{"title":"InxGa1−xAs/InP量子阱中应变层的光学跃迁","authors":"D. Gershoni, H. Temkin, M. Panish","doi":"10.1364/qwoe.1989.wa2","DOIUrl":null,"url":null,"abstract":"We present a study of the optical transitions between confined particle states of strained layer quantum wells (SLQWs). SLQWs of InxGa1−xAs/InP with x ranging from 0 to 1 are an excellent system for this type of study because their strain varies systematically from −3.8%(x = 0) to +3.2%(x = 1). In previous studies we have used electro-optic techniques [1,2] and admittance spectroscopy [3] to show that most of the change with x in the band gap discontinuity between InP and InxGa1−xAs layers, takes place in the conduction band. A simple phenomenological deformation potential model, has enabled us to successfully calculate the lowest ( n = 1 ) excitonic transitions for any x and in particular to explain a type I to type II superlattice transition for x ≅ 0.2. In this study we show that in order to account for higer order transitions one has to include non-linear terms in strain and band non-parabolicity effects. Our model which contains no adjustable parameters agrees well with the observed transitions.","PeriodicalId":205579,"journal":{"name":"Quantum Wells for Optics and Optoelectronics","volume":"17 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Optical Transitions in Strained Layer InxGa1−xAs/InP Quantum Wells\",\"authors\":\"D. Gershoni, H. Temkin, M. Panish\",\"doi\":\"10.1364/qwoe.1989.wa2\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We present a study of the optical transitions between confined particle states of strained layer quantum wells (SLQWs). SLQWs of InxGa1−xAs/InP with x ranging from 0 to 1 are an excellent system for this type of study because their strain varies systematically from −3.8%(x = 0) to +3.2%(x = 1). In previous studies we have used electro-optic techniques [1,2] and admittance spectroscopy [3] to show that most of the change with x in the band gap discontinuity between InP and InxGa1−xAs layers, takes place in the conduction band. A simple phenomenological deformation potential model, has enabled us to successfully calculate the lowest ( n = 1 ) excitonic transitions for any x and in particular to explain a type I to type II superlattice transition for x ≅ 0.2. In this study we show that in order to account for higer order transitions one has to include non-linear terms in strain and band non-parabolicity effects. Our model which contains no adjustable parameters agrees well with the observed transitions.\",\"PeriodicalId\":205579,\"journal\":{\"name\":\"Quantum Wells for Optics and Optoelectronics\",\"volume\":\"17 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.wa2\",\"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.wa2","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Optical Transitions in Strained Layer InxGa1−xAs/InP Quantum Wells
We present a study of the optical transitions between confined particle states of strained layer quantum wells (SLQWs). SLQWs of InxGa1−xAs/InP with x ranging from 0 to 1 are an excellent system for this type of study because their strain varies systematically from −3.8%(x = 0) to +3.2%(x = 1). In previous studies we have used electro-optic techniques [1,2] and admittance spectroscopy [3] to show that most of the change with x in the band gap discontinuity between InP and InxGa1−xAs layers, takes place in the conduction band. A simple phenomenological deformation potential model, has enabled us to successfully calculate the lowest ( n = 1 ) excitonic transitions for any x and in particular to explain a type I to type II superlattice transition for x ≅ 0.2. In this study we show that in order to account for higer order transitions one has to include non-linear terms in strain and band non-parabolicity effects. Our model which contains no adjustable parameters agrees well with the observed transitions.