Full metadata record

DC Field Value Language
dc.contributor.authorKeshavarzian, Pouyan-
dc.contributor.authorGramuglia, Francesco-
dc.contributor.authorKizilkan, Ekin-
dc.contributor.authorBruschini, Claudio-
dc.contributor.authorTan, Shyue Seng-
dc.contributor.authorTng, Michelle-
dc.contributor.authorChong, Daniel-
dc.contributor.authorQuek, Elgin-
dc.contributor.authorLee, Myung-Jae-
dc.contributor.authorCharbon, Edoardo-
dc.date.accessioned2024-01-12T03:42:46Z-
dc.date.available2024-01-12T03:42:46Z-
dc.date.created2022-09-05-
dc.date.issued2022-04-05-
dc.identifier.issn0277-786X-
dc.identifier.urihttps://pubs.kist.re.kr/handle/201004/77234-
dc.description.abstractSingle-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.languageEnglish-
dc.publisherSPIE-INT SOC OPTICAL ENGINEERING-
dc.titleLow-noise high-dynamic-range single-photon avalanche diodes with integrated PQAR circuit in a standard 55 nm BCD-
dc.typeConference-
dc.identifier.doi10.1117/12.2618349-
dc.description.journalClass1-
dc.identifier.bibliographicCitationConference on Advanced Photon Counting Techniques XVI-
dc.citation.titleConference on Advanced Photon Counting Techniques XVI-
dc.citation.conferencePlaceUS-
dc.citation.conferencePlaceOrlando-
dc.citation.conferenceDate2022-04-03-
dc.relation.isPartOfADVANCED PHOTON COUNTING TECHNIQUES XVI-
dc.identifier.wosid000839268300010-
Appears in Collections:
KIST Conference Paper > 2022
Files in This Item:
There are no files associated with this item.
Export
RIS (EndNote)
XLS (Excel)
XML

qrcode

Items in DSpace are protected by copyright, with all rights reserved, unless otherwise indicated.

BROWSE