Full metadata record
DC Field | Value | Language |
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dc.contributor.author | Keshavarzian, Pouyan | - |
dc.contributor.author | Gramuglia, Francesco | - |
dc.contributor.author | Kizilkan, Ekin | - |
dc.contributor.author | Bruschini, Claudio | - |
dc.contributor.author | Tan, Shyue Seng | - |
dc.contributor.author | Tng, Michelle | - |
dc.contributor.author | Chong, Daniel | - |
dc.contributor.author | Quek, Elgin | - |
dc.contributor.author | Lee, Myung-Jae | - |
dc.contributor.author | Charbon, Edoardo | - |
dc.date.accessioned | 2024-01-12T03:42:46Z | - |
dc.date.available | 2024-01-12T03:42:46Z | - |
dc.date.created | 2022-09-05 | - |
dc.date.issued | 2022-04-05 | - |
dc.identifier.issn | 0277-786X | - |
dc.identifier.uri | https://pubs.kist.re.kr/handle/201004/77234 | - |
dc.description.abstract | Single-photon avalanche diode (SPAD) based sensors and systems enable a variety of applications in biomedical, automotive, consumer, and security domains. While several established standard technologies, which can facilitate the design of SPAD-based systems are already in existence, challenges remain for the development of deep sub-micron monolithic integration of circuits and SPADs. In this work, we present SPADs along with pixel circuits in a standard GF 55 nm BCDL process. Two different designs demonstrate the flexibility allowed by the technology for a variety of applications. Both shallow and deep junction SPADs present excellent noise performance of less than 1 cps/mu m(2) at 3 V excess bias. An integrated passive-quench active-recharge (PQAR) circuit is used in conjunction with the SPADs, which enables a dead time of less than 2 ns, easily allowing for high dynamic range applications that require > 100 Mcps such as quantum communication and information technologies. The deep and shallow junction SPADs demonstrate an afterpulsing probability of < 0.5 % and < 2 % at 3V excess bias, respectively. The dead time is adjustable through analog control of the active-recharge circuit, allowing for afterpulsing reduction to below 0.1 % while maintaining Mcps operation. The shallow junction, which has a breakdown voltage of about 18 V and a peak sensitivity at 430 nm is particularly interesting for applications requiring low supply voltage, whereas the deep SPAD, which demonstrates > 4 % photon detection probability (PDP) at 940 nm, can be implemented in LiDAR sensors that require enhanced sensitivity at near-infrared (NIR) wavelengths. The measured timing jitter of both SPADs is < 50 ps FWHM at 3 V excess bias and 780 nm. | - |
dc.language | English | - |
dc.publisher | SPIE-INT SOC OPTICAL ENGINEERING | - |
dc.title | Low-noise high-dynamic-range single-photon avalanche diodes with integrated PQAR circuit in a standard 55 nm BCD | - |
dc.type | Conference | - |
dc.identifier.doi | 10.1117/12.2618349 | - |
dc.description.journalClass | 1 | - |
dc.identifier.bibliographicCitation | Conference on Advanced Photon Counting Techniques XVI | - |
dc.citation.title | Conference on Advanced Photon Counting Techniques XVI | - |
dc.citation.conferencePlace | US | - |
dc.citation.conferencePlace | Orlando | - |
dc.citation.conferenceDate | 2022-04-03 | - |
dc.relation.isPartOf | ADVANCED PHOTON COUNTING TECHNIQUES XVI | - |
dc.identifier.wosid | 000839268300010 | - |
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