Quantum efficiency and noise equivalent power of nanostructured, NbN, single-photon detectors in the wavelength range from visible to infrared
We present our studies on the quantum efficiency (QE) and the noise equivalent power (NEP) of the latest-generation, nanostructured, superconducting, single-photon detectors (SSPDs) in the wavelength range from 0.5 to 5.6 /spl mu/m, operated at temperatures in the 2.0- to 4.2-K range. Our detectors...
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Veröffentlicht in: | IEEE transactions on applied superconductivity 2005-06, Vol.15 (2), p.571-574 |
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creator | Korneev, A. Matvienko, V. Minaeva, O. Milostnaya, I. Rubtsova, I. Chulkova, G. Smirnov, K. Voronov, V. Gol'tsman, G. Slysz, W. Pearlman, A. Verevkin, A. Sobolewski, R. |
description | We present our studies on the quantum efficiency (QE) and the noise equivalent power (NEP) of the latest-generation, nanostructured, superconducting, single-photon detectors (SSPDs) in the wavelength range from 0.5 to 5.6 /spl mu/m, operated at temperatures in the 2.0- to 4.2-K range. Our detectors are designed as 4-nm-thick and 100-nm-wide NbN meander-shaped stripes, patterned by electron-beam lithography and cover a 10/spl times/10-/spl mu/m/sup 2/ active area. The best-achieved QE at 2.0 K for 1.55-/spl mu/m photons is 17%, and QE for 1.3-/spl mu/m infrared photons reaches its saturation value of /spl sim/30%. The SSPD NEP at 2.0 K is as low as 5/spl times/10/sup -21/ W/Hz/sup -1/2/. Our nanostructured SSPDs, operated at 2.0 K, significantly outperform their semiconducting counterparts, and, together with their GHz counting rate and picosecond timing jitter, they are devices-of-choice for practical quantum key distribution systems and free-space (even interplanetary) quantum optical communications. |
doi_str_mv | 10.1109/TASC.2005.849923 |
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Our detectors are designed as 4-nm-thick and 100-nm-wide NbN meander-shaped stripes, patterned by electron-beam lithography and cover a 10/spl times/10-/spl mu/m/sup 2/ active area. The best-achieved QE at 2.0 K for 1.55-/spl mu/m photons is 17%, and QE for 1.3-/spl mu/m infrared photons reaches its saturation value of /spl sim/30%. The SSPD NEP at 2.0 K is as low as 5/spl times/10/sup -21/ W/Hz/sup -1/2/. Our nanostructured SSPDs, operated at 2.0 K, significantly outperform their semiconducting counterparts, and, together with their GHz counting rate and picosecond timing jitter, they are devices-of-choice for practical quantum key distribution systems and free-space (even interplanetary) quantum optical communications.</description><identifier>ISSN: 1051-8223</identifier><identifier>EISSN: 1558-2515</identifier><identifier>DOI: 10.1109/TASC.2005.849923</identifier><identifier>CODEN: ITASE9</identifier><language>eng</language><publisher>New York: IEEE</publisher><subject>Detectors ; Electron beam lithography ; Equivalence ; Infrared ; Infrared detectors ; Infrared optical detectors ; Lithography ; Nanoscale devices ; Nanostructure ; NbN superconducting films ; Optical fiber communication ; Photons ; Semiconductivity ; Semiconductor device noise ; single-photon counters ; Superconducting device noise ; superconducting devices ; Superconducting photodetectors ; Superconductivity ; Temperature distribution ; Timing jitter ; Wavelengths</subject><ispartof>IEEE transactions on applied superconductivity, 2005-06, Vol.15 (2), p.571-574</ispartof><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) 2005</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c451t-d35c9305cf8e187166e83d023bf716fea5004349081421f5fcd6bf5ec4d487d53</citedby><cites>FETCH-LOGICAL-c451t-d35c9305cf8e187166e83d023bf716fea5004349081421f5fcd6bf5ec4d487d53</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/1439702$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,776,780,792,27901,27902,54733</link.rule.ids><linktorsrc>$$Uhttps://ieeexplore.ieee.org/document/1439702$$EView_record_in_IEEE$$FView_record_in_$$GIEEE</linktorsrc></links><search><creatorcontrib>Korneev, A.</creatorcontrib><creatorcontrib>Matvienko, V.</creatorcontrib><creatorcontrib>Minaeva, O.</creatorcontrib><creatorcontrib>Milostnaya, I.</creatorcontrib><creatorcontrib>Rubtsova, I.</creatorcontrib><creatorcontrib>Chulkova, G.</creatorcontrib><creatorcontrib>Smirnov, K.</creatorcontrib><creatorcontrib>Voronov, V.</creatorcontrib><creatorcontrib>Gol'tsman, G.</creatorcontrib><creatorcontrib>Slysz, W.</creatorcontrib><creatorcontrib>Pearlman, A.</creatorcontrib><creatorcontrib>Verevkin, A.</creatorcontrib><creatorcontrib>Sobolewski, R.</creatorcontrib><title>Quantum efficiency and noise equivalent power of nanostructured, NbN, single-photon detectors in the wavelength range from visible to infrared</title><title>IEEE transactions on applied superconductivity</title><addtitle>TASC</addtitle><description>We present our studies on the quantum efficiency (QE) and the noise equivalent power (NEP) of the latest-generation, nanostructured, superconducting, single-photon detectors (SSPDs) in the wavelength range from 0.5 to 5.6 /spl mu/m, operated at temperatures in the 2.0- to 4.2-K range. Our detectors are designed as 4-nm-thick and 100-nm-wide NbN meander-shaped stripes, patterned by electron-beam lithography and cover a 10/spl times/10-/spl mu/m/sup 2/ active area. The best-achieved QE at 2.0 K for 1.55-/spl mu/m photons is 17%, and QE for 1.3-/spl mu/m infrared photons reaches its saturation value of /spl sim/30%. The SSPD NEP at 2.0 K is as low as 5/spl times/10/sup -21/ W/Hz/sup -1/2/. Our nanostructured SSPDs, operated at 2.0 K, significantly outperform their semiconducting counterparts, and, together with their GHz counting rate and picosecond timing jitter, they are devices-of-choice for practical quantum key distribution systems and free-space (even interplanetary) quantum optical communications.</description><subject>Detectors</subject><subject>Electron beam lithography</subject><subject>Equivalence</subject><subject>Infrared</subject><subject>Infrared detectors</subject><subject>Infrared optical detectors</subject><subject>Lithography</subject><subject>Nanoscale devices</subject><subject>Nanostructure</subject><subject>NbN superconducting films</subject><subject>Optical fiber communication</subject><subject>Photons</subject><subject>Semiconductivity</subject><subject>Semiconductor device noise</subject><subject>single-photon counters</subject><subject>Superconducting device noise</subject><subject>superconducting devices</subject><subject>Superconducting photodetectors</subject><subject>Superconductivity</subject><subject>Temperature distribution</subject><subject>Timing jitter</subject><subject>Wavelengths</subject><issn>1051-8223</issn><issn>1558-2515</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2005</creationdate><recordtype>article</recordtype><sourceid>RIE</sourceid><recordid>eNqNkU9rFDEYhwdRsK7eBS_Bg3jorG_-zWSOZalWKBWxnkM282Y3ZTbZJpkt_RJ-ZrOsUPAgnt688Px-IXma5i2FJaUwfLq9-LFaMgC5VGIYGH_WnFEpVcsklc_rGSRtFWP8ZfMq5zsAKpSQZ82v77MJZd4RdM5bj8E-EhNGEqLPSPB-9gczYShkHx8wkehIMCHmkmZb5oTjOblZ35yT7MNmwna_jSUGMmJBW2LKxAdStkgezAFry6ZsSTJhg8SluCMHn_16QlJi5Vwyte5188KZKeObP3PR_Px8ebu6aq-_ffm6urhurZC0tCOXduAgrVNIVU-7DhUfgfG1q4tDIwEEFwMoKhh10tmxWzuJVoxC9aPki-bDqXef4v2MueidzxanyQSMc9ZM0Y4zUP8BQt-rnlfw4z9ByrtqQnTiiL7_C72Lcwr1vXqg9VKAWrho4ATZFHNO6PQ--Z1Jj5qCPhrXR-P6aFyfjNfIu1PEI-ITLvjQ16_5Da4GqI8</recordid><startdate>20050601</startdate><enddate>20050601</enddate><creator>Korneev, A.</creator><creator>Matvienko, V.</creator><creator>Minaeva, O.</creator><creator>Milostnaya, I.</creator><creator>Rubtsova, I.</creator><creator>Chulkova, G.</creator><creator>Smirnov, K.</creator><creator>Voronov, V.</creator><creator>Gol'tsman, G.</creator><creator>Slysz, W.</creator><creator>Pearlman, A.</creator><creator>Verevkin, A.</creator><creator>Sobolewski, R.</creator><general>IEEE</general><general>The Institute of Electrical and Electronics Engineers, Inc. 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Our detectors are designed as 4-nm-thick and 100-nm-wide NbN meander-shaped stripes, patterned by electron-beam lithography and cover a 10/spl times/10-/spl mu/m/sup 2/ active area. The best-achieved QE at 2.0 K for 1.55-/spl mu/m photons is 17%, and QE for 1.3-/spl mu/m infrared photons reaches its saturation value of /spl sim/30%. The SSPD NEP at 2.0 K is as low as 5/spl times/10/sup -21/ W/Hz/sup -1/2/. Our nanostructured SSPDs, operated at 2.0 K, significantly outperform their semiconducting counterparts, and, together with their GHz counting rate and picosecond timing jitter, they are devices-of-choice for practical quantum key distribution systems and free-space (even interplanetary) quantum optical communications.</abstract><cop>New York</cop><pub>IEEE</pub><doi>10.1109/TASC.2005.849923</doi><tpages>4</tpages></addata></record> |
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subjects | Detectors Electron beam lithography Equivalence Infrared Infrared detectors Infrared optical detectors Lithography Nanoscale devices Nanostructure NbN superconducting films Optical fiber communication Photons Semiconductivity Semiconductor device noise single-photon counters Superconducting device noise superconducting devices Superconducting photodetectors Superconductivity Temperature distribution Timing jitter Wavelengths |
title | Quantum efficiency and noise equivalent power of nanostructured, NbN, single-photon detectors in the wavelength range from visible to infrared |
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