{"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":"60 1","pages":"0"},"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}
引用次数: 0
Abstract
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.