dc.date.available2014-10-07T02:55:44Z
dc.date.issued1999
dc.identifier.citationLing, C.H., See, L.K. (1999). A Modified Lucky Electron Model for Impact lonization Rate in NMOSFET's at 77 K. IEEE Transactions on Electron Devices 46 (1) : 263-266. ScholarBank@NUS Repository. https://doi.org/10.1109/16.737470
dc.identifier.issn00189383
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/80275
dc.description.abstractThe nonstationary effects of electrons at 77 K, in the highfield saturation region of the MOSFET, are modeled by incorporating an appropriate electron temperature decrease (-ATe) to the carrier energy, within the framework of a modified lucky electron model. For a thin oxide MOSFET (Tox = 5 nm, Lg = 0.5 μm), ATe is a function of the electric field in the saturation region, and increases rapidly with drain bias. However, for a thick oxide MOSFET (Tox = 12.5 nm, Lg = 5 μm), ATe = 280 K is found to adequately describe the impact ionization rate. Our model also explains the crossover of the ionization rates in the thick oxide MOSFET at 77 K and 300 K. © 1999 IEEE.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1109/16.737470
dc.sourceScopus
dc.subjectImpact ionization rate
dc.subjectLow temperature
dc.subjectMosfet's
dc.subjectNonstationary effects
dc.typeArticle
dc.contributor.departmentELECTRICAL ENGINEERING
dc.description.doi10.1109/16.737470
dc.description.sourcetitleIEEE Transactions on Electron Devices
dc.description.volume46
dc.description.issue1
dc.description.page263-266
dc.description.codenIETDA
dc.identifier.isiut000077769000037
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