{"id":1509,"date":"2010-02-01T21:37:00","date_gmt":"2010-02-01T20:37:00","guid":{"rendered":"https:\/\/gqm.lpl.univ-paris13.fr\/?p=1509"},"modified":"2025-11-08T16:25:09","modified_gmt":"2025-11-08T15:25:09","slug":"control-of-dipolar-relaxation-in-external-fields","status":"publish","type":"post","link":"https:\/\/gqm.lpl.univ-paris13.fr\/index.php\/2010\/02\/01\/control-of-dipolar-relaxation-in-external-fields\/","title":{"rendered":"Control of dipolar relaxation in external fields"},"content":{"rendered":"\n<div class=\"wp-block-columns is-layout-flex wp-container-core-columns-is-layout-28f84493 wp-block-columns-is-layout-flex\">\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:66.66%\">\n<p>Although dipolar relaxation generally increases as a function of a static magnetic-field intensity, we find a range of nonzero magnetic-field intensities where dipolar relaxation is strongly reduced. We use this resonant reduction to accurately determine the \ud835\udc46=6 scattering length of Cr atoms: \ud835\udc4e<sub>6<\/sub>=103\u00b14\u2062\ud835\udc4e<sub>0<\/sub>. We compare this new measurement to another new determination of \ud835\udc4e<sub>6<\/sub>, which we perform by analyzing the precise spectroscopy of a Feshbach resonance in \ud835\udc51-wave collisions, yielding \ud835\udc4e6=102.5\u00b10.4\u2062\ud835\udc4e0. These two measurements provide, by far, the most precise determination of \ud835\udc4e<sub>6<\/sub> to date.<\/p>\n\n\n\n<p>We then show that, although dipolar interactions are long-range interactions, dipolar relaxation only involves the incoming partial wave \ud835\udc59=0 for large enough magnetic-field intensities, which has interesting consequences on the stability of dipolar Fermi gases. We then study ultracold Cr gases in a one-dimensional (1D) optical lattice resulting in a collection of independent 2D gases. We show that dipolar relaxation is modified when the atoms collide in reduced dimensionality at low magnetic-field intensities, and that the corresponding dipolar relaxation rate parameter is reduced by a factor up to 7 compared to the 3D case.<\/p>\n\n\n\n<p>Finally, we study dipolar relaxation in the presence of RF oscillating magnetic fields, and we show that both the output channel energy and the transition amplitude can be controlled by means of the RF frequency and Rabi frequency.<\/p>\n<\/div>\n\n\n\n<div class=\"wp-block-column is-vertically-aligned-center is-layout-flow wp-block-column-is-layout-flow\" style=\"flex-basis:33.33%\">\n<figure class=\"wp-block-image aligncenter size-full has-custom-border is-style-rounded wp-duotone-unset-1\" id=\"wp-block-themeisle-blocks-image-11cfb22b\" style=\"margin-top:var(--wp--preset--spacing--20);margin-right:var(--wp--preset--spacing--20);margin-bottom:var(--wp--preset--spacing--20);margin-left:var(--wp--preset--spacing--20)\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/gqm.lpl.univ-paris13.fr\/wp-content\/uploads\/2025\/11\/Article-Control-dipolar-relaxation-341638.svg\" alt=\"\" class=\"wp-image-1653\" style=\"border-style:none;border-width:0px;border-radius:10px\"\/><figcaption class=\"wp-element-caption\">Dipolar relaxation loss parameter as a function of magnetic field, in the lattice (filled triangles) and without the lattice (open triangles).<\/figcaption><\/figure>\n<\/div>\n<\/div>\n","protected":false},"excerpt":{"rendered":"<p>We study dipolar relaxation in both ultracold thermal and Bose-condensed Cr atom gases. We show three different ways to control dipolar relaxation, making use of either a static magnetic field, an oscillatory magnetic field, or an optical lattice to reduce the dimensionality of the gas from three-dimensional (3D) to two-dimensional (2D).<br \/>\n<a href=\"https:\/\/doi.org\/10.48550\/arXiv.1002.0222\">arXiv:1002.0222 (2010)<\/a>  \/  <a href=\"https:\/\/doi.org\/10.1103\/PhysRevA.81.042716\">Phys. Rev. A 81, 042716 (2010)<\/a><\/p>\n","protected":false},"author":3,"featured_media":1653,"comment_status":"closed","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"_themeisle_gutenberg_block_has_review":false,"_jetpack_memberships_contains_paid_content":false,"footnotes":""},"categories":[18,63,129],"tags":[269,28,26,31,77,61,42,44,151],"class_list":["post-1509","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-article","category-chromium","category-theory","tag-anne-crubellier","tag-benjamin-pasquiou","tag-bruno-laburthe-tolra","tag-etienne-marechal","tag-gabriel-bismut","tag-laurent-vernac","tag-olivier-gorceix","tag-paolo-pedri","tag-quentin-beaufils"],"blocksy_meta":[],"yoast_head":"<!-- This site is optimized with the Yoast SEO plugin v27.4 - https:\/\/yoast.com\/product\/yoast-seo-wordpress\/ -->\n<title>Control of dipolar relaxation in external fields - Magnetic Quantum Gases<\/title>\n<meta name=\"robots\" content=\"index, follow, max-snippet:-1, max-image-preview:large, max-video-preview:-1\" \/>\n<link rel=\"canonical\" href=\"https:\/\/gqm.lpl.univ-paris13.fr\/index.php\/2010\/02\/01\/control-of-dipolar-relaxation-in-external-fields\/\" \/>\n<meta property=\"og:locale\" content=\"en_US\" \/>\n<meta property=\"og:type\" content=\"article\" \/>\n<meta property=\"og:title\" content=\"Control of dipolar relaxation in external fields - Magnetic Quantum Gases\" \/>\n<meta property=\"og:description\" content=\"We study dipolar relaxation in both ultracold thermal and Bose-condensed Cr atom gases. We show three different ways to control dipolar relaxation, making use of either a static magnetic field, an oscillatory magnetic field, or an optical lattice to reduce the dimensionality of the gas from three-dimensional (3D) to two-dimensional (2D). arXiv:1002.0222 (2010) \/ Phys. Rev. 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