{"title":"一种用于单光子成像传感器的紧凑型主动淬火和充电像素电路","authors":"S. Panda, B. Choubey","doi":"10.1109/SENSORS52175.2022.9967310","DOIUrl":null,"url":null,"abstract":"This paper presents a compact pixel for single photon imaging applications, comprising of an actively quenched and recharged p+/n-well single photon avalanche diode (SPAD) with $10\\ \\mu \\mathrm{m}$ active area diameter and a novel 8-bit analogue counter. Additionally, the pixel includes a current starved inverter to regulate the hold-off time. Fabricated in $0.18\\ \\mu \\mathrm{m}$ complementary metal oxide semiconductor (CMOS) technology, the pixel occupies an overall area of $21\\ \\mu \\mathrm{m}\\times 21\\ \\mu \\mathrm{m}$ which is considerably smaller. Early analytical results demonstrate a fast quenching and recharge time of 120 ps and 4.38 ns respectively. Furthermore, a programmable dead time varying between 4.5 ns to 81 ns can be achieved, hence, leading to a reduction in afterpulsing probability.","PeriodicalId":120357,"journal":{"name":"2022 IEEE Sensors","volume":"1 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2022-10-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"A Compact Active Quenching and Recharge Pixel Circuit for Single Photon Imaging Sensors\",\"authors\":\"S. Panda, B. Choubey\",\"doi\":\"10.1109/SENSORS52175.2022.9967310\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"This paper presents a compact pixel for single photon imaging applications, comprising of an actively quenched and recharged p+/n-well single photon avalanche diode (SPAD) with $10\\\\ \\\\mu \\\\mathrm{m}$ active area diameter and a novel 8-bit analogue counter. Additionally, the pixel includes a current starved inverter to regulate the hold-off time. Fabricated in $0.18\\\\ \\\\mu \\\\mathrm{m}$ complementary metal oxide semiconductor (CMOS) technology, the pixel occupies an overall area of $21\\\\ \\\\mu \\\\mathrm{m}\\\\times 21\\\\ \\\\mu \\\\mathrm{m}$ which is considerably smaller. Early analytical results demonstrate a fast quenching and recharge time of 120 ps and 4.38 ns respectively. Furthermore, a programmable dead time varying between 4.5 ns to 81 ns can be achieved, hence, leading to a reduction in afterpulsing probability.\",\"PeriodicalId\":120357,\"journal\":{\"name\":\"2022 IEEE Sensors\",\"volume\":\"1 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2022-10-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"2022 IEEE Sensors\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1109/SENSORS52175.2022.9967310\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"2022 IEEE Sensors","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1109/SENSORS52175.2022.9967310","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
A Compact Active Quenching and Recharge Pixel Circuit for Single Photon Imaging Sensors
This paper presents a compact pixel for single photon imaging applications, comprising of an actively quenched and recharged p+/n-well single photon avalanche diode (SPAD) with $10\ \mu \mathrm{m}$ active area diameter and a novel 8-bit analogue counter. Additionally, the pixel includes a current starved inverter to regulate the hold-off time. Fabricated in $0.18\ \mu \mathrm{m}$ complementary metal oxide semiconductor (CMOS) technology, the pixel occupies an overall area of $21\ \mu \mathrm{m}\times 21\ \mu \mathrm{m}$ which is considerably smaller. Early analytical results demonstrate a fast quenching and recharge time of 120 ps and 4.38 ns respectively. Furthermore, a programmable dead time varying between 4.5 ns to 81 ns can be achieved, hence, leading to a reduction in afterpulsing probability.