{"id":30,"date":"2009-06-22T23:36:52","date_gmt":"2009-06-22T20:36:52","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=30"},"modified":"2011-01-01T23:40:56","modified_gmt":"2011-01-01T21:40:56","slug":"paper-up-to-n3lo-heavy-baryon-chiral-perturbation-theory-calculation-for-the-m1-properties-of-three-nucleon-systems","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=30","title":{"rendered":"[paper] Up to N3<\/sup>LO heavy-baryon chiral perturbation theory calculation for the M1 properties of three-nucleon systems"},"content":{"rendered":"

Up to N3<\/sup>LO heavy-baryon chiral perturbation theory calculation for the M1 properties of three-nucleon systems<\/em><\/p>\n

Y.-H. Song et al.<\/em><\/p>\n

10.1103\/PhysRevC.79.064002<\/a><\/p>\n

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 N3<\/sup>LO using heavy baryon chiral perturbation theory à la Weinberg. Calculations have been performed for several qualitatively different realistic nuclear Hamiltonians, which permits us to analyze model dependence of our results. Our results are found to be strongly correlated with the effective range parameters such as binding energies and the scattering lengths. Taking into account such correlations, the results are in good agreement with the experimental data with small model dependence.<\/p>\n","protected":false},"excerpt":{"rendered":"

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...<\/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":[8,27,50,5,6],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-u","jetpack-related-posts":[{"id":206,"url":"https:\/\/magneticmoments.info\/wp\/?p=206","url_meta":{"origin":30,"position":0},"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 "theory"","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":14,"url":"https:\/\/magneticmoments.info\/wp\/?p=14","url_meta":{"origin":30,"position":1},"title":"[paper] Correct use of the Gordon decomposition in the calculation of nucleon magnetic dipole moments","date":"Nov 26, 2008","format":false,"excerpt":"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. This calculation has become necessary because of frequent misuse of\u2026","rel":"","context":"In "theory"","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":16,"url":"https:\/\/magneticmoments.info\/wp\/?p=16","url_meta":{"origin":30,"position":2},"title":"[paper] Quantum Monte Carlo calculations of magnetic moments and M1 transitions in A≤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 "g factor"","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":204,"url":"https:\/\/magneticmoments.info\/wp\/?p=204","url_meta":{"origin":30,"position":3},"title":"[Paper] Radii and Binding Energies in Oxygen Isotopes: A Challenge for Nuclear Forces","date":"Jul 29, 2016","format":false,"excerpt":"Radii and Binding Energies in Oxygen Isotopes: A Challenge for Nuclear Forces V. Lapoux et al. doi: 10.1103\/PhysRevLett.117.052501 We present a systematic study of both nuclear radii and binding energies in (even) oxygen isotopes from the valley of stability to the neutron drip line. Both charge and matter radii are\u2026","rel":"","context":"In "radii"","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":138,"url":"https:\/\/magneticmoments.info\/wp\/?p=138","url_meta":{"origin":30,"position":4},"title":"[paper] Deuteron magnetic quadrupole moment from chiral effective field theory","date":"Jul 18, 2012","format":false,"excerpt":"Deuteron magnetic quadrupole moment from chiral effective field theory C.-P. Liu et al. doi: 10.1016\/j.physletb.2012.06.024 We calculate the magnetic quadrupole moment (MQM) of the deuteron at leading order in the systematic expansion provided by chiral effective field theory. We take into account parity (P) and time-reversal (T) violation which, at\u2026","rel":"","context":"In "theory"","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":132,"url":"https:\/\/magneticmoments.info\/wp\/?p=132","url_meta":{"origin":30,"position":5},"title":"[paper] Magnetic moments of the low-lying JP = 1\/2–, 3\/2– Λ resonances within the framework of the chiral quark model","date":"Jan 6, 2013","format":false,"excerpt":"Magnetic moments of the low-lying JP = 1\/2-, 3\/2- \u039b resonances within the framework of the chiral quark model A. Martinez Torres et al doi: 10.1140\/epja\/i2012-12185-3 The magnetic moments of the low-lying spin-parity JP = 1\/2-, 3\/2- \u039b resonances, like, for example, \u039b(1405)1\/2-, \u039b(1520) 3\/2-, as well as their transition\u2026","rel":"","context":"In "theory"","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/30"}],"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=30"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/30\/revisions"}],"predecessor-version":[{"id":31,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/30\/revisions\/31"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=30"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=30"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=30"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}