{"title":"Γ-X Transfer in Tunneling through Single AlAs Barriers","authors":"D. Landheer, H. Liu, M. Buchanan, R. Stoner","doi":"10.1364/qwoe.1989.tud2","DOIUrl":null,"url":null,"abstract":"When electrons tunnel through a single barrier of AlAs between GaAs contact layers there is a possibility of transfer from the Γ-conduction band to the X-band.1,2,3 The basic mechanism for Γ-X transfer based on the model of Liu 3 is shown in Fig. 1 along with Γ (solid lines) and X (dashed lines) conduction-band profiles for a 5.2 nm AlAs barrier. A Γ-electron can (1) tunnel through the entire structure without transfer, it can (2) transfer to the X-minimum at the first interface and propagate through the AlAs layer before transferring back to the Γ-minimum, or it can (3) transfer to the X-minimum at the first interface and propagate through the whole structure. The transfer at the interfaces is described by an interaction vertex VΓX or a coupling parameter α as described in Ref. 3. The process (2) is relatively unimportant at low applied potentials but becomes dominant above about 0.3 V where the Fermi energy has crossed the X-band in the AlAs.","PeriodicalId":205579,"journal":{"name":"Quantum Wells for Optics and Optoelectronics","volume":"32 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":"Quantum Wells for Optics and Optoelectronics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/qwoe.1989.tud2","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
When electrons tunnel through a single barrier of AlAs between GaAs contact layers there is a possibility of transfer from the Γ-conduction band to the X-band.1,2,3 The basic mechanism for Γ-X transfer based on the model of Liu 3 is shown in Fig. 1 along with Γ (solid lines) and X (dashed lines) conduction-band profiles for a 5.2 nm AlAs barrier. A Γ-electron can (1) tunnel through the entire structure without transfer, it can (2) transfer to the X-minimum at the first interface and propagate through the AlAs layer before transferring back to the Γ-minimum, or it can (3) transfer to the X-minimum at the first interface and propagate through the whole structure. The transfer at the interfaces is described by an interaction vertex VΓX or a coupling parameter α as described in Ref. 3. The process (2) is relatively unimportant at low applied potentials but becomes dominant above about 0.3 V where the Fermi energy has crossed the X-band in the AlAs.