D. Jena, Tara Prasanna Dash, N. Sahoo, A. Sahu, A. K. Panda, T. Sahu
{"title":"Improvement of Transport Mobility in Asymmetric V-shaped Double Quantum Well Structure","authors":"D. Jena, Tara Prasanna Dash, N. Sahoo, A. Sahu, A. K. Panda, T. Sahu","doi":"10.1109/EDKCON56221.2022.10032965","DOIUrl":null,"url":null,"abstract":"The improvement of transport electron mobility μ is theoretically reported through a change in well width w in an asymmetric V-shaped double quantum well (AVDQW) structure. The side barriers are doped with different doping concentrations i.e., Nd1 (vary) and Nd2 (fixed) towards the substrate and surface respectively which produces asymmetry in the structure. An increase in w enhances μ. The magnitude of μ is decided by the alloy disorder scattering but the trend in the variation of μ as a function of Nd1 is mainly decided by the impurity scattering.","PeriodicalId":296883,"journal":{"name":"2022 IEEE International Conference of Electron Devices Society Kolkata Chapter (EDKCON)","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2022-11-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"2022 IEEE International Conference of Electron Devices Society Kolkata Chapter (EDKCON)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/EDKCON56221.2022.10032965","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 1
Abstract
The improvement of transport electron mobility μ is theoretically reported through a change in well width w in an asymmetric V-shaped double quantum well (AVDQW) structure. The side barriers are doped with different doping concentrations i.e., Nd1 (vary) and Nd2 (fixed) towards the substrate and surface respectively which produces asymmetry in the structure. An increase in w enhances μ. The magnitude of μ is decided by the alloy disorder scattering but the trend in the variation of μ as a function of Nd1 is mainly decided by the impurity scattering.