{"id":76,"date":"2011-07-19T18:54:00","date_gmt":"2011-07-19T16:54:00","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=76"},"modified":"2011-07-19T18:54:00","modified_gmt":"2011-07-19T16:54:00","slug":"paper-magnetic-moments-of-the-first-excited-2-states-in-the-semi-magic-112114116122124sn-isotopes","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=76","title":{"rendered":"[paper] Magnetic moments of the first excited 2<sup>+<\/sup> states in the semi-magic <sup>112,114,116,122,124<\/sup>Sn isotopes"},"content":{"rendered":"<p><em>Magnetic moments of the first excited 2<sup>+<\/sup> states in the semi-magic <sup>112,114,116,122,124<\/sup>Sn isotopes<\/em><\/p>\n<p>J. Walker <em>et al.<\/em><\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevC.84.014319\">10.1103\/PhysRevC.84.014319<\/a><\/p>\n<p>The g factors of the first excited 2<sup>+<\/sup> states in the <sup>112,114,116,122,124<\/sup>Sn isotopes have been measured with high accuracy using the transient field technique in combination with Coulomb excitation in inverse kinematics. The experimental results are discussed in a qualitative way on the basis of empirical single-particle g factors of the relevant proton and neutron orbitals and are compared to a number of different theoretical calculations. The results are found to be best described by shell-model calculations in an extended configuration space. Clear evidence for the contribution of neutron pair excitations from the 1d<sub>3\/2<\/sub> to the 0h<sub>11\/2<\/sub> orbital to the wave function of the 2<sub>1<\/sub><sup>+<\/sup> state in <sup>122,124<\/sup>Sn has been obtained.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Magnetic moments of the first excited 2+ states in the semi-magic 112,114,116,122,124Sn isotopes J. Walker et al. doi: 10.1103\/PhysRevC.84.014319 The g factors of the first excited 2+ states in the 112,114,116,122,124Sn isotopes have been measured with high accuracy using the&#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":[3,1],"tags":[116,117,118,119,120,121,39,5,6,115],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-1e","jetpack-related-posts":[{"id":115,"url":"https:\/\/magneticmoments.info\/wp\/?p=115","url_meta":{"origin":76,"position":0},"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. 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The magnitude of the B(E2) values,\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":10,"url":"https:\/\/magneticmoments.info\/wp\/?p=10","url_meta":{"origin":76,"position":2},"title":"[paper] Nuclear spins, magnetic moments, and quadrupole moments of Cu isotopes from N=28 to N=46: Probes for core polarization effects","date":"Dec 17, 2010","format":false,"excerpt":"Nuclear spins, magnetic moments, and quadrupole moments of Cu isotopes from N=28 to N=46: Probes for core polarization effects P. Vingerhoets et al. doi: 10.1103\/PhysRevC.82.064311 Measurements of the ground-state nuclear spins and magnetic and quadrupole moments of the copper isotopes from 61Cu up to 75Cu are reported. The experiments were\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":22,"url":"https:\/\/magneticmoments.info\/wp\/?p=22","url_meta":{"origin":76,"position":3},"title":"[paper] g factors of first 2+ states of neutron-rich Xe, Ba, and Ce isotopes","date":"Mar 26, 2009","format":false,"excerpt":"g factors of first 2+ states of neutron-rich Xe, Ba, and Ce isotopes C. Goodin et al. 10.1103\/PhysRevC.79.034316 Using new techniques developed for measuring angular correlations with large detector arrays, the g factors of 2+ states in 140,142Xe are measured for the first time by the method of correlation attenuation\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":101,"url":"https:\/\/magneticmoments.info\/wp\/?p=101","url_meta":{"origin":76,"position":4},"title":"[paper] g factor of the 21+ state of 168Hf","date":"Mar 19, 2012","format":false,"excerpt":"g factor of the 21+ state of 168Hf A. Wolf et al. doi: 10.1103\/PhysRevC.85.037304 The g factor of the 21+ state of 168Hf was measured using the perturbed angular correlation technique in a static external magnetic field. The result, g(21+)=0.17(3), is discussed in relation to the systematics of the previously\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":426,"url":"https:\/\/magneticmoments.info\/wp\/?p=426","url_meta":{"origin":76,"position":5},"title":"Reexamination of nuclear magnetic dipole and electric quadrupole moments of polonium isotopes","date":"Feb 17, 2024","format":false,"excerpt":"Leonid V. Skripnikov and Anatoly E. Barzak DOI: 10.1103\/PhysRevC.109.024315 Abstract We reexamined the electronic structure parameters used to interpret the hyperfine structure of neutral polonium. 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