{"publication_status":"published","date_updated":"2023-01-12T15:13:40Z","language":[{"iso":"eng"}],"article_number":"081303","title":"Opto-electronic bias of a superconducting nanowire single photon detector using a cryogenic photodiode","department":[{"_id":"15"},{"_id":"230"},{"_id":"623"}],"publisher":"AIP Publishing","citation":{"ieee":"F. Thiele, T. Hummel, M. Protte, and T. Bartley, “Opto-electronic bias of a superconducting nanowire single photon detector using a cryogenic photodiode,” <i>APL Photonics</i>, vol. 7, no. 8, Art. no. 081303, 2022, doi: <a href=\"https://doi.org/10.1063/5.0097506\">10.1063/5.0097506</a>.","apa":"Thiele, F., Hummel, T., Protte, M., &#38; Bartley, T. (2022). Opto-electronic bias of a superconducting nanowire single photon detector using a cryogenic photodiode. <i>APL Photonics</i>, <i>7</i>(8), Article 081303. <a href=\"https://doi.org/10.1063/5.0097506\">https://doi.org/10.1063/5.0097506</a>","mla":"Thiele, Frederik, et al. “Opto-Electronic Bias of a Superconducting Nanowire Single Photon Detector Using a Cryogenic Photodiode.” <i>APL Photonics</i>, vol. 7, no. 8, 081303, AIP Publishing, 2022, doi:<a href=\"https://doi.org/10.1063/5.0097506\">10.1063/5.0097506</a>.","chicago":"Thiele, Frederik, Thomas Hummel, Maximilian Protte, and Tim Bartley. “Opto-Electronic Bias of a Superconducting Nanowire Single Photon Detector Using a Cryogenic Photodiode.” <i>APL Photonics</i> 7, no. 8 (2022). <a href=\"https://doi.org/10.1063/5.0097506\">https://doi.org/10.1063/5.0097506</a>.","bibtex":"@article{Thiele_Hummel_Protte_Bartley_2022, title={Opto-electronic bias of a superconducting nanowire single photon detector using a cryogenic photodiode}, volume={7}, DOI={<a href=\"https://doi.org/10.1063/5.0097506\">10.1063/5.0097506</a>}, number={8081303}, journal={APL Photonics}, publisher={AIP Publishing}, author={Thiele, Frederik and Hummel, Thomas and Protte, Maximilian and Bartley, Tim}, year={2022} }","ama":"Thiele F, Hummel T, Protte M, Bartley T. Opto-electronic bias of a superconducting nanowire single photon detector using a cryogenic photodiode. <i>APL Photonics</i>. 2022;7(8). doi:<a href=\"https://doi.org/10.1063/5.0097506\">10.1063/5.0097506</a>","short":"F. Thiele, T. Hummel, M. Protte, T. Bartley, APL Photonics 7 (2022)."},"user_id":"83846","author":[{"last_name":"Thiele","full_name":"Thiele, Frederik","id":"50819","first_name":"Frederik","orcid":"0000-0003-0663-5587"},{"last_name":"Hummel","full_name":"Hummel, Thomas","first_name":"Thomas","id":"83846"},{"first_name":"Maximilian","id":"46170","full_name":"Protte, Maximilian","last_name":"Protte"},{"last_name":"Bartley","full_name":"Bartley, Tim","id":"49683","first_name":"Tim"}],"status":"public","_id":"33673","intvolume":"         7","publication_identifier":{"issn":["2378-0967"]},"year":"2022","type":"journal_article","publication":"APL Photonics","issue":"8","date_created":"2022-10-11T07:15:09Z","keyword":["Computer Networks and Communications","Atomic and Molecular Physics","and Optics"],"volume":7,"doi":"10.1063/5.0097506","abstract":[{"lang":"eng","text":"<jats:p> Superconducting Nanowire Single Photon Detectors (SNSPDs) have become an integral part of quantum optics in recent years because of their high performance in single photon detection. We present a method to replace the electrical input by supplying the required bias current via the photocurrent of a photodiode situated on the cold stage of the cryostat. Light is guided to the bias photodiode through an optical fiber, which enables a lower thermal conduction and galvanic isolation between room temperature and the cold stage. We show that an off-the-shelf InGaAs–InP photodiode exhibits a responsivity of at least 0.55 A/W at 0.8 K. Using this device to bias an SNSPD, we characterize the count rate dependent on the optical power incident on the photodiode. This configuration of the SNSPD and photodiode shows an expected plateau in the single photon count rate with an optical bias power on the photodiode above 6.8 µW. Furthermore, we compare the same detector under both optical and electrical bias, and show there is no significant changes in performance. This has the advantage of avoiding an electrical input cable, which reduces the latent heat load by a factor of 100 and, in principle, allows for low loss RF current supply at the cold stage. </jats:p>"}]}