{"title":"Evolution of multi-valley electron distributions in GaAs","authors":"R. Chennupati, M. Cheng","doi":"10.1109/SECON.1994.324355","DOIUrl":null,"url":null,"abstract":"An approach based on the physical evolution of the distribution function in the energy relaxation scale is used to study multi-valley distribution functions of electrons in GaAs subjected to a rapid change in electric field. This approach, which assumes the distribution can be determined by mean energy, is able to describe transport phenomena, including inter-valley transitions, in the scale as small as the energy relaxation time. Results show that, near the peak of velocity overshoot and bottom of undershoot in the /spl Gamma/ valley, the energy-dependent distribution cannot respond as fast as the distribution obtained from Monte Carlo method. This results in less pronounced overshoot and undershoot in the /spl Gamma/ valley when using the introduced approach than using the Monte Carlo method. However, in the L valley, overshoot and undershoot are not pronounced, and these two approaches are in very good agreement.<<ETX>>","PeriodicalId":119615,"journal":{"name":"Proceedings of SOUTHEASTCON '94","volume":"145 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1994-04-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of SOUTHEASTCON '94","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SECON.1994.324355","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
An approach based on the physical evolution of the distribution function in the energy relaxation scale is used to study multi-valley distribution functions of electrons in GaAs subjected to a rapid change in electric field. This approach, which assumes the distribution can be determined by mean energy, is able to describe transport phenomena, including inter-valley transitions, in the scale as small as the energy relaxation time. Results show that, near the peak of velocity overshoot and bottom of undershoot in the /spl Gamma/ valley, the energy-dependent distribution cannot respond as fast as the distribution obtained from Monte Carlo method. This results in less pronounced overshoot and undershoot in the /spl Gamma/ valley when using the introduced approach than using the Monte Carlo method. However, in the L valley, overshoot and undershoot are not pronounced, and these two approaches are in very good agreement.<>