{"title":"Physical mechanism of current fluctuation under ultra-small device structures","authors":"N. Sano, K. Natori, M. Mukai, K. Matsuzawa","doi":"10.1109/IWCE.1998.742723","DOIUrl":null,"url":null,"abstract":"Monte Carlo analyses of the current fluctuation in Si n-i-n structures have been carried out by varying the length of the i (channel) region so that the diffusive to quasi-ballistic transport is covered. It has been demonstrated that the current fluctuation is dominated by thermal noise at low bias regions and makes a direct transition to hot carrier noise in moderately large devices. On the other hand, a new fluctuation mode appears under sub-0.1 micron device structures. This is associated with the fluctuation of the electron number in the i (channel) region and results from both the ballistic electrons emitted from the left n (source) region and the electrons diffused from the right n (drain) region.","PeriodicalId":357304,"journal":{"name":"1998 Sixth International Workshop on Computational Electronics. Extended Abstracts (Cat. No.98EX116)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1998-10-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"3","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1998 Sixth International Workshop on Computational Electronics. Extended Abstracts (Cat. No.98EX116)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IWCE.1998.742723","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 3
Abstract
Monte Carlo analyses of the current fluctuation in Si n-i-n structures have been carried out by varying the length of the i (channel) region so that the diffusive to quasi-ballistic transport is covered. It has been demonstrated that the current fluctuation is dominated by thermal noise at low bias regions and makes a direct transition to hot carrier noise in moderately large devices. On the other hand, a new fluctuation mode appears under sub-0.1 micron device structures. This is associated with the fluctuation of the electron number in the i (channel) region and results from both the ballistic electrons emitted from the left n (source) region and the electrons diffused from the right n (drain) region.