{"id":727,"date":"2021-06-28T17:37:57","date_gmt":"2021-06-28T17:37:57","guid":{"rendered":"https:\/\/www.matterwaveoptics.eu\/?p=727"},"modified":"2021-06-28T17:38:00","modified_gmt":"2021-06-28T17:38:00","slug":"bernard-jeanne-progress-towards-the-development-of-a-cold-atom-inertial-measurement-unit-for-onboard-applications","status":"publish","type":"post","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/fomo2021\/contributed-talks\/fomo2021-abstract\/bernard-jeanne-progress-towards-the-development-of-a-cold-atom-inertial-measurement-unit-for-onboard-applications\/","title":{"rendered":"Bernard, Jeanne &#8212; Progress towards the development of a cold-atom inertial measurement unit for onboard applications"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">Cold atom interferometers (AIs) have proven to be extremely sensitive and accurate inertial<br>sensors measuring gravity [1], gravity gradients [2] and rotations [3]. Unlike classical sensors,<br>they do not require any calibration and exhibit an inherent long-term stability and accuracy : they<br>are promising candidates for geodesy, geophysics or inertial navigation. We present our progress<br>towards the development of a cold-atom inertial measurement unit, a device measuring each<br>component of acceleration and rotation. We demonstrate two techniques allowing to perform<br>acceleration measurements using a Mach-Zehnder type AI in a single diffraction regime, even<br>for atoms with close to zero velocity. The first technique lifts the degeneracy between the<br>two Raman transitions \u00b1\u00afhkeff by using a frequency chirp on the Raman lasers. In the second<br>technique, we use the selection rules of the \u03c3+\u03c3\u2212 Raman transitions between the states F =<br>1, mF = \u00b11 and F = 2, mF = \u00b11 to select between one of the two possible transitions. We<br>compare the performances and the bias induced by both methods and highlight their relevance<br>for multiaxis inertial sensors or atom interferometry in a microgravity environment.<\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><br>[1] A. Peters, K. Y. Chung, and S. Chu. High-precision gravity measurements using atom interferometry.<br>Metrologia 38, 25 (2001).<br>[2] J. M. McGuirk, G. T. Foster, J. B. Fixler, M. J. Snadden, and M. A. Kasevich. Sensitive absolutegravity gradiometry using atom interferometry. Phys. Rev. A 65, 033608 (2002).<br>[3] I. Dutta, D. Savoie, B. Fang, B. Venon, C. L. Garrido Alzar, R. Geiger, and A. Landragin. Continuous<br>Cold-Atom Inertial Sensor with 1 nrad\/sec Rotation Stability. Phys. Rev. Lett. 116, 183003 (2016).<br>[4] Y. Bidel, N. Zahzam, C. Blanchard, A. Bonnin, M. Cadoret, A. Bresson, D. Rouxel and M. F.<br>Lequentrec-Lalancette. Absolute marine gravimetry with matter-wave interferometry. Nat. Commun.<br>9, 627 (2018).<br>[5] I. Perrin, J. Bernard,Y. Bidel, A. Bonnin, N. Zahzam, C. Blanchard, A. Bresson, and M. Cadoret.<br>Zero-velocity atom interferometry using a retroreflected frequency-chirped laser. Phys. Rev. A 100,<br>053618 (2019).<\/p>\n\n\n\n<div class=\"wp-block-file\"><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/06\/Bernard-Jeanne-Progress-towards-the-development-of-a-cold-atom-inertial-measurement-unit-for-onboard-applications.pdf\">Bernard-Jeanne-Progress-towards-the-development-of-a-cold-atom-inertial-measurement-unit-for-onboard-applications<\/a><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/06\/Bernard-Jeanne-Progress-towards-the-development-of-a-cold-atom-inertial-measurement-unit-for-onboard-applications.pdf\" class=\"wp-block-file__button\" download>Download<\/a><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Cold atom interferometers (AIs) have proven to be extremely sensitive and accurate inertial<br \/>\nsensors measuring gravity [1], gravity gradients [2] and rotations [3]. Unlike classical sensors,<br \/>\nthey do not require any calibration and exhibit an inherent long-term stability and accuracy : they<br \/>\nare promising candidates for geodesy, geophysics or inertial navigation. We present our progress<br \/>\ntowards the development of a cold-atom inertial measurement unit, a device measuring each<br \/>\ncomponent of acceleration and rotation. We demonstrate two techniques allowing to perform<br \/>\nacceleration measurements using a Mach-Zehnder type AI in a single diffraction regime, even<br \/>\nfor atoms with close to zero velocity. The first technique lifts the degeneracy between the<br \/>\ntwo Raman transitions \u00b1\u00afhkeff by using a frequency chirp on the Raman lasers. In the second<br \/>\ntechnique, we use the selection rules of the \u03c3+\u03c3\u2212 Raman transitions between the states F =<br \/>\n1, mF = \u00b11 and F = 2, mF = \u00b11 to select between one of the two possible transitions. We<br \/>\ncompare the performances and the bias induced by both methods and highlight their relevance<br \/>\nfor multiaxis inertial sensors or atom interferometry in a microgravity environment.<br \/>\n[1] A. Peters, K. Y. Chung, and S. Chu. High-precision gravity measurements using atom interferometry.<br \/>\nMetrologia 38, 25 (2001).<br \/>\n[2] J. M. McGuirk, G. T. Foster, J. B. Fixler, M. J. Snadden, and M. A. Kasevich. Sensitive absolutegravity gradiometry using atom interferometry. Phys. Rev. A 65, 033608 (2002).<br \/>\n[3] I. Dutta, D. Savoie, B. Fang, B. Venon, C. L. Garrido Alzar, R. Geiger, and A. Landragin. Continuous<br \/>\nCold-Atom Inertial Sensor with 1 nrad\/sec Rotation Stability. Phys. Rev. Lett. 116, 183003 (2016).<br \/>\n[4] Y. Bidel, N. Zahzam, C. Blanchard, A. Bonnin, M. Cadoret, A. Bresson, D. Rouxel and M. F.<br \/>\nLequentrec-Lalancette. Absolute marine gravimetry with matter-wave interferometry. Nat. Commun.<br \/>\n9, 627 (2018).<br \/>\n[5] I. Perrin, J. Bernard,Y. Bidel, A. Bonnin, N. Zahzam, C. Blanchard, A. Bresson, and M. Cadoret.<br \/>\nZero-velocity atom interferometry using a retroreflected frequency-chirped laser. Phys. Rev. A 100,<br \/>\n053618 (2019).<\/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-727","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":"Cold atom interferometers (AIs) have proven to be extremely sensitive and accurate inertial sensors measuring gravity [1], gravity gradients [2] and rotations [3]. Unlike classical sensors, they do not require any calibration and exhibit an inherent long-term stability and accuracy : they are promising candidates for geodesy, geophysics or inertial navigation. We present our progress&hellip;","jetpack_sharing_enabled":true,"publishpress_future_action":{"enabled":false,"date":"2026-07-29 19:43:16","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\/727","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=727"}],"version-history":[{"count":1,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/727\/revisions"}],"predecessor-version":[{"id":729,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/727\/revisions\/729"}],"wp:attachment":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/media?parent=727"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/categories?post=727"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/tags?post=727"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}