{"id":57,"date":"2009-10-10T12:56:34","date_gmt":"2009-10-10T09:56:34","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=57"},"modified":"2011-06-02T13:04:04","modified_gmt":"2011-06-02T10:04:04","slug":"paper-magnetic-moments-of-33mg-in-the-time-odd-relativistic-mean-field-approach","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=57","title":{"rendered":"[paper] Magnetic moments of <sup>33<\/sup>Mg in the time-odd relativistic mean field approach"},"content":{"rendered":"<p><em>Magnetic moments of <sup>33<\/sup>Mg in the time-odd relativistic mean field approach<\/em><\/p>\n<p>Jian Li <em>et al.<\/em><\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1007\/s11433-009-0194-y\">10.1007\/s11433-009-0194-y<\/a><\/p>\n<p>The configuration-fixed deformation constrained relativistic mean field approach with time-odd component has been applied to investigate the ground state properties of <sup>33<\/sup>Mg with effective interaction PK1. The ground state of <sup>33<\/sup>Mg has been found to be prolate deformed, \u03b2<sub>2<\/sub>=0.23, with the odd neutron in 1\/2[330] orbital and the energy \u2212251.85 MeV which is close to the data \u2212252.06 MeV. The magnetic moment \u22120.9134 \u00b5<sub>N<\/sub> is obtained with the effective electromagnetic current which well reproduces the data \u22120.7456 \u00b5<sub>N<\/sub> self-consistently without introducing any parameter. The energy splittings of time reversal conjugate states, the neutron current, the energy contribution from the nuclear magnetic potential, and the effect of core polarization are discussed in detail.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Magnetic moments of 33Mg in the time-odd relativistic mean field approach Jian Li et al. doi: 10.1007\/s11433-009-0194-y The configuration-fixed deformation constrained relativistic mean field approach with time-odd component has been applied to investigate the ground state properties of 33Mg with&#46;&#46;&#46;<\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"jetpack_post_was_ever_published":false,"jetpack_publicize_message":"","jetpack_is_tweetstorm":false,"jetpack_publicize_feature_enabled":true,"jetpack_social_post_already_shared":false,"jetpack_social_options":{"image_generator_settings":{"template":"highway","enabled":false}}},"categories":[4],"tags":[87,8,86,5,85],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-V","jetpack-related-posts":[{"id":214,"url":"https:\/\/magneticmoments.info\/wp\/?p=214","url_meta":{"origin":57,"position":0},"title":"[paper] Hyperfine fields in the BaFe2As2 family and their relation to the magnetic moment","date":"Dec 13, 2016","format":false,"excerpt":"Hyperfine fields in the BaFe2As2 family and their relation to the magnetic moment G. 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