{"id":228,"date":"2017-01-26T10:34:27","date_gmt":"2017-01-26T08:34:27","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=228"},"modified":"2017-01-26T10:34:27","modified_gmt":"2017-01-26T08:34:27","slug":"paper-relativistic-description-of-second-order-correction-to-nuclear-magnetic-moments-with-point-coupling-residual-interaction","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=228","title":{"rendered":"[paper] Relativistic description of second-order correction to nuclear magnetic moments with point-coupling residual interaction"},"content":{"rendered":"<p><em>Relativistic description of second-order correction to nuclear magnetic moments with point-coupling residual interaction<\/em><\/p>\n<p>Jian Li et al.<\/p>\n<p>doi: <a href=\"https:\/\/doi.org\/10.1007\/s11433-010-4215-7\">10.1007\/s11433-010-4215-7<\/a><\/p>\n<p>Using the single particle states and the residual interaction derived from the relativistic point-coupling model with the PC-F1 parameter set, the second-order core polarization corrections to nuclear magnetic moments of LS closed shell nuclei \u00b11 nucleon with A = 15, 17, 39 and 41 are studied and compared with previous non-relativistic results. It is found that the second-order corrections are significant. With these corrections, the isovector magnetic moments of the concerned nuclei are well reproduced, especially those for A = 17 and A = 41.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Relativistic description of second-order correction to nuclear magnetic moments with point-coupling residual interaction Jian Li et al. doi: 10.1007\/s11433-010-4215-7 Using the single particle states and the residual interaction derived from the relativistic point-coupling model with the PC-F1 parameter set, the&#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":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","enabled":false}}},"categories":[1,4],"tags":[274,85],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-3G","jetpack-related-posts":[{"id":57,"url":"https:\/\/magneticmoments.info\/wp\/?p=57","url_meta":{"origin":228,"position":0},"title":"[paper] Magnetic moments of 33Mg in the time-odd relativistic mean field approach","date":"Oct 10, 2009","format":false,"excerpt":"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 effective interaction PK1. The ground state of 33Mg has been\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":239,"url":"https:\/\/magneticmoments.info\/wp\/?p=239","url_meta":{"origin":228,"position":1},"title":"[paper] The first self-consistent calculation of quadrupole moments of odd semi-magic nuclei accounting for phonon-induced corrections","date":"Apr 24, 2017","format":false,"excerpt":"The first self-consistent calculation of quadrupole moments of odd semi-magic nuclei accounting for phonon-induced corrections E.E. Saperstein et al. doi: 10.1088\/1361-6471\/aa65f5 The self-consistent model, developed previously to describe phonon coupling (PC) effects in magnetic moments of odd magic and semi-magic nuclei, is extended to quadrupole moments. It is based on\u2026","rel":"","context":"In &quot;quadrupole&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":55,"url":"https:\/\/magneticmoments.info\/wp\/?p=55","url_meta":{"origin":228,"position":2},"title":"[paper] g factors of nuclear low-lying states: A covariant description","date":"Dec 6, 2010","format":false,"excerpt":"g factors of nuclear low-lying states: A covariant description JiangMing Yao et al. doi: 10.1007\/s11433-010-4214-8 The g factors and spectroscopic quadrupole moments of low-lying excited states 21+, \u2026, 81+ in 24Mg are studied in a covariant density functional theory. The wave functions are constructed by configuration mixing of axially deformed\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":225,"url":"https:\/\/magneticmoments.info\/wp\/?p=225","url_meta":{"origin":228,"position":3},"title":"[paper] g factors of nuclear low-lying states: A covariant description","date":"Jan 26, 2017","format":false,"excerpt":"g factors of nuclear low-lying states: A covariant description JangMing Yao et al. doi: 10.1007\/s11433-010-4214-8 The g factors and spectroscopic quadrupole moments of low-lying excited states 2+1 , ... , 8+1 in 24Mg are studied in a covariant density functional theory. 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We used a computational scheme that treats relativistic and high-order electronic correlation effects within the coupled cluster with single, double, triple, and perturbative quadruple excitations\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":214,"url":"https:\/\/magneticmoments.info\/wp\/?p=214","url_meta":{"origin":228,"position":5},"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. Derondeau et al. doi: 10.1103\/PhysRevB.94.214508 The hyperfine field Bhf and the magnetic properties of the BaFe2As2 family are studied using the fully relativistic Dirac formalism for different types of substitution. The study covers electron doped Ba(Fe1\u2212xCox)2As2\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/228"}],"collection":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=228"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/228\/revisions"}],"predecessor-version":[{"id":229,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/228\/revisions\/229"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=228"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=228"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=228"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}