{"id":28,"date":"2009-06-05T23:21:40","date_gmt":"2009-06-05T20:21:40","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=28"},"modified":"2011-01-01T23:30:10","modified_gmt":"2011-01-01T21:30:10","slug":"paper-doubly-magic-nature-of-56ni-measurement-of-the-ground-state-nuclear-magnetic-dipole-moment-of-55ni","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=28","title":{"rendered":"[paper] Doubly-magic nature of <sup>56<\/sup>Ni: Measurement of the ground state nuclear magnetic dipole moment of <sup>55<\/sup>Ni"},"content":{"rendered":"<p><em>Doubly-magic nature of <sup>56<\/sup>Ni: Measurement of the ground state nuclear magnetic dipole moment of <sup>55<\/sup>Ni<\/em><\/p>\n<p>J.S. Berryman <em>et al.<\/em><\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevC.79.064305\">10.1103\/PhysRevC.79.064305<\/a><\/p>\n<p>The nuclear magnetic moment of the ground state of <sup>55<\/sup>Ni  (I<sup>&pi;<\/sup>=3\/2<sup>&#8211;<\/sup>, T<sub>1\/2<\/sub>=204 ms) has been deduced to be |&#038;mul(<sup>55<\/sup>Ni)|=(0.976&#038;plusminus;0.026)\u2002&mu;<sub>N<\/sub> using the &beta;-ray detecting nuclear magnetic resonance technique. Results of a shell model calculation in the full <em>fp<\/em> shell model space with the GXPF1 interaction reproduce the experimental value. Together with the known magnetic moment of the mirror partner <sup>55<\/sup>Co, the isoscalar spin expectation value was extracted as <&Sigma;&sigma;<sub>z<\/sub>>=0.91&#038;plusminus;0.07. The <&Sigma;&sigma;<sub>z<\/sub>> shows a trend similar to that established in the <em>sd<\/em> shell. The present theoretical interpretations of both &#038;mul(<sup>55<\/sup>Ni) and <&Sigma;&sigma;<sub>z<\/sub>> for the T=1\/2, A=55  mirror partners support the softness of the <sup>56<\/sup>Ni  core.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Doubly-magic nature of 56Ni: Measurement of the ground state nuclear magnetic dipole moment of 55Ni J.S. Berryman et al. doi: 10.1103\/PhysRevC.79.064305 The nuclear magnetic moment of the ground state of 55Ni (I&pi;=3\/2&#8211;, T1\/2=204 ms) has been deduced to be |&#038;mul(55Ni)|=(0.976&#038;plusminus;0.026)\u2002&mu;N&#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":[48,30,5,6,31,49],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-s","jetpack-related-posts":[{"id":143,"url":"https:\/\/magneticmoments.info\/wp\/?p=143","url_meta":{"origin":28,"position":0},"title":"[paper] Nuclear ground-state spin and magnetic moment of 21Mg","date":"Aug 3, 2009","format":false,"excerpt":"Nuclear ground-state spin and magnetic moment of 21Mg J. Kr\u00e4mer et al. doi: 10.1016\/j.physletb.2009.06.063 We present the results of combined laser spectroscopy and nuclear magnetic resonance studies of 21Mg. The nuclear ground-state spin was measured to be I=5\/2 with a magnetic moment of &mul;=\u22120.983(7)\u03bcN. The isoscalar magnetic moment of the\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":28,"position":1},"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":200,"url":"https:\/\/magneticmoments.info\/wp\/?p=200","url_meta":{"origin":28,"position":2},"title":"[paper] Microscopic description of ground state magnetic moment and low-lying magnetic dipole excitations in heavy odd-mass 181Ta nucleus","date":"Jul 20, 2016","format":false,"excerpt":"Microscopic description of ground state magnetic moment and low-lying magnetic dipole excitations in heavy odd-mass181Ta nucleus E. Tabar et al. doi: http:\/\/dx.doi.org\/10.1142\/S0218301316500531 The ground state magnetic moments and the low-lying magnetic dipole (Ml) transitions from the ground to excited states in heavy deformed odd-mass 181Ta have been microscopically investigated on\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":20,"url":"https:\/\/magneticmoments.info\/wp\/?p=20","url_meta":{"origin":28,"position":3},"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":18,"url":"https:\/\/magneticmoments.info\/wp\/?p=18","url_meta":{"origin":28,"position":4},"title":"[paper] Ground-state electric quadrupole moment of 31Al","date":"Feb 18, 2009","format":false,"excerpt":"Ground-state electric quadrupole moment of 31Al D. Nagae et al. The ground-state electric quadrupole moment of 31Al(I\u03c0=5\/2+,T1\/2=644(25) ms) has been measured by means of \u03b2-ray-detected nuclear magnetic resonance spectroscopy using a spin-polarized 31Al beam produced in the projectile fragmentation reaction. The obtained Q moment, |Qexp(31Al)|=112(32) e\u2002mb, is in agreement with\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":36,"url":"https:\/\/magneticmoments.info\/wp\/?p=36","url_meta":{"origin":28,"position":5},"title":"[paper] g factor of the 44Cl ground state: Probing the reduced Z=16 and N=28 gaps","date":"Mar 19, 2010","format":false,"excerpt":"g factor of the 44Cl ground state: Probing the reduced Z=16 and N=28 gaps M. 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