{"id":554,"date":"2021-06-27T15:39:21","date_gmt":"2021-06-27T15:39:21","guid":{"rendered":"https:\/\/www.matterwaveoptics.eu\/?p=554"},"modified":"2021-06-27T15:39:25","modified_gmt":"2021-06-27T15:39:25","slug":"atkocius-vilius-ring-lattice-trap-for-neutral-atoms-with-rf-dressed-time-averaged-adiabatic-potentials","status":"publish","type":"post","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/fomo2021\/contributed-talks\/fomo2021-abstract\/atkocius-vilius-ring-lattice-trap-for-neutral-atoms-with-rf-dressed-time-averaged-adiabatic-potentials\/","title":{"rendered":"Atkocius, Vilius  &#8212; Ring lattice trap for neutral atoms with RF-dressed time-averaged adiabatic potentials"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">We are working towards a matter-wave interferometer based on\u00a0Sagnac\u00a0effect that requires atoms to traverse an enclosed path to accumulate phase. Our scheme relies on time-averaged adiabatic RF-dressed potentials (TAAP) to guide neutral atoms around a circular path which will provide a scalable approach towards building a compact atom-based rotation sensor. I will present to you our method to create a fully guided ring lattice trap on an atom chip setup.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>We are working towards a matter-wave interferometer based on Sagnac effect that requires atoms to traverse an enclosed path to accumulate phase. Our scheme relies on time-averaged adiabatic RF-dressed potentials (TAAP) to guide neutral atoms around a circular path which will provide a scalable approach towards building a compact atom-based rotation sensor. I will present to you our method to create a fully guided ring lattice trap on an atom chip setup.<\/p>\n","protected":false},"author":4,"featured_media":0,"comment_status":"closed","ping_status":"closed","sticky":false,"template":"","format":"standard","meta":{"_crdt_document":"","_uag_custom_page_level_css":"","_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"_jetpack_memberships_contains_paid_content":false,"footnotes":""},"categories":[6],"tags":[],"class_list":["post-554","post","type-post","status-publish","format-standard","hentry","category-fomo2021-abstract"],"jetpack_featured_media_url":"","uagb_featured_image_src":{"full":false,"thumbnail":false,"medium":false,"medium_large":false,"large":false,"1536x1536":false,"2048x2048":false,"ashe-slider-full-thumbnail":false,"ashe-full-thumbnail":false,"ashe-list-thumbnail":false,"ashe-grid-thumbnail":false,"ashe-single-navigation":false},"uagb_author_info":{"display_name":"Wolf von Klitzing","author_link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/author\/klitzing\/"},"uagb_comment_info":0,"uagb_excerpt":"We are working towards a matter-wave interferometer based on Sagnac effect that requires atoms to traverse an enclosed path to accumulate phase. Our scheme relies on time-averaged adiabatic RF-dressed potentials (TAAP) to guide neutral atoms around a circular path which will provide a scalable approach towards building a compact atom-based rotation sensor. I will present&hellip;","jetpack_sharing_enabled":true,"publishpress_future_action":{"enabled":false,"date":"2026-07-29 19:48:33","action":"category","newStatus":"draft","terms":[],"taxonomy":"category","extraData":[]},"publishpress_future_workflow_manual_trigger":{"enabledWorkflows":[]},"_links":{"self":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/554","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/users\/4"}],"replies":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/comments?post=554"}],"version-history":[{"count":1,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/554\/revisions"}],"predecessor-version":[{"id":555,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/554\/revisions\/555"}],"wp:attachment":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/media?parent=554"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/categories?post=554"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/tags?post=554"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}