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A Near-Infrared Enhanced Silicon Single-Photon Avalanche Diode With a Spherically Uniform Electric Field Peak

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dc.contributor.authorVan Sieleghem, Edward-
dc.contributor.authorSuss, Andreas-
dc.contributor.authorBoulenc, Pierre-
dc.contributor.authorLee, Jiwon-
dc.contributor.authorKarve, Gauri-
dc.contributor.authorDe Munck, Koen-
dc.contributor.authorCavaco, Celso-
dc.contributor.authorVan Hoof, Chris-
dc.date.accessioned2023-08-16T07:31:01Z-
dc.date.available2023-08-16T07:31:01Z-
dc.date.issued2021-03-
dc.identifier.issn0741-3106-
dc.identifier.issn1558-0563-
dc.identifier.urihttps://scholarworks.bwise.kr/erica/handle/2021.sw.erica/113778-
dc.description.abstractA near-infrared (NIR) enhanced silicon single-photon avalanche diode (SPAD) fabricated in a customized $0.13~\mu \text{m}$ CMOS technology is presented. The SPAD has a depleted absorption volume of approximately $15\,\,\mu \text{m}\,\,\times 15\,\,\mu \text{m}\,\,\times 18\,\,\mu \text{m}$. Electrons generated in the absorption region are efficiently transported by drift to a central active avalanche region with a diameter of $2~\mu \text{m}$. At the operating voltage, the active region contains a spherically uniform field peak, enabling the multiplication of electrons originating from all corners of the device. The advantages of the SPAD architecture include high NIR photon detection efficiency (PDE), drift-based transport, low afterpulsing, and compatibility with an integrated CMOS readout. A front-side illuminated device is fabricated and characterized. The SPAD has a PDE of 13% at wavelength 905 nm, an afterpulsing probability < 0.1% for a dead time of 13 ns, and a median dark count rate (DCR) of 840 Hz at room temperature. The device shows promising performance for time-of-flight applications that benefit from uniform NIR-sensitive SPAD arrays. © 1980-2012 IEEE.-
dc.format.extent4-
dc.language영어-
dc.language.isoENG-
dc.publisherInstitute of Electrical and Electronics Engineers-
dc.titleA Near-Infrared Enhanced Silicon Single-Photon Avalanche Diode With a Spherically Uniform Electric Field Peak-
dc.typeArticle-
dc.publisher.location미국-
dc.identifier.doi10.1109/LED.2021.3070691-
dc.identifier.scopusid2-s2.0-85103762086-
dc.identifier.wosid000652794800025-
dc.identifier.bibliographicCitationIEEE Electron Device Letters, v.42, no.6, pp 879 - 882-
dc.citation.titleIEEE Electron Device Letters-
dc.citation.volume42-
dc.citation.number6-
dc.citation.startPage879-
dc.citation.endPage882-
dc.type.docType정기학술지(Article(Perspective Article포함))-
dc.description.isOpenAccessN-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaEngineering-
dc.relation.journalWebOfScienceCategoryEngineering, Electrical & Electronic-
dc.subject.keywordPlusSPAD-
dc.subject.keywordAuthorCMOS integrated circuit-
dc.subject.keywordAuthornear-infrared enhanced SPAD-
dc.subject.keywordAuthorSingle-photon avalanche diode (SPAD)-
dc.subject.keywordAuthorspherically uniform field peak-
dc.subject.keywordAuthortime-of-flight (ToF)-
dc.identifier.urlhttps://ieeexplore.ieee.org/document/9393954?arnumber=9393954&SID=EBSCO:edseee-
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