{"title":"具有大二阶光学非线性的非对称量子阱结构","authors":"J. Khurgin","doi":"10.1364/nlopm.1988.md4","DOIUrl":null,"url":null,"abstract":"Nonlinear optical properties of quantum wells (QW’s) and superlattices (SL’s) 1,2 are attracting increasing interest. Calculations and observations of strong third-order nonlinearities were reported in GaAs-GaAlAs QW and SL structures. Among the phenomena mentioned as leading to large values of x(3) in such structures are conduction band nonparabolicity 3,4, exciton line saturation 5 and the quantum confined Stark effect (QCSE) 6,7. Practical devices using QCSE, the so-called self-electrooptic effect devices, or SEED’s have been successfully demonstrated 8.","PeriodicalId":208307,"journal":{"name":"Nonlinear Optical Properties of Materials","volume":"7 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Asymmetric Quantum Well Structures Possessing Large Second Order Optical Nonlinearities\",\"authors\":\"J. Khurgin\",\"doi\":\"10.1364/nlopm.1988.md4\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Nonlinear optical properties of quantum wells (QW’s) and superlattices (SL’s) 1,2 are attracting increasing interest. Calculations and observations of strong third-order nonlinearities were reported in GaAs-GaAlAs QW and SL structures. Among the phenomena mentioned as leading to large values of x(3) in such structures are conduction band nonparabolicity 3,4, exciton line saturation 5 and the quantum confined Stark effect (QCSE) 6,7. Practical devices using QCSE, the so-called self-electrooptic effect devices, or SEED’s have been successfully demonstrated 8.\",\"PeriodicalId\":208307,\"journal\":{\"name\":\"Nonlinear Optical Properties of Materials\",\"volume\":\"7 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\":\"Nonlinear Optical Properties of Materials\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1364/nlopm.1988.md4\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nonlinear Optical Properties of Materials","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/nlopm.1988.md4","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Asymmetric Quantum Well Structures Possessing Large Second Order Optical Nonlinearities
Nonlinear optical properties of quantum wells (QW’s) and superlattices (SL’s) 1,2 are attracting increasing interest. Calculations and observations of strong third-order nonlinearities were reported in GaAs-GaAlAs QW and SL structures. Among the phenomena mentioned as leading to large values of x(3) in such structures are conduction band nonparabolicity 3,4, exciton line saturation 5 and the quantum confined Stark effect (QCSE) 6,7. Practical devices using QCSE, the so-called self-electrooptic effect devices, or SEED’s have been successfully demonstrated 8.