{"id":153,"date":"2015-10-02T23:22:11","date_gmt":"2015-10-02T20:22:11","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=153"},"modified":"2015-10-02T23:23:32","modified_gmt":"2015-10-02T20:23:32","slug":"paper-orientation-features-of-24mg2-aligned-nuclei-in-pp-and-dd-reactions-at-ex-%e2%89%88-7-5-mev-per-nucleon","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=153","title":{"rendered":"[paper] Orientation features of <sup>24<\/sup>Mg(2<sup>+<\/sup>) aligned nuclei in (p,p) and (d,d) reactions at E<sub>x<\/sub> \u2248 7.5 MeV per nucleon"},"content":{"rendered":"<p><em>Orientation features of <sup>24<\/sup>Mg(2<sup>+<\/sup>) aligned nuclei in (p,p) and (d,d) reactions at E<sub>x<\/sub> \u2248 7.5 MeV per nucleon<\/em><\/p>\n<p>L.I. Galanina et al.<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1134\/S1063778815060095\">10.1134\/S1063778815060095<\/a><\/p>\n<p>Experimental angular dependences of cross sections for elastic and inelastic scattering and the result obtained by reconstructing the populations of magnetic sublevels, multipole-moment orientation tensors, and polarization tensors are presented for <sup>24<\/sup>Mg (2+, 1.369 MeV) aligned nuclei produced in inelastic proton scattering at E<sub>p<\/sub> = 7.4 MeV. The experimental results in question are compared with the results of calculations based on the coupled-channel method and on the compound-nucleus model, the 3\/2+ resonance in the <sup>25<\/sup>Al compound nucleus being taken into account. The orientation features of <sup>24<\/sup>Mg (2+, 1.369 MeV) nuclei produced in inelastic proton and deuteron scattering on <sup>24<\/sup>Mg at E<sub>x<\/sub> \u2248 7.5 MeV per nucleon are found to be generally similar despite a substantial difference in the respective differential cross sections.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Orientation features of 24Mg(2+) aligned nuclei in (p,p) and (d,d) reactions at Ex \u2248 7.5 MeV per nucleon L.I. Galanina et al. doi: 10.1134\/S1063778815060095 Experimental angular dependences of cross sections for elastic and inelastic scattering and the result obtained by&#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":[3],"tags":[139,209,208],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-2t","jetpack-related-posts":[{"id":103,"url":"https:\/\/magneticmoments.info\/wp\/?p=103","url_meta":{"origin":153,"position":0},"title":"[paper] Nuclear Charge Radii of 21-32Mg","date":"Jan 26, 2012","format":false,"excerpt":"Nuclear Charge Radii of 21-32Mg D.T. Yordanov et al. doi: 10.1103\/PhysRevLett.108.042504 Charge radii of all magnesium isotopes in the sd shell have been measured, revealing evolution of the nuclear shape throughout two prominent regions of assumed deformation centered on 24Mg and 32Mg. A striking correspondence is found between the nuclear\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":156,"url":"https:\/\/magneticmoments.info\/wp\/?p=156","url_meta":{"origin":153,"position":1},"title":"[paper] Structural evolution in transitional nuclei of mass 82\u2264A\u2264132","date":"Oct 3, 2015","format":false,"excerpt":"Structural evolution in transitional nuclei of mass 82\u2264A\u2264132 M. Bhutan doi: 10.1103\/PhysRevC.92.034323 In this theoretical study, we report an investigation on the behavior of two-neutron separation energy, a differential variation of the nucleon separation energy, the nuclear charge radii, and the single-particle energy levels along the isotopic chains of transitional\u2026","rel":"","context":"In &quot;radii&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":16,"url":"https:\/\/magneticmoments.info\/wp\/?p=16","url_meta":{"origin":153,"position":2},"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":341,"url":"https:\/\/magneticmoments.info\/wp\/?p=341","url_meta":{"origin":153,"position":3},"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":347,"url":"https:\/\/magneticmoments.info\/wp\/?p=347","url_meta":{"origin":153,"position":4},"title":"[paper] Interplay between nuclear shell evolution and shape deformation revealed by the magnetic moment of 75Cu","date":"Jan 22, 2019","format":false,"excerpt":"Interplay between nuclear shell evolution and shape deformation revealed by the magnetic moment of 75Cu Y. Ishikawa et al. Nature Physics (2019) DOI: 10.1038\/s41567-018-0410-7 Exotic nuclei are characterized by having a number of neutrons (or protons) in excess relative to stable nuclei. Their shell structure, which represents single-particle motion in\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"https:\/\/i0.wp.com\/magneticmoments.info\/wp\/wp-content\/uploads\/2019\/01\/cu75.png?resize=350%2C200","width":350,"height":200},"classes":[]},{"id":30,"url":"https:\/\/magneticmoments.info\/wp\/?p=30","url_meta":{"origin":153,"position":5},"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":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/153"}],"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=153"}],"version-history":[{"count":2,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/153\/revisions"}],"predecessor-version":[{"id":155,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/153\/revisions\/155"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=153"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=153"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=153"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}