{"title":"砷化镓和硅体1/f噪声的性质(综述)","authors":"N. V. D’yakonova, M. Levinshtein, S. L. Rumyantev","doi":"10.1063/1.44616","DOIUrl":null,"url":null,"abstract":"It is demonstrated, that the bulk 1/f noise in semiconductors can appear as a result of fluctuations of the occupancy of levels formed density‐of‐states tail near the band edge. It is shown that in pure Si with value of Hooge parameter α=10−4–10−6 and n‐GaAs with α=10−4–10−5 the nature of 1/f bulk noise is determined by this mechanism. Phenomenological model of the bulk 1/f noise in semiconductors is developed. This model explained well all main experimental data. The model predicts some new physical effects. All these effects have been observed experimentally.","PeriodicalId":316087,"journal":{"name":"Soviet physics. Semiconductors","volume":"75 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2008-05-29","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"21","resultStr":"{\"title\":\"Nature of the bulk 1/f noise in GaAs and Si (review)\",\"authors\":\"N. V. D’yakonova, M. Levinshtein, S. L. Rumyantev\",\"doi\":\"10.1063/1.44616\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"It is demonstrated, that the bulk 1/f noise in semiconductors can appear as a result of fluctuations of the occupancy of levels formed density‐of‐states tail near the band edge. It is shown that in pure Si with value of Hooge parameter α=10−4–10−6 and n‐GaAs with α=10−4–10−5 the nature of 1/f bulk noise is determined by this mechanism. Phenomenological model of the bulk 1/f noise in semiconductors is developed. This model explained well all main experimental data. The model predicts some new physical effects. All these effects have been observed experimentally.\",\"PeriodicalId\":316087,\"journal\":{\"name\":\"Soviet physics. Semiconductors\",\"volume\":\"75 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2008-05-29\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"21\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Soviet physics. Semiconductors\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1063/1.44616\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Soviet physics. Semiconductors","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1063/1.44616","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Nature of the bulk 1/f noise in GaAs and Si (review)
It is demonstrated, that the bulk 1/f noise in semiconductors can appear as a result of fluctuations of the occupancy of levels formed density‐of‐states tail near the band edge. It is shown that in pure Si with value of Hooge parameter α=10−4–10−6 and n‐GaAs with α=10−4–10−5 the nature of 1/f bulk noise is determined by this mechanism. Phenomenological model of the bulk 1/f noise in semiconductors is developed. This model explained well all main experimental data. The model predicts some new physical effects. All these effects have been observed experimentally.