{"id":14,"date":"2008-11-26T22:42:12","date_gmt":"2008-11-26T20:42:12","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=14"},"modified":"2011-01-01T22:54:48","modified_gmt":"2011-01-01T20:54:48","slug":"paper-correct-use-of-the-gordon-decomposition-in-the-calculation-of-nucleon-magnetic-dipole-moments","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=14","title":{"rendered":"[paper] Correct use of the Gordon decomposition in the calculation of nucleon magnetic dipole moments"},"content":{"rendered":"<p><em>Correct use of the Gordon decomposition in the calculation of nucleon magnetic dipole moments<\/em><\/p>\n<p>M. Mekhfi<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevC.78.055205\">10.1103\/PhysRevC.78.055205<\/a><\/p>\n<p>We perform the calculation of the nucleon dipole magnetic moment in full detail using the Gordon decomposition of the free quark current. This calculation has become necessary because of frequent misuse of the Gordon decomposition by some authors in computing the nucleon dipole magnetic moment.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Correct use of the Gordon decomposition in the calculation of nucleon magnetic dipole moments M. Mekhfi doi: 10.1103\/PhysRevC.78.055205 We perform the calculation of the nucleon dipole magnetic moment in full detail using the Gordon decomposition of the free quark current.&#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":[8,25,5,6,204],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-e","jetpack-related-posts":[{"id":20,"url":"https:\/\/magneticmoments.info\/wp\/?p=20","url_meta":{"origin":14,"position":0},"title":"[paper] Charge radii and electromagnetic moments of Li and Be isotopes from the ab initio no-core shell model","date":"Feb 25, 2009","format":false,"excerpt":"Charge radii and electromagnetic moments of Li and Be isotopes from the ab initio no-core shell model C. Forss\u00e9n et al. Recently, charge radii and ground-state electromagnetic moments of Li and Be isotopes were measured precisely. We have performed large-scale ab initio no-core shell model calculations for these isotopes using\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":168,"url":"https:\/\/magneticmoments.info\/wp\/?p=168","url_meta":{"origin":14,"position":1},"title":"[Paper] Magnetic moments in odd-A Cd isotopes and coupling of particles with zero-point vibrations","date":"Oct 28, 2015","format":false,"excerpt":"Magnetic moments in odd-A Cd isotopes and coupling of particles with zero-point vibrations S. Mishev and V. V. Voronov DOI: 10.1103\/PhysRevC.92.044329 Background: The coupling of the last nucleon with configurations in the ground state of the even-even core is known to augment the single quasiparticle fragmentation pattern. In a recent\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":30,"url":"https:\/\/magneticmoments.info\/wp\/?p=30","url_meta":{"origin":14,"position":2},"title":"[paper] Up to N3LO heavy-baryon chiral perturbation theory calculation for the M1 properties of three-nucleon systems","date":"Jun 22, 2009","format":false,"excerpt":"Up to N3LO heavy-baryon chiral perturbation theory calculation for the M1 properties of three-nucleon systems Y.-H. Song et al. 10.1103\/PhysRevC.79.064002 M1 properties, comprising magnetic moments and radiative capture of thermal neutron observables, are studied in two- and three-nucleon systems. We use meson exchange current derived up to N3LO using heavy\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":206,"url":"https:\/\/magneticmoments.info\/wp\/?p=206","url_meta":{"origin":14,"position":3},"title":"[Paper] Sensitivities and correlations of nuclear structure observables emerging from chiral interactions","date":"Jul 31, 2016","format":false,"excerpt":"Sensitivities and correlations of nuclear structure observables emerging from chiral interactions Angelo Calci and Robert Roth doi: 10.1103\/PhysRevC.94.014322 Abstract Starting from a set of different two- and three-nucleon interactions from chiral effective field theory, we use the importance-truncated no-core shell model for ab initio calculations of excitation energies as well\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":16,"url":"https:\/\/magneticmoments.info\/wp\/?p=16","url_meta":{"origin":14,"position":4},"title":"[paper] Quantum Monte Carlo calculations of magnetic moments and M1 transitions in A&le;7 nuclei including meson-exchange currents","date":"Dec 10, 2008","format":false,"excerpt":"Quantum Monte Carlo calculations of magnetic moments and M1 transitions in A\u22647 nuclei including meson-exchange currents L.E. Marcucci et al. doi: 10.1103\/PhysRevC.78.065501 Green's function Monte Carlo calculations of magnetic moments and M1 transitions including two-body meson-exchange current (MEC) contributions are reported for A\u22647 nuclei. The realistic Argonne v18 two-nucleon and\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":196,"url":"https:\/\/magneticmoments.info\/wp\/?p=196","url_meta":{"origin":14,"position":5},"title":"[paper] Magnetic moment of the 13\/2+ isomeric state in 69Cu: Spin alignment in the one-nucleon removal reaction","date":"May 16, 2016","format":false,"excerpt":"Magnetic moment of the 13\/2+ isomeric state in 69Cu: Spin alignment in the one-nucleon removal reaction A. Kusoglu et al. doi: http:\/\/dx.doi.org\/10.1103\/PhysRevC.93.054313 We report on a new measurement of the g factor of the (13\/2+) isomeric state in the neutron-rich nucleus 69Cu. This study demonstrates the possibility of obtaining considerable\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/14"}],"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=14"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/14\/revisions"}],"predecessor-version":[{"id":15,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/14\/revisions\/15"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=14"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=14"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=14"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}