{"title":"利用数值模拟技术确定嵌入Si1−yCy源/漏极nmosfet的单轴应力","authors":"A. Biswas","doi":"10.1109/ELECTRO.2009.5441176","DOIUrl":null,"url":null,"abstract":"Uniaxial stress induced by recessed or embedded Si<inf>1−y</inf>C<inf>y</inf> source/ drain in nanoscale nMOSFETs is computed using finite element method adopted in numerical process simulator. The lateral, vertical and perpendicular stress components S<inf>xx</inf>, S<inf>yy</inf> and S<inf>zz</inf>, respectively, are determined as a function of mole fraction y in the range 0.5 – 2.5 % and channel length L between 22–130 nm. Simulation results show that S<inf>xx</inf> in the middle of the channel at a distance 0.35 nm below the oxide semiconductor interface decreases linearly with L, while the other components exhibit a stronger nonlinear dependence on length. The implications for further device and process modeling will be addressed in a nutshell.","PeriodicalId":149384,"journal":{"name":"2009 International Conference on Emerging Trends in Electronic and Photonic Devices & Systems","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2009-12-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Determination of uniaxial stress of embedded Si1−yCy source/drain nMOSFETs using numerical simulation techniques\",\"authors\":\"A. Biswas\",\"doi\":\"10.1109/ELECTRO.2009.5441176\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Uniaxial stress induced by recessed or embedded Si<inf>1−y</inf>C<inf>y</inf> source/ drain in nanoscale nMOSFETs is computed using finite element method adopted in numerical process simulator. The lateral, vertical and perpendicular stress components S<inf>xx</inf>, S<inf>yy</inf> and S<inf>zz</inf>, respectively, are determined as a function of mole fraction y in the range 0.5 – 2.5 % and channel length L between 22–130 nm. Simulation results show that S<inf>xx</inf> in the middle of the channel at a distance 0.35 nm below the oxide semiconductor interface decreases linearly with L, while the other components exhibit a stronger nonlinear dependence on length. The implications for further device and process modeling will be addressed in a nutshell.\",\"PeriodicalId\":149384,\"journal\":{\"name\":\"2009 International Conference on Emerging Trends in Electronic and Photonic Devices & Systems\",\"volume\":null,\"pages\":null},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2009-12-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2009 International Conference on Emerging Trends in Electronic and Photonic Devices & Systems\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ELECTRO.2009.5441176\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2009 International Conference on Emerging Trends in Electronic and Photonic Devices & Systems","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ELECTRO.2009.5441176","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Determination of uniaxial stress of embedded Si1−yCy source/drain nMOSFETs using numerical simulation techniques
Uniaxial stress induced by recessed or embedded Si1−yCy source/ drain in nanoscale nMOSFETs is computed using finite element method adopted in numerical process simulator. The lateral, vertical and perpendicular stress components Sxx, Syy and Szz, respectively, are determined as a function of mole fraction y in the range 0.5 – 2.5 % and channel length L between 22–130 nm. Simulation results show that Sxx in the middle of the channel at a distance 0.35 nm below the oxide semiconductor interface decreases linearly with L, while the other components exhibit a stronger nonlinear dependence on length. The implications for further device and process modeling will be addressed in a nutshell.