{"title":"Γ-X通过单一屏障的隧道传输","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":"{\"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}","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}
Γ-X Transfer in Tunneling through Single AlAs Barriers
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.