{"id":89,"date":"2011-09-22T19:48:00","date_gmt":"2011-09-22T16:48:00","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=89"},"modified":"2012-04-26T20:11:39","modified_gmt":"2012-04-26T17:11:39","slug":"paper-gyromagnetic-factors-in-144-150nd","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=89","title":{"rendered":"[paper] Gyromagnetic factors in <sup>144-150<\/sup>Nd"},"content":{"rendered":"<p><em>Gyromagnetic factors in <sup>144-150<\/sup>Nd<\/em><\/p>\n<p>A. Giannatiempo<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevC.84.034319\">10.1103\/PhysRevC.84.034319<\/a><\/p>\n<p>The U(5) to SU(3) evolution of the nuclear structure in the even <sup>144-156<\/sup>Nd isotopes has been investigated in the framework of the interacting boson approximation (IBA-2) model, taking into account the effect of the partial Z=64 subshell closure on the structure of the states of a collective nature. The analysis, which led to a satisfactory description of excitation energy patterns, quadrupole moments, and decay properties of the states (even when important M1 components were present in the transitions), is extended to the available data on g factors, in <sup>144-150<\/sup>Nd. Their values are reasonably reproduced by the calculations.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Gyromagnetic factors in 144-150Nd A. Giannatiempo doi: 10.1103\/PhysRevC.84.034319 The U(5) to SU(3) evolution of the nuclear structure in the even 144-156Nd isotopes has been investigated in the framework of the interacting boson approximation (IBA-2) model, taking into account the effect&#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":[1],"tags":[122,123,124,125,39,43,5,6],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-1r","jetpack-related-posts":[{"id":162,"url":"https:\/\/magneticmoments.info\/wp\/?p=162","url_meta":{"origin":89,"position":0},"title":"[paper] Gyromagnetic gs factors of the spin-1\/2 particles in the (\u00bd+-\u00bd&#8211;-3\/2&#8211;) triad of the four-vector spinor, \u03c8\u03bc, irreducibility and linearity","date":"Oct 13, 2015","format":false,"excerpt":"Gyromagnetic gs factors of the spin-1\/2 particles in the (\u00bd+-\u00bd--3\/2-) triad of the four-vector spinor, \u03c8\u03bc, irreducibility and linearity E.G. Delgado Acosta et al. DOI: 10.1142\/S0218301315500603 The gauged Klein\u2013Gordon equation, extended by a gs\u03c3\u03bc\u03bdF\u03bc\u03bd\/4 interaction, the contraction of the electromagnetic field strength tensor, F\u03bc\u03bd, with the generators, \u03c3\u03bc\u03bd\/2, of the\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":341,"url":"https:\/\/magneticmoments.info\/wp\/?p=341","url_meta":{"origin":89,"position":1},"title":"[paper] Isoscalar Spin Matrix Elements in s\u2013d Shell Nuclei","date":"Jan 2, 2019","format":false,"excerpt":"Isoscalar Spin Matrix Elements in s\u2013d Shell Nuclei by Akito Arima and Wolfgang Bentz doi: 10.7566\/JPSCP.23.012011 The quenching of isovector spin matrix elements in s\u2013d shell nuclei is well established experimentally as well as theoretically [1,2,3]. The isoscalar spin gyromagnetic ratios gsIS of nuclei with one nucleon or hole outside\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"https:\/\/i0.wp.com\/mertzimekis.gr\/home\/wp-content\/uploads\/2019\/01\/GT-1.png?resize=350%2C200","width":350,"height":200},"classes":[]},{"id":196,"url":"https:\/\/magneticmoments.info\/wp\/?p=196","url_meta":{"origin":89,"position":2},"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":[]},{"id":119,"url":"https:\/\/magneticmoments.info\/wp\/?p=119","url_meta":{"origin":89,"position":3},"title":"[paper] Observation of 239Pu Nuclear Magnetic Resonance","date":"May 28, 2012","format":false,"excerpt":"Observation of 239Pu Nuclear Magnetic Resonance H. Yasuoka et al. doi: 10.1126\/science.1220801 In principle, the spin-\u00bd plutonium-239 (239Pu) nucleus should be active in nuclear magnetic resonance spectroscopy. However, its signal has eluded detection for the past 50 years. Here, we report observation of a 239Pu resonance from a solid sample\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":144,"url":"https:\/\/magneticmoments.info\/wp\/?p=144","url_meta":{"origin":89,"position":4},"title":"[paper] g factor of the exotic N=21 isotope 34Al: probing the N=20 and N=28 shell gaps at the border of the &quot;island of inversion&quot;","date":"Jan 10, 2008","format":false,"excerpt":"g factor of the exotic N=21 isotope 34Al: probing the N=20 and N=28 shell gaps at the border of the \"island of inversion\" P. Himpe et al. doi: 10.1016\/j.physletb.2007.11.017 For the first time the g factor of an isotope beyond N=20 near the \"island of inversion\" has been measured. A\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":115,"url":"https:\/\/magneticmoments.info\/wp\/?p=115","url_meta":{"origin":89,"position":5},"title":"[paper] Structure of the Sr-Zr isotopes near and at the magic N=50 shell from g-factor and lifetime measurements in8840Zr and 84,86,8838Sr","date":"Apr 30, 2012","format":false,"excerpt":"Structure of the Sr-Zr isotopes near and at the magic N=50 shell from g-factor and lifetime measurements in8840Zr and 84,86,8838Sr G. Kumbartzki et al. doi: 10.1103\/PhysRevC.85.044322 Background: The evolution of and interplay between single-particle and collective excitations in the 40 \u2a7dN\u2a7d 50 range for 38Sr and 40Zr isotopes have been\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\/89"}],"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=89"}],"version-history":[{"count":2,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/89\/revisions"}],"predecessor-version":[{"id":94,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/89\/revisions\/94"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=89"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=89"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=89"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}