{"title":"量子阱结构与量子点结构的光致发光光谱比较","authors":"Miyuki Esaki, N. Inaba, A. Fukuda, H. Imai","doi":"10.1109/ICIPRM.2010.5516393","DOIUrl":null,"url":null,"abstract":"We have compared the photoluminescence (PL) spectra of InAs/InGaAsP/InP quantum dots (QD) structures with that of InGaAs/InP quantum well (QW) structures by changing the incident angle for TE polarized excitation light. From the results, we have found the shift of the PL peak wavelength is different between QD and QW. Then, we have measured the change in the FWHM of the PL spectrum against the excitation light intensity. The increment rate of the FWHM for QD is larger than that for QW. From the above, we have supposed each QD couples electrically to form a continuous band structure and the quantum levels broaden, due to adjacent QD whose size are variant. It means the band filling effect for the bulk sample occurs in QD samples.","PeriodicalId":197102,"journal":{"name":"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)","volume":"29 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2010-07-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"1","resultStr":"{\"title\":\"Comparison of the photoluminescence spectra between quantum well structure and quantum dots structure\",\"authors\":\"Miyuki Esaki, N. Inaba, A. Fukuda, H. Imai\",\"doi\":\"10.1109/ICIPRM.2010.5516393\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We have compared the photoluminescence (PL) spectra of InAs/InGaAsP/InP quantum dots (QD) structures with that of InGaAs/InP quantum well (QW) structures by changing the incident angle for TE polarized excitation light. From the results, we have found the shift of the PL peak wavelength is different between QD and QW. Then, we have measured the change in the FWHM of the PL spectrum against the excitation light intensity. The increment rate of the FWHM for QD is larger than that for QW. From the above, we have supposed each QD couples electrically to form a continuous band structure and the quantum levels broaden, due to adjacent QD whose size are variant. It means the band filling effect for the bulk sample occurs in QD samples.\",\"PeriodicalId\":197102,\"journal\":{\"name\":\"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)\",\"volume\":\"29 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2010-07-23\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"1\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/ICIPRM.2010.5516393\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2010 22nd International Conference on Indium Phosphide and Related Materials (IPRM)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/ICIPRM.2010.5516393","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Comparison of the photoluminescence spectra between quantum well structure and quantum dots structure
We have compared the photoluminescence (PL) spectra of InAs/InGaAsP/InP quantum dots (QD) structures with that of InGaAs/InP quantum well (QW) structures by changing the incident angle for TE polarized excitation light. From the results, we have found the shift of the PL peak wavelength is different between QD and QW. Then, we have measured the change in the FWHM of the PL spectrum against the excitation light intensity. The increment rate of the FWHM for QD is larger than that for QW. From the above, we have supposed each QD couples electrically to form a continuous band structure and the quantum levels broaden, due to adjacent QD whose size are variant. It means the band filling effect for the bulk sample occurs in QD samples.