{"id":589,"date":"2021-06-27T18:42:21","date_gmt":"2021-06-27T18:42:21","guid":{"rendered":"https:\/\/www.matterwaveoptics.eu\/?p=589"},"modified":"2021-07-08T14:21:03","modified_gmt":"2021-07-08T14:21:03","slug":"gerstenecker-benedikt-ultracold-caesium-on-an-atomchip-an-atom-interferometer-with-tunable-interactions","status":"publish","type":"post","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/fomo2021\/contributed-talks\/fomo2021-abstract\/gerstenecker-benedikt-ultracold-caesium-on-an-atomchip-an-atom-interferometer-with-tunable-interactions\/","title":{"rendered":"Gerstenecker, Benedikt &#8212; Ultracold Caesium on an Atomchip: An Atom Interferometer with Tunable Interactions"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">The matter-wave properties of atoms and the macroscopic behavior of Bose-Einstein condensates make interference experiments with ultracold atoms a useful tool for both fundamental research and metrology applications. A unique design allows us to combine the advantages of atomchip technology with the flexibility of optical traps and furthermore the favorable magnetically induced Feshbach resonances in Caesium, which are well-suited for interaction-tuning and therefore enable condensation of this challenging atomic species. The tunability of the atoms&#8217; scattering length and the convenient access to the trap characteristics will give us full control over the crucial parameters, allowing for the simulation of different regimes of two-mode systems as well as for competing with the sensitivity of large interferometric sensors despite a much more compact setup.<\/p>\n\n\n\n<h2 class=\"wp-block-heading\">Presentation:<\/h2>\n\n\n\n<div data-wp-interactive=\"core\/file\" class=\"wp-block-file\"><object data-wp-bind--hidden=\"!state.hasPdfPreview\" hidden class=\"wp-block-file__embed\" data=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/07\/Gerstenecker-Benedikt-Ultracold-Caesium-on-an-Atomchip-An-Atom-Interferometer-with-Tunable-Interactions.pdf\" type=\"application\/pdf\" style=\"width:100%;height:600px\" aria-label=\"Embed of Embed of Gerstenecker-Benedikt-Ultracold-Caesium-on-an-Atomchip-An-Atom-Interferometer-with-Tunable-Interactions..\"><\/object><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/07\/Gerstenecker-Benedikt-Ultracold-Caesium-on-an-Atomchip-An-Atom-Interferometer-with-Tunable-Interactions.pdf\">Gerstenecker-Benedikt-Ultracold-Caesium-on-an-Atomchip-An-Atom-Interferometer-with-Tunable-Interactions<\/a><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/07\/Gerstenecker-Benedikt-Ultracold-Caesium-on-an-Atomchip-An-Atom-Interferometer-with-Tunable-Interactions.pdf\" class=\"wp-block-file__button\" download>Download<\/a><\/div>\n","protected":false},"excerpt":{"rendered":"<p>The matter-wave properties of atoms and the macroscopic behavior of Bose-Einstein condensates make interference experiments with ultracold atoms a useful tool for both fundamental research and metrology applications. A unique design allows us to combine the advantages of atomchip technology with the flexibility of optical traps and furthermore the favorable magnetically induced Feshbach resonances in Caesium, which are well-suited for interaction-tuning and therefore enable condensation of this challenging atomic species. The tunability of the atoms&#8217; scattering length and the convenient access to the trap characteristics will give us full control over the crucial parameters, allowing for the simulation of different regimes of two-mode systems as well as for competing with the sensitivity of large interferometric sensors despite a much more compact 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":[6,18],"tags":[],"class_list":["post-589","post","type-post","status-publish","format-standard","hentry","category-fomo2021-abstract","category-presentations"],"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":"The matter-wave properties of atoms and the macroscopic behavior of Bose-Einstein condensates make interference experiments with ultracold atoms a useful tool for both fundamental research and metrology applications. A unique design allows us to combine the advantages of atomchip technology with the flexibility of optical traps and furthermore the favorable magnetically induced Feshbach resonances in&hellip;","jetpack_sharing_enabled":true,"publishpress_future_action":{"enabled":false,"date":"2026-08-21 20:30:10","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\/589","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=589"}],"version-history":[{"count":4,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/589\/revisions"}],"predecessor-version":[{"id":1016,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/589\/revisions\/1016"}],"wp:attachment":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/media?parent=589"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/categories?post=589"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/tags?post=589"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}