{"title":"模拟单片集成单光子计数器","authors":"D. Cronin, A. M. Moloney, A. Morrison","doi":"10.1109/HFPSC.2004.1360336","DOIUrl":null,"url":null,"abstract":"Simulations of a Geiger-mode avalanche photodiode (GMAP) monolithically integrated with its corresponding active quench and reset circuit (AQRC) are presented. The AQRC design is simulated in Agilent's ADS simulator using BSIM3 MOSFET models acquired from Europractice's 0.6 /spl mu/m CMOS process. The novelty of the design ensures a minimum dead-time of 13 ns between adjacent incident photons. This corresponds to a maximum achievable saturated count-rate of 77 Mcounts/sec, not previously reported.","PeriodicalId":405718,"journal":{"name":"High Frequency Postgraduate Student Colloquium, 2004","volume":"37 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2004-11-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"12","resultStr":"{\"title\":\"Simulated monolithically integrated single photon counter\",\"authors\":\"D. Cronin, A. M. Moloney, A. Morrison\",\"doi\":\"10.1109/HFPSC.2004.1360336\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Simulations of a Geiger-mode avalanche photodiode (GMAP) monolithically integrated with its corresponding active quench and reset circuit (AQRC) are presented. The AQRC design is simulated in Agilent's ADS simulator using BSIM3 MOSFET models acquired from Europractice's 0.6 /spl mu/m CMOS process. The novelty of the design ensures a minimum dead-time of 13 ns between adjacent incident photons. This corresponds to a maximum achievable saturated count-rate of 77 Mcounts/sec, not previously reported.\",\"PeriodicalId\":405718,\"journal\":{\"name\":\"High Frequency Postgraduate Student Colloquium, 2004\",\"volume\":\"37 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2004-11-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"12\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"High Frequency Postgraduate Student Colloquium, 2004\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/HFPSC.2004.1360336\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"High Frequency Postgraduate Student Colloquium, 2004","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/HFPSC.2004.1360336","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Simulated monolithically integrated single photon counter
Simulations of a Geiger-mode avalanche photodiode (GMAP) monolithically integrated with its corresponding active quench and reset circuit (AQRC) are presented. The AQRC design is simulated in Agilent's ADS simulator using BSIM3 MOSFET models acquired from Europractice's 0.6 /spl mu/m CMOS process. The novelty of the design ensures a minimum dead-time of 13 ns between adjacent incident photons. This corresponds to a maximum achievable saturated count-rate of 77 Mcounts/sec, not previously reported.
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