{"title":"具有双轴拉伸应变的GaAsP/AlGaAs单量子阱中的空穴特征能","authors":"D. C. Bertolet, J. Hsu, K. Lau","doi":"10.1364/qwoe.1989.tue7","DOIUrl":null,"url":null,"abstract":"The effects of biaxial strain on the band-structure of III-V semiconductors have been investigated theoretically1,2 and experimentally3. These effects offer new degrees of freedom for heterostructure design, so-called \"band-structure engineering4.\" In particular, when III-V semiconductors are biaxially strained, the heavy- and light-hole bands become non-degenerate, and anisotropic. The valence-band configuration that arises from biaxial tensile strain is particularly well-suited for devices that involve optical absorption. Tensile strain and the quantum size effect (QSE) of a square potential well have the opposite effect on hole energy at k=0, and if the appropriate material parameters and structural dimensions are chosen, the heavy and light-hole eigenenergies of the QW will coincide. Equivalent heavy- and light-hole excitonic resonances will result in a larger absorption coefficient5, which can improve the performance of photodiodes and high speed optical modulators6. In addition, the capability to tailor the relative energies of the heavy- and light-hole could lead to new devices that exploit the different polarization-selection rules for the heavy- and light-hole excitonic transitions6,7. In this presentation we report on the growth and photoluminescence of strained GaAsP/ALGaAs single QW′S. The combined effects of biaxial tensile strain and QSE on the hole eigenenergies will be clearly demonstrated.","PeriodicalId":205579,"journal":{"name":"Quantum Wells for Optics and Optoelectronics","volume":"21 3","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Hole eigenenergies in GaAsP/AlGaAs single quantum wells with biaxial tensile strain\",\"authors\":\"D. C. Bertolet, J. Hsu, K. Lau\",\"doi\":\"10.1364/qwoe.1989.tue7\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The effects of biaxial strain on the band-structure of III-V semiconductors have been investigated theoretically1,2 and experimentally3. These effects offer new degrees of freedom for heterostructure design, so-called \\\"band-structure engineering4.\\\" In particular, when III-V semiconductors are biaxially strained, the heavy- and light-hole bands become non-degenerate, and anisotropic. The valence-band configuration that arises from biaxial tensile strain is particularly well-suited for devices that involve optical absorption. Tensile strain and the quantum size effect (QSE) of a square potential well have the opposite effect on hole energy at k=0, and if the appropriate material parameters and structural dimensions are chosen, the heavy and light-hole eigenenergies of the QW will coincide. Equivalent heavy- and light-hole excitonic resonances will result in a larger absorption coefficient5, which can improve the performance of photodiodes and high speed optical modulators6. In addition, the capability to tailor the relative energies of the heavy- and light-hole could lead to new devices that exploit the different polarization-selection rules for the heavy- and light-hole excitonic transitions6,7. In this presentation we report on the growth and photoluminescence of strained GaAsP/ALGaAs single QW′S. The combined effects of biaxial tensile strain and QSE on the hole eigenenergies will be clearly demonstrated.\",\"PeriodicalId\":205579,\"journal\":{\"name\":\"Quantum Wells for Optics and Optoelectronics\",\"volume\":\"21 3\",\"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.tue7\",\"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.tue7","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Hole eigenenergies in GaAsP/AlGaAs single quantum wells with biaxial tensile strain
The effects of biaxial strain on the band-structure of III-V semiconductors have been investigated theoretically1,2 and experimentally3. These effects offer new degrees of freedom for heterostructure design, so-called "band-structure engineering4." In particular, when III-V semiconductors are biaxially strained, the heavy- and light-hole bands become non-degenerate, and anisotropic. The valence-band configuration that arises from biaxial tensile strain is particularly well-suited for devices that involve optical absorption. Tensile strain and the quantum size effect (QSE) of a square potential well have the opposite effect on hole energy at k=0, and if the appropriate material parameters and structural dimensions are chosen, the heavy and light-hole eigenenergies of the QW will coincide. Equivalent heavy- and light-hole excitonic resonances will result in a larger absorption coefficient5, which can improve the performance of photodiodes and high speed optical modulators6. In addition, the capability to tailor the relative energies of the heavy- and light-hole could lead to new devices that exploit the different polarization-selection rules for the heavy- and light-hole excitonic transitions6,7. In this presentation we report on the growth and photoluminescence of strained GaAsP/ALGaAs single QW′S. The combined effects of biaxial tensile strain and QSE on the hole eigenenergies will be clearly demonstrated.