{"id":191,"date":"2016-05-16T00:32:30","date_gmt":"2016-05-15T21:32:30","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=191"},"modified":"2016-05-16T00:32:30","modified_gmt":"2016-05-15T21:32:30","slug":"paper-infrared-extrapolations-of-quadrupole-moments-and-transitions","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=191","title":{"rendered":"[paper] Infrared extrapolations of quadrupole moments and transitions"},"content":{"rendered":"<p><em>Infrared extrapolations of quadrupole moments and transitions<\/em><\/p>\n<p>D. Odell et al.<\/p>\n<p>doi:\u00a0<a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevC.93.044331\"><span style=\"color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\">10.1103\/PhysRevC.93.044331<\/span><\/a><\/p>\n<p><span style=\"color: #222222; font-family: 'Helvetica Neue', Helvetica, Roboto, Arial, sans-serif;\">We study the convergence of bound-state quadrupole moments in finite harmonic oscillator spaces. We derive an expression for the infrared extrapolation for the quadrupole moment of a nucleus and benchmark our results using different model interactions for the deuteron. We find good agreement between the analytically derived and numerically obtained convergence behavior. We also derive an extrapolation formula for electric quadrupole transitions and find good agreement with the numerical calculation of a simple system.<\/span><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Infrared extrapolations of quadrupole moments and transitions D. Odell et al. doi:\u00a010.1103\/PhysRevC.93.044331 We study the convergence of bound-state quadrupole moments in finite harmonic oscillator spaces. We derive an expression for the infrared extrapolation for the quadrupole moment of a nucleus&#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":[205,4],"tags":[248],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-35","jetpack-related-posts":[{"id":121,"url":"https:\/\/magneticmoments.info\/wp\/?p=121","url_meta":{"origin":191,"position":0},"title":"[paper] Self-consistent calculations of quadrupole moments of the first 2+ states in Sn and Pb isotopes","date":"Jun 3, 2012","format":false,"excerpt":"Self-consistent calculations of quadrupole moments of the first 2+ states in Sn and Pb isotopes D. Voitenkov et al. doi: 10.1103\/PhysRevC.85.054319 A method of describing static moments of excited states and transitions between excited states is formulated for nonmagic nuclei within the Green's function formalism. Quadrupole moments of the first\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":117,"url":"https:\/\/magneticmoments.info\/wp\/?p=117","url_meta":{"origin":191,"position":1},"title":"[paper] Quadrupole moments of spherical semi-magic nuclei within the self-consistent Theory of Finite Fermi Systems","date":"May 27, 2012","format":false,"excerpt":"Quadrupole moments of spherical semi-magic nuclei within the self-consistent Theory of Finite Fermi Systems S.V. 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Minamisono et al. doi: 10.1016\/j.physletb.2009.01.006 The electric-quadrupole coupling constant of the ground states of the proton drip line nucleus 20Na (I\u03c0=2+, T1\/2=447.9 ms) and the neutron-deficient nucleus 21Na (I\u03c0=3\/2+, T1\/2=22.49 s) in a hexagonal ZnO single crystal were precisely measured to be |eqQ\/h|=690\u00b112 kHz\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":20,"url":"https:\/\/magneticmoments.info\/wp\/?p=20","url_meta":{"origin":191,"position":4},"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":239,"url":"https:\/\/magneticmoments.info\/wp\/?p=239","url_meta":{"origin":191,"position":5},"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":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/191"}],"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=191"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/191\/revisions"}],"predecessor-version":[{"id":192,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/191\/revisions\/192"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=191"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=191"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=191"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}