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Oxide thickness dependence of plasma charging damage

dc.citation.epage364en_US
dc.citation.issue3en_US
dc.citation.spage357en_US
dc.citation.volume39en_US
dc.citation.woscount1
dc.contributor.authorLin, HCen_US
dc.contributor.authorChen, CCen_US
dc.contributor.authorWang, MFen_US
dc.contributor.authorHsien, SKen_US
dc.contributor.authorChien, CHen_US
dc.contributor.authorHuang, TYen_US
dc.contributor.authorChang, CYen_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.date.accessioned2014-12-08T15:46:47Z
dc.date.available2014-12-08T15:46:47Z
dc.date.issued1999-03-01en_US
dc.description.abstractCharging damage induced in oxides with thickness ranging from 8.7 to 2.5 nm is investigated. Results of charge-to-breakdown (Q(bd)) measurements performed on control devices indicate that the polarity dependence increases with decreasing oxide thickness at both room and elevated temperature (180 degrees C) conditions. As the oxide thickness is thinned down below 3nm, the Q(bd) becomes very sensitive to the stressing current density and temperature. Experimental results show that severe antenna effect would occur during plasma ashing treatment in devices with gate oxides as thin as 2.6 nm. It is concluded that high stressing current level, negative plasma charging, and high process temperature are key factors responsible for the damage. (C) 1999 Elsevier Science Ltd. All rights reserved.en_US
dc.identifier.doi10.1016/S0026-2714(98)00247-9en_US
dc.identifier.issn0026-2714en_US
dc.identifier.journalMICROELECTRONICS RELIABILITYen_US
dc.identifier.urihttp://dx.doi.org/10.1016/S0026-2714(98)00247-9en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/31471
dc.identifier.wosnumberWOS:000080890200005
dc.language.isoen_USen_US
dc.titleOxide thickness dependence of plasma charging damageen_US
dc.typeArticleen_US

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