{"id":4298,"date":"2025-10-08T12:58:54","date_gmt":"2025-10-08T16:58:54","guid":{"rendered":"https:\/\/oge.mit.edu\/msrp\/?post_type=profiles&#038;p=4298"},"modified":"2025-12-09T11:23:59","modified_gmt":"2025-12-09T16:23:59","slug":"jaime-alvarez-2","status":"publish","type":"profiles","link":"https:\/\/oge.mit.edu\/msrp\/profiles\/jaime-alvarez-2\/","title":{"rendered":"Jaime Alvarez"},"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\/10\/Alvarez-Jaime-edited-scaled.jpg\" alt=\"\" class=\"wp-image-4308\" style=\"width:200px;height:auto\" srcset=\"https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/10\/Alvarez-Jaime-edited-scaled.jpg 2560w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/10\/Alvarez-Jaime-edited-300x300.jpg 300w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/10\/Alvarez-Jaime-edited-1024x1024.jpg 1024w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/10\/Alvarez-Jaime-edited-150x150.jpg 150w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/10\/Alvarez-Jaime-edited-768x768.jpg 768w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/10\/Alvarez-Jaime-edited-1536x1536.jpg 1536w, https:\/\/oge.mit.edu\/msrp\/wp-content\/uploads\/sites\/2\/2025\/10\/Alvarez-Jaime-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>Physics<br><strong>Faculty Mentor<\/strong>: Prof. Nergis Mavalvala<br><strong>Research Supervisor: <\/strong>Eric Oelker, Beg\u00fcm Kabag\u00f6z<br><strong>Undergraduate Institution:<\/strong> University of California, Berkley<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<p><\/p>\n\n\n\n<h4 class=\"wp-block-heading\"><strong>Biography<\/strong><\/h4>\n\n\n\n<p>Jaime Alvarez is a rising senior majoring in Physics at the University of California, Berkeley.He hopes to obtain a PhD in Physics and pursue an academic career. At the University of Southern California, he worked with Dr. Kris Pardo, using astrometric techniques to explore properties of gravitational waves, focusing on the chirp mass and distance of supermassive black hole binaries.At MIT, Jaime works with Dr. Nergis Mavalvala and Dr. Eric Oelker in the Laser Interferometer Gravitational-Wave Observatory (LIGO) lab. During the summer of 2024, he worked on the GRAVITES project, where he built a servo board for laser stabilization and assembled a high vacuum chamber for optical noise reduction. For the summer of 2025, he is returning to the MIT LIGO lab to assist with the assembling and characterizing of a new Optical Parametric Oscillator (OPO) cavity for the LIGO Hanford Observatory. He is also helping develop a prototype squeezed light source to study new nonlinear materials for squeezed vacuum generation to increase the source&#8217;s lifetime and reduce optical loss. Jaime hopes to inspire others to pursue their curiosity and achieve their goals, regardless of their background<\/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>Higher Order Mode Generation for Optical Damping of Parametric Instabilities in LIGO<\/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<p class=\"has-text-align-center\"><strong>Jaime Alvarez<sup>1<\/sup>, Beg\u00fcm Kabag\u00f6z<sup>2<\/sup>, Eric Oelker<sup>2<\/sup>, and Nergis Mavalvala<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><sup>1<\/sup>Department of Physics, University of California, Berkeley<\/p>\n\n\n\n<p><sup>2<\/sup>Department of Physics, Massachusetts Institute of Technology<\/p>\n<\/div>\n<\/div><\/div>\n<\/div>\n<\/div><\/div>\n<\/div><\/div>\n\n\n\n<p class=\"has-text-align-center\"><\/p>\n\n\n\n<p>During the most recent observation run of the Laser Interferometer Gravitational-Wave Observatory (LIGO), the detector suffered multiple lock losses due to parametric instabilities(PIs) driven by higher-order modes (HOMs) in the interferometer arm cavities. Currently, certain PIs are mitigated by the thermal compensation system (TCS), which shifts the resonant frequency of the HOMs to stable positions. However, as arm power increases, PIs become increasingly disruptive, and the TCS method is no longer viable. A more robust method is optical damping, which involves injecting a HOM with the opposite phase to dampen the PI-coupled target mode. In this project, we aim to generate target HOMs for injection into the cavities. We first developed a script implementing the Gerchberg-Saxton algorithm for phase mask generation, typically achieving over 95% beam overlap after approximately 20-30 iterations. We then built a tabletop setup using a spatial light modulator with two phase masks on its screen; the first allows amplitude shaping, while the second corrects phase. In the future, we will characterize the generated beam profiles with a phase camera, then inject them into a reference cavity to assess mode coupling. Ultimately, implementing optical damping will help\nsuppress PIs and improve LIGO\u2019s stability and observation time.\n\n<\/p>\n","protected":false},"featured_media":4308,"template":"","profile_category":[23],"class_list":["post-4298","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\/4298","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":5,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profiles\/4298\/revisions"}],"predecessor-version":[{"id":4777,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profiles\/4298\/revisions\/4777"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/media\/4308"}],"wp:attachment":[{"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/media?parent=4298"}],"wp:term":[{"taxonomy":"profile_category","embeddable":true,"href":"https:\/\/oge.mit.edu\/msrp\/wp-json\/wp\/v2\/profile_category?post=4298"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}