J. Shanley, C. T. Flanagan, M. Reine, T. Casselman
{"title":"Thermal diffusion current mechanisms in n+-p-p+Hg1-xCdxTe photodiodes","authors":"J. Shanley, C. T. Flanagan, M. Reine, T. Casselman","doi":"10.1109/IEDM.1980.189878","DOIUrl":null,"url":null,"abstract":"The thermal diffusion current mechanisms present in an 8-14 micrometer n<sup>+</sup>-p-p<sup>+</sup>(Hg,Cd)Te photodiode are analyzed. The n<sup>+</sup>region diffusion current is determined by first calculating the Auger 1 lifetime in degenerate n-type (Hg,Cd)Te. The Auger 1 lifetime is found to vary as 1/n<sup>α</sup><inf>o</inf>, where 0.7 ≤ α ≤ 1.0 and no is the equilibrium carrier density, for degenerate n-type (Hg,Cd)Te. The p-side diffusion current is calculated by considering the radiative and Auger 7 recombination mechanisms. A comparison of the n<sup>+</sup>- and p- side thermal diffusion current components reveals that the p-side contribution is dominant.","PeriodicalId":180541,"journal":{"name":"1980 International Electron Devices Meeting","volume":"34 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"1980 International Electron Devices Meeting","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IEDM.1980.189878","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
The thermal diffusion current mechanisms present in an 8-14 micrometer n+-p-p+(Hg,Cd)Te photodiode are analyzed. The n+region diffusion current is determined by first calculating the Auger 1 lifetime in degenerate n-type (Hg,Cd)Te. The Auger 1 lifetime is found to vary as 1/nαo, where 0.7 ≤ α ≤ 1.0 and no is the equilibrium carrier density, for degenerate n-type (Hg,Cd)Te. The p-side diffusion current is calculated by considering the radiative and Auger 7 recombination mechanisms. A comparison of the n+- and p- side thermal diffusion current components reveals that the p-side contribution is dominant.