{"title":"1.9皮秒光学时间分析仪采用1.2皮秒光电探测器和栅极","authors":"Y. Chen, S. Williamson, T. Brock, F. Smith","doi":"10.1109/IEDM.1991.235366","DOIUrl":null,"url":null,"abstract":"The authors report on a novel photoconductive-type detector with a response time of 1.2 ps. This is the fastest photodetector to date. It is based on low-temperature-grown GaAs and uses interdigitated electrodes of 0.2 mu m spacing to match the carrier transit time to the carrier lifetime. The responsivity is 0.1 A/W. The detector can be driven to an on-state resistance of a few of ohms, with the response time increasing to only 1.5 ps. The photodetector can therefore also function as a picosecond photogate. The two components have been combined to form an all-semiconductor optical temporal analyzer. The system response time is 1.9 ps, with a minimum detectable average power of 500 pW. The technique is jitter-free, permitting long integration times. Ultraweak picosecond fluorescence and scattering experiments, as well as other ultrafast phenomena can be time-resolved using this relatively simple tool.<<ETX>>","PeriodicalId":13885,"journal":{"name":"International Electron Devices Meeting 1991 [Technical Digest]","volume":"12 1","pages":"416-421"},"PeriodicalIF":0.0000,"publicationDate":"1991-12-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"4","resultStr":"{\"title\":\"1.9 picosecond optical temporal analyzer using 1.2 picosecond photodetector and gate\",\"authors\":\"Y. Chen, S. Williamson, T. Brock, F. Smith\",\"doi\":\"10.1109/IEDM.1991.235366\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The authors report on a novel photoconductive-type detector with a response time of 1.2 ps. This is the fastest photodetector to date. It is based on low-temperature-grown GaAs and uses interdigitated electrodes of 0.2 mu m spacing to match the carrier transit time to the carrier lifetime. The responsivity is 0.1 A/W. The detector can be driven to an on-state resistance of a few of ohms, with the response time increasing to only 1.5 ps. The photodetector can therefore also function as a picosecond photogate. The two components have been combined to form an all-semiconductor optical temporal analyzer. The system response time is 1.9 ps, with a minimum detectable average power of 500 pW. The technique is jitter-free, permitting long integration times. Ultraweak picosecond fluorescence and scattering experiments, as well as other ultrafast phenomena can be time-resolved using this relatively simple tool.<<ETX>>\",\"PeriodicalId\":13885,\"journal\":{\"name\":\"International Electron Devices Meeting 1991 [Technical Digest]\",\"volume\":\"12 1\",\"pages\":\"416-421\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"1991-12-08\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"4\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Electron Devices Meeting 1991 [Technical Digest]\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/IEDM.1991.235366\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Electron Devices Meeting 1991 [Technical Digest]","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/IEDM.1991.235366","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
1.9 picosecond optical temporal analyzer using 1.2 picosecond photodetector and gate
The authors report on a novel photoconductive-type detector with a response time of 1.2 ps. This is the fastest photodetector to date. It is based on low-temperature-grown GaAs and uses interdigitated electrodes of 0.2 mu m spacing to match the carrier transit time to the carrier lifetime. The responsivity is 0.1 A/W. The detector can be driven to an on-state resistance of a few of ohms, with the response time increasing to only 1.5 ps. The photodetector can therefore also function as a picosecond photogate. The two components have been combined to form an all-semiconductor optical temporal analyzer. The system response time is 1.9 ps, with a minimum detectable average power of 500 pW. The technique is jitter-free, permitting long integration times. Ultraweak picosecond fluorescence and scattering experiments, as well as other ultrafast phenomena can be time-resolved using this relatively simple tool.<>