{"id":724,"date":"2021-06-28T17:34:48","date_gmt":"2021-06-28T17:34:48","guid":{"rendered":"https:\/\/www.matterwaveoptics.eu\/?p=724"},"modified":"2021-06-28T17:34:52","modified_gmt":"2021-06-28T17:34:52","slug":"tennstedt-benjamin-high-rate-navigation-with-atom-interferometers","status":"publish","type":"post","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/fomo2021\/contributed-talks\/fomo2021-abstract\/tennstedt-benjamin-high-rate-navigation-with-atom-interferometers\/","title":{"rendered":"Tennstedt, Benjamin &#8212; High-rate navigation with atom interferometers"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">Atom Interferometers as inertial sensors were getting quite some interest in the last decade.<br>The superior sensitivity of the sensors is mostly reached by large interrogation times of the atoms.<br>For high-rate navigation scenarios, however, the long measurement intervals and preparation times<br>of the atoms lead to severe systematic errors in the navigation solution.<br>In this contribution a quite promising combination of the atom interferometer and a classical inertial<br>measurement unit (IMU) in an error state extended Kalman Filter framework is presented. This<br>approach aims especially on improving the performance of the conventional IMU, while the<br>drawbacks of the quantum sensor are negated.<\/p>\n\n\n\n<div class=\"wp-block-file\"><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/06\/Tennstedt-Benjamin-High-rate-navigation-with-atom-interferometers.pdf\">Tennstedt-Benjamin-High-rate-navigation-with-atom-interferometers<\/a><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/06\/Tennstedt-Benjamin-High-rate-navigation-with-atom-interferometers.pdf\" class=\"wp-block-file__button\" download>Download<\/a><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Atom Interferometers as inertial sensors were getting quite some interest in the last decade.<br \/>\nThe superior sensitivity of the sensors is mostly reached by large interrogation times of the atoms.<br \/>\nFor high-rate navigation scenarios, however, the long measurement intervals and preparation times<br \/>\nof the atoms lead to severe systematic errors in the navigation solution.<br \/>\nIn this contribution a quite promising combination of the atom interferometer and a classical inertial<br \/>\nmeasurement unit (IMU) in an error state extended Kalman Filter framework is presented. This<br \/>\napproach aims especially on improving the performance of the conventional IMU, while the<br \/>\ndrawbacks of the quantum sensor are negated. <\/p>\n","protected":false},"author":5,"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-724","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":"Cretan Matterwaves","author_link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/author\/bec\/"},"uagb_comment_info":0,"uagb_excerpt":"Atom Interferometers as inertial sensors were getting quite some interest in the last decade. The superior sensitivity of the sensors is mostly reached by large interrogation times of the atoms. For high-rate navigation scenarios, however, the long measurement intervals and preparation times of the atoms lead to severe systematic errors in the navigation solution. In&hellip;","jetpack_sharing_enabled":true,"publishpress_future_action":{"enabled":false,"date":"2026-07-29 18:35:50","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\/724","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\/5"}],"replies":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/comments?post=724"}],"version-history":[{"count":1,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/724\/revisions"}],"predecessor-version":[{"id":726,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/724\/revisions\/726"}],"wp:attachment":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/media?parent=724"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/categories?post=724"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/tags?post=724"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}