{"id":145,"date":"2005-06-02T13:46:00","date_gmt":"2005-06-02T10:46:00","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=145"},"modified":"2013-06-04T13:47:20","modified_gmt":"2013-06-04T10:47:20","slug":"paper-magnetic-moments-of-3013al17-and-3213al19","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=145","title":{"rendered":"[paper] Magnetic moments of <sup>30<\/sup><sub>13<\/sub>Al<sub>17<\/sub> and <sup>32<\/sup><sub>13<\/sub>Al<sub>19<\/sub>"},"content":{"rendered":"<p><em>Magnetic moments of <sup>30<\/sup><sub>13<\/sub>Al<sub>17<\/sub> and <sup>32<\/sup><sub>13<\/sub>Al<sub>19<\/sub><\/em><\/p>\n<p>H. Ueno et al.<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1016\/j.physletb.2005.04.037\">10.1016\/j.physletb.2005.04.037<\/a><\/p>\n<p>Ground-state magnetic moments of <sup>30<\/sup>Al and <sup>32<\/sup>Al were measured<br \/>\nwith the &beta;-NMR method using radioactive-isotope beams spin-polarized in the projectile-fragmentation<br \/>\nreaction. Polarization of sizes |P|=0.5\u20131% were obtained in spite of the large numbers of nucleons<br \/>\nthat are removed from the projectile <sup>40<\/sup>Ar, providing a promising prospect that<br \/>\nsubstantial polarizations are obtained even in fragment nuclei that are far removed from the projectile nucleus.<br \/>\nThe obtained &mu; moments, |&mu;<sub>exp<\/sub>(<sup>30<\/sup>Al)|=3.010(7) &mu;<sub>N<\/sub><br \/>\nand |&mu;<sub>exp<\/sub>(<sup>32<\/sup>Al)|=1.959(9) &mu;<sub>N<\/sub>, are in agreement with<br \/>\nshell model calculations within the sd valence space, although a reduction in the energy-gap between<br \/>\nthe sd and pf states is predicted for <sup>32<\/sup>Al in recent theoretical studies.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Magnetic moments of 3013Al17 and 3213Al19 H. Ueno et al. doi: 10.1016\/j.physletb.2005.04.037 Ground-state magnetic moments of 30Al and 32Al were measured with the &beta;-NMR method using radioactive-isotope beams spin-polarized in the projectile-fragmentation reaction. Polarization of sizes |P|=0.5\u20131% were obtained in&#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":[200,201,30,8],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-2l","jetpack-related-posts":[{"id":18,"url":"https:\/\/magneticmoments.info\/wp\/?p=18","url_meta":{"origin":145,"position":0},"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":143,"url":"https:\/\/magneticmoments.info\/wp\/?p=143","url_meta":{"origin":145,"position":1},"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":119,"url":"https:\/\/magneticmoments.info\/wp\/?p=119","url_meta":{"origin":145,"position":2},"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":28,"url":"https:\/\/magneticmoments.info\/wp\/?p=28","url_meta":{"origin":145,"position":3},"title":"[paper] Doubly-magic nature of 56Ni: Measurement of the ground state nuclear magnetic dipole moment of 55Ni","date":"Jun 5, 2009","format":false,"excerpt":"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\u03c0=3\/2-, T1\/2=204 ms) has been deduced to be |&mul(55Ni)|=(0.976&plusminus;0.026)\u2002\u03bcN using the \u03b2-ray detecting nuclear magnetic resonance technique. Results of\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":145,"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":34,"url":"https:\/\/magneticmoments.info\/wp\/?p=34","url_meta":{"origin":145,"position":5},"title":"[paper] Magnetic dipole moments of 57,58,59Cu","date":"Jan 28, 2010","format":false,"excerpt":"Magnetic dipole moments of 57,58,59Cu T.E. Cocolios et al. doi: 10.1103\/PhysRevC.81.014314 In-gas-cell laser spectroscopy of the isotopes 57,58,59,63,65Cu has been performed at the LISOL facility using the 244.164-nm optical transition from the atomic ground state of copper. A detailed discussion on the hyperfine structure of 63Cu is presented. 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