{"title":"超小型器件结构下电流波动的物理机制","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":"{\"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}","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}
Physical mechanism of current fluctuation under ultra-small device structures
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.