{"title":"双极场效应晶体管的双极理论:最新进展","authors":"B. Jie, C. Sah","doi":"10.1109/ICSICT.2008.4734585","DOIUrl":null,"url":null,"abstract":"This article summarizes the history and progresses on our development of the Bipolar Field-Effect Transistor Theory (BiFET). The 2-Dimensional (2-D) rectangular geometry of the transistor (uniform in the width or Z-direction) is employed to decompose the 2-D equation into two 1-D equations which are parametrically coupled by the surface-electric-potential. This decomposition enables us to obtain the generic baseline solutions, both analytical and numerical, without the 2-D features which are then treated as the modifications of the 1-D solutions. The 1952-Shockley 2-section model used for the volume-channel geometry of his Junction-Gate (JG) FET is employed to both the surface and the volume-channels of the MOS BiFET, which we have designated and coined as the emitter and collector sections, each can simultaneously be electron and hole, surface or volume channels.","PeriodicalId":436457,"journal":{"name":"2008 9th International Conference on Solid-State and Integrated-Circuit Technology","volume":"42 5 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-12-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"The bipolar theory of the Bipolar Field-Effect Transistor: Recent advances\",\"authors\":\"B. Jie, C. Sah\",\"doi\":\"10.1109/ICSICT.2008.4734585\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This article summarizes the history and progresses on our development of the Bipolar Field-Effect Transistor Theory (BiFET). The 2-Dimensional (2-D) rectangular geometry of the transistor (uniform in the width or Z-direction) is employed to decompose the 2-D equation into two 1-D equations which are parametrically coupled by the surface-electric-potential. This decomposition enables us to obtain the generic baseline solutions, both analytical and numerical, without the 2-D features which are then treated as the modifications of the 1-D solutions. The 1952-Shockley 2-section model used for the volume-channel geometry of his Junction-Gate (JG) FET is employed to both the surface and the volume-channels of the MOS BiFET, which we have designated and coined as the emitter and collector sections, each can simultaneously be electron and hole, surface or volume channels.\",\"PeriodicalId\":436457,\"journal\":{\"name\":\"2008 9th International Conference on Solid-State and Integrated-Circuit Technology\",\"volume\":\"42 5 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-12-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2008 9th International Conference on Solid-State and Integrated-Circuit Technology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ICSICT.2008.4734585\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2008 9th International Conference on Solid-State and Integrated-Circuit Technology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICSICT.2008.4734585","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
The bipolar theory of the Bipolar Field-Effect Transistor: Recent advances
This article summarizes the history and progresses on our development of the Bipolar Field-Effect Transistor Theory (BiFET). The 2-Dimensional (2-D) rectangular geometry of the transistor (uniform in the width or Z-direction) is employed to decompose the 2-D equation into two 1-D equations which are parametrically coupled by the surface-electric-potential. This decomposition enables us to obtain the generic baseline solutions, both analytical and numerical, without the 2-D features which are then treated as the modifications of the 1-D solutions. The 1952-Shockley 2-section model used for the volume-channel geometry of his Junction-Gate (JG) FET is employed to both the surface and the volume-channels of the MOS BiFET, which we have designated and coined as the emitter and collector sections, each can simultaneously be electron and hole, surface or volume channels.