{"title":"界面陷阱对PMOS器件中价带电子隧穿的贡献","authors":"T. Pompl, M. Kerber, H. Wurzer, I. Eisele","doi":"10.1109/ESSDERC.2000.194772","DOIUrl":null,"url":null,"abstract":"The I-V characteristic of the negatively biased p-poly PMOS changes from near valence band electron injection to near conduction band electron injection. The Fermi level is the reference energy level for valence band electron tunneling rather than the valence band edge, which results in a voltage dependent barrier height. The proposed Interface State Injection Model explains this by electron injection from interface states, quickly recharged by band to trap tunneling due to the small depletion layer width in highly doped gate material.","PeriodicalId":354721,"journal":{"name":"30th European Solid-State Device Research Conference","volume":"102 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2000-09-11","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"9","resultStr":"{\"title\":\"Contribution of interface traps to valence band electron tunneling in PMOS devices\",\"authors\":\"T. Pompl, M. Kerber, H. Wurzer, I. Eisele\",\"doi\":\"10.1109/ESSDERC.2000.194772\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The I-V characteristic of the negatively biased p-poly PMOS changes from near valence band electron injection to near conduction band electron injection. The Fermi level is the reference energy level for valence band electron tunneling rather than the valence band edge, which results in a voltage dependent barrier height. The proposed Interface State Injection Model explains this by electron injection from interface states, quickly recharged by band to trap tunneling due to the small depletion layer width in highly doped gate material.\",\"PeriodicalId\":354721,\"journal\":{\"name\":\"30th European Solid-State Device Research Conference\",\"volume\":\"102 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2000-09-11\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"9\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"30th European Solid-State Device Research Conference\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ESSDERC.2000.194772\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"30th European Solid-State Device Research Conference","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ESSDERC.2000.194772","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Contribution of interface traps to valence band electron tunneling in PMOS devices
The I-V characteristic of the negatively biased p-poly PMOS changes from near valence band electron injection to near conduction band electron injection. The Fermi level is the reference energy level for valence band electron tunneling rather than the valence band edge, which results in a voltage dependent barrier height. The proposed Interface State Injection Model explains this by electron injection from interface states, quickly recharged by band to trap tunneling due to the small depletion layer width in highly doped gate material.