Low-frequency noise in n-channel metal-oxide-semiconductor field-effect transistors undergoing soft breakdown

dc.citation.epage653en_US
dc.citation.issue1en_US
dc.citation.spage648en_US
dc.citation.volume89en_US
dc.citation.woscount7
dc.contributor.authorChen, MJen_US
dc.contributor.authorKang, TKen_US
dc.contributor.authorLee, YHen_US
dc.contributor.authorLiu, CHen_US
dc.contributor.authorChang, YJen_US
dc.contributor.authorFu, KYen_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.accessioned2014-12-08T15:44:25Z
dc.date.available2014-12-08T15:44:25Z
dc.date.issued2001-01-01en_US
dc.description.abstractFor 3.3-nm thick gate oxide n-channel metal-oxide-semiconductor field-effect transistors subject to a stress gate voltage of 5.5 V, three distinct events are encountered in the time evolution of the gate current: stress-induced leakage current (SILC), soft breakdown (SBD), and hard breakdown (HBD). The localization of SBD and HBD paths, as well as their developments with the time, is determined electrically, showing random distribution in nature. At several stress times, we interrupt the stressing to measure the drain current low-frequency noise power S-id. As expected, S-id follows up the spontaneous changes at the onset of SBD and HBD. The S-id spectra measured in fresh and SILC mode are reproduced by a literature model accounting for the carrier number and surface mobility fluctuations in the channel, and, as a result, both preexisting and newly generated trap densities are assessed. The post-SBD S-id does originate from current fluctuations in the SBD percolation paths, which can couple indirectly to drain via underlying channel in series, or directly to drain if the SBD path is formed close to drain extension. In particular, a fluctuation in S-id itself in the whole SBD duration is observed. This phenomenon is very striking since it indeed evidences the dynamic percolation origin concerning the trapping-detrapping processes in and around the SBD paths. The subsequent HBD duration remarkably features a flat S-id, indicating the set-up of a complete conductive path prevailing over the trapping-detrapping processes. (C) 2001 American Institute of Physics.en_US
dc.identifier.doi10.1063/1.1333029en_US
dc.identifier.issn0021-8979en_US
dc.identifier.journalJOURNAL OF APPLIED PHYSICSen_US
dc.identifier.urihttp://dx.doi.org/10.1063/1.1333029en_US
dc.identifier.urihttps://ir.lib.nycu.edu.tw/handle/11536/30001
dc.identifier.wosnumberWOS:000166118900100
dc.language.isoen_USen_US
dc.titleLow-frequency noise in n-channel metal-oxide-semiconductor field-effect transistors undergoing soft breakdownen_US
dc.typeArticleen_US

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