{"id":462,"date":"2025-01-30T11:15:50","date_gmt":"2025-01-30T11:15:50","guid":{"rendered":"https:\/\/mora.ganil-spiral2.eu\/?page_id=462"},"modified":"2025-11-04T17:24:15","modified_gmt":"2025-11-04T17:24:15","slug":"publications","status":"publish","type":"page","link":"https:\/\/mora.ganil-spiral2.eu\/?page_id=462","title":{"rendered":"Publications"},"content":{"rendered":"\t\t<div data-elementor-type=\"wp-page\" data-elementor-id=\"462\" class=\"elementor elementor-462\">\n\t\t\t\t\t\t<div class=\"elementor-inner\">\n\t\t\t\t<div class=\"elementor-section-wrap\">\n\t\t\t\t\t\t\t\t\t<section class=\"elementor-section elementor-top-section elementor-element elementor-element-996752b elementor-section-boxed elementor-section-height-default elementor-section-height-default\" data-id=\"996752b\" data-element_type=\"section\">\n\t\t\t\t\t\t<div class=\"elementor-container elementor-column-gap-default\">\n\t\t\t\t\t\t\t<div class=\"elementor-row\">\n\t\t\t\t\t<div class=\"elementor-column elementor-col-100 elementor-top-column elementor-element elementor-element-d593179\" data-id=\"d593179\" data-element_type=\"column\">\n\t\t\t<div class=\"elementor-column-wrap elementor-element-populated\">\n\t\t\t\t\t\t\t<div class=\"elementor-widget-wrap\">\n\t\t\t\t\t\t<div class=\"elementor-element elementor-element-f0649af elementor-widget elementor-widget-text-editor\" data-id=\"f0649af\" data-element_type=\"widget\" data-widget_type=\"text-editor.default\">\n\t\t\t\t<div class=\"elementor-widget-container\">\n\t\t\t\t\t\t\t\t<div class=\"elementor-text-editor elementor-clearfix\">\n\t\t\t\t<ul><li><a href=\"https:\/\/doi.org\/10.1007\/s10751-019-1611-x\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">P. Delahaye<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, E. Li\u00e9nard, I. Moore, et <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">al., <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">The MORA <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">project<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, Hyperfine <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Interact<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\"> (2019) 240: 63.<\/span><\/a><\/li><li><a href=\"https:\/\/doi.org\/10.1140\/epja\/i2019-12740-4\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">P. Delahaye,<\/span> <span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">Analytical<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\"> model of an ion cloud <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">cooled<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\"> by collisions<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Eur<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">. Phys. J. A (2019) 55: 83.<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">.<\/span><\/a><\/li><li><a href=\"https:\/\/doi.org\/10.1140\/epja\/i2019-12777-3\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">P. Delahaye, G. Ban, M. Benali et al<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">., <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">The open LPC <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">trap<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\"> for <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">precision<\/span> <span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">measurements<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\"> in beta <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">decay<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Eur<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">. Phys. J. A (2019) 55: 101.<\/span><\/a><\/li><li><a href=\"https:\/\/doi.org\/10.1140\/epja\/s10050-020-00168-y\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">M. Benali M., G. <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Quemener<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, P. Delahaye et al, <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">Geometry <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">optimisation<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\"> of a transparent axisymmetric ion trap for the MORA <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">project<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, Eur. Phys. J. A (2020) 56: <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">163.<\/span><\/a><\/li><li><a href=\"https:\/\/doi.org\/10.1007\/JHEP04%282021%29126\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">A. Falkowski, M. Gonzalez Alonso and O. Naviliat <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Cuncic<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">,<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\"> Comprehensive analysis of beta <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">decays within <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">and beyond the Standard <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black;font-style: italic\">Model<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">arXiv:2010.13797<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, JHEP04(2021)126<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">.<\/span><\/a><\/li><li><a href=\"https:\/\/doi.org\/10.48550\/arXiv.2112.07688\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">A. Falkowski, M. Gonz\u00e1lez-Alonso, A. <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Palavri\u0107<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, A. Rodr\u00edguez-S\u00e1nchez, Constraints on <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">subleading<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\"> interactions in beta decay <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Lagrangian<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">arXiv:2112.07688\u00a0<\/span><\/a><\/li><li><a href=\"https:\/\/doi.org\/10.48550\/arXiv.2207.02161\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">A. Falkowski, A. Rodr\u00edguez-S\u00e1nchez, On the sensitivity of the D parameter to new physics<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">, arXiv:2207.02161.<\/span><\/a><\/li><li><a href=\"https:\/\/doi.org\/10.1088\/1742-6596\/2586\/1\/012142\"><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">N. Goyal et al., detection of recoil ion in the beta decay of laser oriented\u00a0 trapped radioactive isotopes for the MORA project, J. <\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">Phys:Conf<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">. Ser. 2586 012142 (INPC 2022).<\/span><\/a><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\"><br \/><\/span><\/li><li><span style=\"color: #000000\"><a style=\"color: #000000\" href=\"https:\/\/doi.org\/10.48550\/arXiv.2412.17702\">E. Alviani and A. Falkowski, On the Coulomb corrections in nuclear beta decay, arXiv:2412.17702 [hep-ph].<\/a><\/span><\/li><li><span style=\"font-size: 12pt;font-family: Calibri;color: #ff0000;font-weight: bold\">Now in EPJ A and arXiv<\/span><span style=\"font-size: 12.0pt;font-family: Calibri;color: black\">: <strong>N. Goyal,\u00a0 A. Singh, S. Daumas-Tschopp, L. M. Motilla et al., <\/strong><\/span><span style=\"color: #333333\"><strong>Performance of the MORA Apparatus for Testing Time-Reversal Invariance in Nuclear Beta Decay,<\/strong><\/span>\u00a0<strong><span style=\"color: #000000\">Eur. Phys. J. A (2025) 61: 221,<\/span>\u00a0<\/strong><strong><a href=\"https:\/\/doi.org\/10.1140\/epja\/s10050-025-01694-3\" target=\"_blank\" rel=\"noopener\"> https:\/\/doi.org\/10.1140\/epja\/s10050-025-01694-3<\/a><\/strong><\/li><\/ul>\t\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/div>\n\t\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t<\/section>\n\t\t\t\t\t\t\t\t\t<\/div>\n\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t","protected":false},"excerpt":{"rendered":"<p>P. Delahaye, E. Li\u00e9nard, I. Moore, et al., The MORA project, Hyperfine Interact (2019) 240: 63. P. Delahaye, Analytical model of an ion cloud cooled by collisions, Eur. Phys. J. A (2019) 55: 83.. P. Delahaye, G. Ban, M. Benali &hellip; <a href=\"https:\/\/mora.ganil-spiral2.eu\/?page_id=462\">Continue reading <span class=\"meta-nav\">&rarr;<\/span><\/a><\/p>\n","protected":false},"author":7,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":[],"_links":{"self":[{"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=\/wp\/v2\/pages\/462"}],"collection":[{"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=\/wp\/v2\/users\/7"}],"replies":[{"embeddable":true,"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=462"}],"version-history":[{"count":13,"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=\/wp\/v2\/pages\/462\/revisions"}],"predecessor-version":[{"id":642,"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=\/wp\/v2\/pages\/462\/revisions\/642"}],"wp:attachment":[{"href":"https:\/\/mora.ganil-spiral2.eu\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=462"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}