{"id":721,"date":"2021-06-28T17:32:47","date_gmt":"2021-06-28T17:32:47","guid":{"rendered":"https:\/\/www.matterwaveoptics.eu\/?p=721"},"modified":"2021-06-28T17:32:51","modified_gmt":"2021-06-28T17:32:51","slug":"meyer-bernd-transfering-entanglement-from-spin-to-momentum-space","status":"publish","type":"post","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/fomo2021\/contributed-talks\/fomo2021-abstract\/meyer-bernd-transfering-entanglement-from-spin-to-momentum-space\/","title":{"rendered":"Meyer, Bernd &#8212; Transfering entanglement from spin to momentum space"},"content":{"rendered":"\n<p class=\"wp-block-paragraph\">Entanglement has been generated in different atomic systems to improve the sensitivity of phase estimation measurements [1, 2]. However, it is challenging to make use of this entanglement in inertially sensitive atom interferometers. <\/p>\n\n\n\n<p class=\"wp-block-paragraph\">One approach is to generate the entanglement directly in momentum space using nonlinear interactions in Bose-Einstein condensates [3, 4]. In our approach, we first create highly entangled states in spin states and then transfer this entanglement to momentum states. This technique generates entanglement in well separated momentum modes and is therefore an appropriate candidate for future entanglement-enhanced quantum sensors [5].<br>[1] L. Pezz<code>e, A. Smerzi, M. K. Oberthaler, R. Schmied, and P. Treutlein, Quantum metrology with nonclassical states of atomic ensembles, Rev. Mod. Phys. 90, 035005 (2018). <\/code><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><code>[2] S. S. Szigeti, O. Hosten, and S. A. Haine, Improving cold-atom sensors with quantum entanglement: Prospects and challenges, Applied Physics Letters 118, 140501 (2021). <\/code><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><code>[3] S. S. Szigeti, S. P. Nolan, J. D. Close, and S. A. Haine, High-Precision QuantumEnhanced Gravimetry with a Bose-Einstein Condensate, Phys. Rev. Lett. 125, 100402 (2020). <\/code><\/p>\n\n\n\n<p class=\"wp-block-paragraph\"><code>[4] R. Corgier and N. Gaaloul, A. Smerzi, and L. Pezz<\/code>e, Delta-kick Squeezing,<br>arXiv:2103.10896 (2021).<br>[5] F. Anders, A. Idel, P. Feldmann, D. Bondarenko, S. Loriani, K. Lange, J. Peise,<br>M. Gersemann, B. Meyer, S. Abend, N. Gaaloul, C. Schubert, D. Schlippert, L.<br>Santos, E. Rasel, and C. Klempt, Momentum entanglement for atom interferometry,<br>arXiv:2010.15796 (2020).<\/p>\n\n\n\n<div class=\"wp-block-file\"><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/06\/Meyer-Bernd-Transfering-entanglement-from-spin-to-momentum-space.pdf\">Meyer-Bernd-Transfering-entanglement-from-spin-to-momentum-space<\/a><a href=\"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-content\/uploads\/2021\/06\/Meyer-Bernd-Transfering-entanglement-from-spin-to-momentum-space.pdf\" class=\"wp-block-file__button\" download>Download<\/a><\/div>\n","protected":false},"excerpt":{"rendered":"<p>Entanglement has been generated in different atomic systems to improve the<br \/>\nsensitivity of phase estimation measurements [1, 2]. However, it is challenging to<br \/>\nmake use of this entanglement in inertially sensitive atom interferometers.<br \/>\nOne approach is to generate the entanglement directly in momentum space using<br \/>\nnonlinear interactions in Bose-Einstein condensates [3, 4]. In our approach, we<br \/>\nfirst create highly entangled states in spin states and then transfer this entanglement to momentum states. This technique generates entanglement in wellseparated momentum modes and is therefore an appropriate candidate for future<br \/>\nentanglement-enhanced quantum sensors [5].<br \/>\n[1] L. Pezz`e, A. Smerzi, M. K. Oberthaler, R. Schmied, and P. Treutlein, Quantum<br \/>\nmetrology with nonclassical states of atomic ensembles, Rev. Mod. Phys. 90, 035005<br \/>\n(2018).<br \/>\n[2] S. S. Szigeti, O. Hosten, and S. A. Haine, Improving cold-atom sensors with quantum entanglement: Prospects and challenges, Applied Physics Letters 118, 140501<br \/>\n(2021).<br \/>\n[3] S. S. Szigeti, S. P. Nolan, J. D. Close, and S. A. Haine, High-Precision QuantumEnhanced Gravimetry with a Bose-Einstein Condensate, Phys. Rev. Lett. 125, 100402<br \/>\n(2020).<br \/>\n[4] R. Corgier and N. Gaaloul, A. Smerzi, and L. Pezz`e, Delta-kick Squeezing,<br \/>\narXiv:2103.10896 (2021).<br \/>\n[5] F. Anders, A. Idel, P. Feldmann, D. Bondarenko, S. Loriani, K. Lange, J. Peise,<br \/>\nM. Gersemann, B. Meyer, S. Abend, N. Gaaloul, C. Schubert, D. Schlippert, L.<br \/>\nSantos, E. Rasel, and C. Klempt, Momentum entanglement for atom interferometry,<br \/>\narXiv:2010.15796 (2020).<\/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-721","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":"Entanglement has been generated in different atomic systems to improve the sensitivity of phase estimation measurements [1, 2]. However, it is challenging to make use of this entanglement in inertially sensitive atom interferometers. One approach is to generate the entanglement directly in momentum space using nonlinear interactions in Bose-Einstein condensates [3, 4]. In our approach,&hellip;","jetpack_sharing_enabled":true,"publishpress_future_action":{"enabled":false,"date":"2026-07-29 18:46:29","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\/721","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=721"}],"version-history":[{"count":1,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/721\/revisions"}],"predecessor-version":[{"id":723,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/posts\/721\/revisions\/723"}],"wp:attachment":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/media?parent=721"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/categories?post=721"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2022\/wp-json\/wp\/v2\/tags?post=721"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}