Please use this identifier to cite or link to this item: https://doi.org/10.1109/16.853038
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dc.titleA thorough study of quasi-breakdown phenomenon of thin gate oxide in dual-gate CMOSFET's
dc.contributor.authorGuan, H.
dc.contributor.authorLi, M.-F.
dc.contributor.authorHe, Y.
dc.contributor.authorCho, B.J.
dc.contributor.authorDong, Z.
dc.date.accessioned2014-10-07T02:55:49Z
dc.date.available2014-10-07T02:55:49Z
dc.date.issued2000-08
dc.identifier.citationGuan, H.,Li, M.-F.,He, Y.,Cho, B.J.,Dong, Z. (2000-08). A thorough study of quasi-breakdown phenomenon of thin gate oxide in dual-gate CMOSFET's. IEEE Transactions on Electron Devices 47 (8) : 1608-1616. ScholarBank@NUS Repository. <a href="https://doi.org/10.1109/16.853038" target="_blank">https://doi.org/10.1109/16.853038</a>
dc.identifier.issn00189383
dc.identifier.urihttp://scholarbank.nus.edu.sg/handle/10635/80283
dc.description.abstractThe conduction mechanism of quasibreakdown (QB) mode for thin gate oxide has been studied in dual-gate CMOSFET with a 3.7-nm thick gate oxide. Systematic carrier separation experiments were conducted to investigate the evolutions of gate, source/drain, and substrate currents before and after gate oxide quasibreakdown (QB). Our experimental results clearly show that QB is due to the formation of a local physically-damaged-region (LPDR) at Si/SiO 2 interface [1]. At this region, the effective oxide thickness is reduced to the direct tunneling (DT) regime. The observed high gate leakage current is due to DT electron or hole currents [14] through the region where the LPDR is generated. Twelve V g, I sub, I s/d versus time curves and forty eight I-V curves of carrier separation measurements have been demonstrated. All curves can be explained in a unified way by the LPDR QB model and the proper interpretation of the carrier separation measurements. Particularly, under substrate injection stress condition, there is several orders of magnitude increase of I sub(I s/d) at the onset point of QB for n(p) - MOSFET, which mainly corresponds to valence electrons DT from the substrate to the gate. Consequently, cold holes are left in the substrate and measured as substrate current. These cold holes have no contribution to the oxide breakdown and thus the lifetime of oxide after QB is very long. Under gate injection stress condition, there is sudden drop and even change of sign of I sub(I s/d) at the onset point of QB for n(p)-MOSFET, which corresponds to the disappearance of impact ionization and the appearance of hole DT current from the substrate to the gate. © 2000 IEEE.
dc.description.urihttp://libproxy1.nus.edu.sg/login?url=http://dx.doi.org/10.1109/16.853038
dc.sourceScopus
dc.subjectDirect tunneling
dc.subjectMOS devices
dc.subjectOxide breakdown
dc.typeArticle
dc.contributor.departmentELECTRICAL ENGINEERING
dc.description.doi10.1109/16.853038
dc.description.sourcetitleIEEE Transactions on Electron Devices
dc.description.volume47
dc.description.issue8
dc.description.page1608-1616
dc.description.codenIETDA
dc.identifier.isiutNOT_IN_WOS
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