{"id":1225,"date":"2024-08-11T13:39:51","date_gmt":"2024-08-11T13:39:51","guid":{"rendered":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/?p=1225"},"modified":"2024-08-11T14:22:44","modified_gmt":"2024-08-11T14:22:44","slug":"gajda-mariusz-frequently-repeated-measurement-of-position-and-momentum-of-a-quantum-particle-2","status":"publish","type":"post","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/gajda-mariusz-frequently-repeated-measurement-of-position-and-momentum-of-a-quantum-particle-2\/","title":{"rendered":"GAJDA MARIUSZ: Frequently repeated measurement of position and momentum of a quantum particle"},"content":{"rendered":"\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\/FOMO2024\/wp-content\/uploads\/2024\/08\/GAJDA-MARIUSZ-Frequently-repeated-measurement-of-position-and-momentum-of-a-quantum-particle-1.pdf\" 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Interferometry of atomic de Broglie waves is a powerful technique for precision measurement. With the 2019 redefinition of the Sl base units, atom interferometry experiments can measure the mass of an atom in kilograms to parts in 1010 [1]. 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Department of Physics, Klingelbergstrasse 82, 4056 Basel, Switzerland\u00a0 2Laboratoire Kastler Brossel, ENS-Universit\u00e9 PSL, CNRS, Universit\u00e9 de la Sorbonne and Coll\u00e8ge de France, 24 rue Lhomond, 75231 Paris, Francephilipp.treutlein@unibas.ch Abstract In 1935, Einstein, Podolsky,\u2026","rel":"","context":"In &quot;Invited Talk&quot;","block_context":{"text":"Invited Talk","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/category\/conference\/talks\/invited-talk\/"},"img":{"alt_text":"","src":"https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/08\/ScreenShotXXX-3.png?resize=350%2C200&ssl=1","width":350,"height":200,"srcset":"https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/08\/ScreenShotXXX-3.png?resize=350%2C200&ssl=1 1x, https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/08\/ScreenShotXXX-3.png?resize=525%2C300&ssl=1 1.5x, 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&quot;Programmes&quot;","block_context":{"text":"Programmes","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/category\/conference\/programmes\/"},"img":{"alt_text":"","src":"https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/09\/ScreenShotXXX-10.png?resize=350%2C200&ssl=1","width":350,"height":200,"srcset":"https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/09\/ScreenShotXXX-10.png?resize=350%2C200&ssl=1 1x, https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/09\/ScreenShotXXX-10.png?resize=525%2C300&ssl=1 1.5x, https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/09\/ScreenShotXXX-10.png?resize=700%2C400&ssl=1 2x"},"classes":[]},{"id":873,"url":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/towards-prime-factorisation-in-holographic-traps\/","url_meta":{"origin":1225,"position":5},"title":"Towards prime factorisation in holographic traps","author":"wvk_3vn943","date":"July 1, 2024","format":false,"excerpt":"Donatella Cassettari Abstract We report the experimental realization of the prime number quantum potential V_N(x), defined as the potential entering the single-particle Schr\u00f6dinger Hamiltonian with eigenvalues given by the first N prime numbers. Using computer-generated holography, we create light intensity profiles suitable to optically trap ultracold atoms in these potentials\u2026","rel":"","context":"In &quot;Conference Videos&quot;","block_context":{"text":"Conference Videos","link":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/category\/conference\/presentation-videos\/"},"img":{"alt_text":"","src":"https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/07\/Cassettari-Towards-prime-factorisation-in-holographic-traps-1.jpg?resize=350%2C200&ssl=1","width":350,"height":200,"srcset":"https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/07\/Cassettari-Towards-prime-factorisation-in-holographic-traps-1.jpg?resize=350%2C200&ssl=1 1x, https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/07\/Cassettari-Towards-prime-factorisation-in-holographic-traps-1.jpg?resize=525%2C300&ssl=1 1.5x, https:\/\/i0.wp.com\/www.matterwaveoptics.eu\/FOMO2024\/wp-content\/uploads\/2024\/07\/Cassettari-Towards-prime-factorisation-in-holographic-traps-1.jpg?resize=700%2C400&ssl=1 2x"},"classes":[]}],"jetpack_sharing_enabled":true,"_links":{"self":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/posts\/1225","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/comments?post=1225"}],"version-history":[{"count":1,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/posts\/1225\/revisions"}],"predecessor-version":[{"id":1230,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/posts\/1225\/revisions\/1230"}],"wp:attachment":[{"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/media?parent=1225"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/categories?post=1225"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/www.matterwaveoptics.eu\/FOMO2024\/wp-json\/wp\/v2\/tags?post=1225"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}