M Lindgren , M Currie , W.-S Zeng , R Sobolewski , S Cherednichenko , B Voronov , G.N Gol'tsman
{"title":"Picosecond response of a superconducting hot-electron NbN photodetector","authors":"M Lindgren , M Currie , W.-S Zeng , R Sobolewski , S Cherednichenko , B Voronov , G.N Gol'tsman","doi":"10.1016/S0964-1807(98)00110-0","DOIUrl":null,"url":null,"abstract":"<div><p>The ps optical response of ultrathin NbN photodetectors has been studied by electro-optic sampling. The detectors were fabricated by patterning ultrathin (3.5<!--> <!-->nm thick) NbN films deposited on sapphire by reactive magnetron sputtering into either a 5×10<!--> <em>μ</em>m<sup>2</sup> microbridge or 25 1<!--> <em>μ</em>m wide, 5<!--> <em>μ</em>m long strips connected in parallel. Both structures were placed at the center of a 4<!--> <!-->mm long coplanar waveguide covered with Ti/Au. The photoresponse was studied at temperatures ranging from 2.15<!--> <!-->K to 10<!--> <!-->K, with the samples biased in the resistive (switched) state and illuminated with 100 fs wide laser pulses at 395<!--> <!-->nm wavelength. At <em>T</em>=2.15<!--> <!-->K, we obtained an approximately 100 ps wide transient, which corresponds to a NbN detector response time of 45 ps. The photoresponse can be attributed to the nonequilibrium electron heating effect, where the incident radiation increases the temperature of the electron subsystem, while the phonons act as the heat sink. The high-speed response of NbN devices makes them an excellent choice for an optoelectronic interface for superconducting digital circuits, as well as mixers for the terahertz regime. The multiple-strip detector showed a linear dependence on input optical power and a responsivity <span><math><mtext>R</mtext></math></span>=3.9<!--> <!-->V/W.</p></div>","PeriodicalId":100110,"journal":{"name":"Applied Superconductivity","volume":"6 7","pages":"Pages 423-428"},"PeriodicalIF":0.0000,"publicationDate":"1998-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://sci-hub-pdf.com/10.1016/S0964-1807(98)00110-0","citationCount":"10","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Applied Superconductivity","FirstCategoryId":"1085","ListUrlMain":"https://www.sciencedirect.com/science/article/pii/S0964180798001100","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 10
Abstract
The ps optical response of ultrathin NbN photodetectors has been studied by electro-optic sampling. The detectors were fabricated by patterning ultrathin (3.5 nm thick) NbN films deposited on sapphire by reactive magnetron sputtering into either a 5×10 μm2 microbridge or 25 1 μm wide, 5 μm long strips connected in parallel. Both structures were placed at the center of a 4 mm long coplanar waveguide covered with Ti/Au. The photoresponse was studied at temperatures ranging from 2.15 K to 10 K, with the samples biased in the resistive (switched) state and illuminated with 100 fs wide laser pulses at 395 nm wavelength. At T=2.15 K, we obtained an approximately 100 ps wide transient, which corresponds to a NbN detector response time of 45 ps. The photoresponse can be attributed to the nonequilibrium electron heating effect, where the incident radiation increases the temperature of the electron subsystem, while the phonons act as the heat sink. The high-speed response of NbN devices makes them an excellent choice for an optoelectronic interface for superconducting digital circuits, as well as mixers for the terahertz regime. The multiple-strip detector showed a linear dependence on input optical power and a responsivity =3.9 V/W.