{"id":4508,"date":"2025-10-31T08:39:05","date_gmt":"2025-10-31T12:39:05","guid":{"rendered":"https:\/\/oge.mit.edu\/msrp\/?post_type=profiles&#038;p=4508"},"modified":"2025-12-09T11:56:47","modified_gmt":"2025-12-09T16:56:47","slug":"hanson-nguyen-2","status":"publish","type":"profiles","link":"https:\/\/oge.mit.edu\/msrp\/profiles\/hanson-nguyen-2\/","title":{"rendered":"Hanson Nguyen"},"content":{"rendered":"<div class=\"wp-block-image\">\n<figure class=\"alignleft size-full is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"2560\" height=\"2560\" src=\"https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-scaled.jpg\" alt=\"\" class=\"wp-image-4509\" style=\"width:200px;height:auto\" srcset=\"https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-scaled.jpg 2560w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-300x300.jpg 300w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-1024x1024.jpg 1024w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-150x150.jpg 150w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-768x768.jpg 768w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-1536x1536.jpg 1536w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/11\/NguyenHanson-edited-2048x2048.jpg 2048w\" sizes=\"auto, (max-width: 2560px) 100vw, 2560px\" \/><\/figure>\n<\/div>\n\n\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<p><strong>MIT Department:<\/strong> Electrical Engineering and Computer Science<br><strong>Faculty Mentor<\/strong>: Prof. Karl Berggren<br><strong>Research Supervisor:<\/strong> Alejandro Simon<br><strong>Undergraduate Institution:<\/strong> Arizona State University<br><strong>Website<\/strong>:<\/p>\n<\/div><\/div>\n\n\n\n<div style=\"height:0px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h4 class=\"wp-block-heading\"><strong>Biography<\/strong><\/h4>\n\n\n\n<p>Hanson H. Nguyen is a rising senior at the Barrett Honors College atASU, majoringin Electrical Engineering and minoring in Mathematics. His research has centered on next-generation integrated-circuit platforms\u2014ranging from photonic to superconducting devices\u2014that promise secure, energy-efficient building blocks for new computing regimes, including quantum and high performance computing. He has joined research groups atASU, MIT, and Purdue, published two first-author papers, and presented both at local and international conferences. Hanson plans to pursue a PhD in Applied Physics to continue developing devices that address today\u2019s computational demands with an emphasis on security and sustainability.Committed to accessibility in STEM education, Hanson has mentored K-12 teachers andstudents, and designed hands-on tools and curricula through an NSF-funded ResearchExperiences for Teachers program. He is currently a student ambassador for ASU\u2019s Electrical Engineering department. In his free time, Hanson enjoys spinning records, doodling over lecture notes, and reading comics.<\/p>\n\n\n\n<h4 class=\"wp-block-heading\"><strong>Abstract<\/strong><\/h4>\n\n\n\n<p class=\"has-text-align-center\"><strong>Thermal and Electronic Reset Times of Superconducting Nanowire Single Photon Detectors<\/strong><\/p>\n\n\n\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-group is-vertical is-content-justification-center is-nowrap is-layout-flex wp-container-core-group-is-layout-73832be3 wp-block-group-is-layout-flex\">\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<p class=\"has-text-align-center\"><strong>Hanson H. Nguyen<sup>1<\/sup>, Alejandro Simon<sup>2<\/sup>, and Karl K. Berggren<sup>2<\/sup><\/strong><\/p>\n\n\n\n<div class=\"wp-block-group\"><div class=\"wp-block-group__inner-container is-layout-constrained wp-block-group-is-layout-constrained\">\n<div class=\"wp-block-group is-vertical is-content-justification-center is-layout-flex wp-container-core-group-is-layout-4b2eccd6 wp-block-group-is-layout-flex\">\n<p class=\"has-text-align-center\"><sup>1<\/sup>School of Electrical, Computer and Energy Engineering, Arizona State University<\/p>\n\n\n\n<p class=\"has-text-align-center\"><sup>2<\/sup>Department of Electrical Engineering and Computer Science, Massachusetts Institute of Technology<\/p>\n<\/div>\n<\/div><\/div>\n<\/div><\/div>\n<\/div>\n<\/div><\/div>\n\n\n\n<p class=\"has-text-align-center\"><\/p>\n<\/div><\/div>\n\n\n\n<p>Superconducting nanowire single-photon detectors (SNSPDs) are ultra-sensitive devices capable of detecting individual photons with high detection efficiency, ultra-low dark count rates, and record low timing jitter time. Thus, SNSPDs have been valuable for applications that require precise photon detection or counting, such as quantum optics, fiber-optic communications, and LiDAR systems. These detectors operate by biasing a superconducting nanowire just below its maximum superconducting current, where the absorption of a single photon can disrupt the superconductivity, leading to the formation of a resistive region. After each detection event, the device undergoes a recovery process governed by the electronic reset time, which determines how quickly the bias current returns, and the thermal relaxation time, which dictates how rapidly the nanowire cools. Here, we model these processes using electrothermal SPICE simulations and design a cryogenic measurement scheme to determine the reset time of SNSPD devices. By illuminating the detector with a continuous-wave laser and recording photon arrival times, we apply statistical analyses to the photon interarrival times. We observe the kinetic-inductance-limited reset time, as well as thermal dynamics manifesting through after-pulsing, relaxation oscillations, and latching, which provides insight into how electronic and thermal reset dynamics jointly determine the maximum count rate of SNSPDs.<\/p>\n","protected":false},"featured_media":4509,"template":"","profile_category":[23],"class_list":["post-4508","profiles","type-profiles","status-publish","has-post-thumbnail","hentry","profile_category-2025-interns"],"acf":[],"_links":{"self":[{"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profiles\/4508","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profiles"}],"about":[{"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/types\/profiles"}],"version-history":[{"count":3,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profiles\/4508\/revisions"}],"predecessor-version":[{"id":4833,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profiles\/4508\/revisions\/4833"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/media\/4509"}],"wp:attachment":[{"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/media?parent=4508"}],"wp:term":[{"taxonomy":"profile_category","embeddable":true,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profile_category?post=4508"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}