{"id":22,"date":"2009-03-26T23:09:03","date_gmt":"2009-03-26T21:09:03","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=22"},"modified":"2011-01-01T23:14:00","modified_gmt":"2011-01-01T21:14:00","slug":"paper-g-factors-of-first-2-states-of-neutron-rich-xe-ba-and-ce-isotopes","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=22","title":{"rendered":"[paper] g factors of first 2<sup>+<\/sup> states of neutron-rich Xe, Ba, and Ce isotopes"},"content":{"rendered":"<p><em>g factors of first 2<sup>+<\/sup> states of neutron-rich Xe, Ba, and Ce isotopes<\/em><\/p>\n<p>C. Goodin <em>et al.<\/em><\/p>\n<p><a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevC.79.034316\">10.1103\/PhysRevC.79.034316<\/a><\/p>\n<p>Using new techniques developed for measuring angular correlations with large detector arrays, the <em>g<\/em> factors of 2<sup>+<\/sup> states in <sup>140,142<\/sup>Xe  are measured for the first time by the method of correlation attenuation in randomly oriented magnetic fields. <em>g<\/em> factors in <sup>146<\/sup>Ba  and <sup>146,148<\/sup>Ce are measured to establish the method by comparison with previous values. The results are discussed in terms of IBM-2 and rotation-vibration models.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>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&#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":[37,38,40,41,42,44,39,43,5,6],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-m","jetpack-related-posts":[{"id":164,"url":"https:\/\/magneticmoments.info\/wp\/?p=164","url_meta":{"origin":22,"position":0},"title":"[Paper] Investigation into the semimagic nature of the tin isotopes through electromagnetic moments","date":"Oct 19, 2015","format":false,"excerpt":"Investigation into the semimagic nature of the tin isotopes through electromagnetic moments J.M. Allmond et al. DOI: 10.1103\/PhysRevC.92.041303 A complete set of electromagnetic moments, B(E2;0+1\u21922+1),Q(2+1), and g(2+1), have been measured from Coulomb excitation of semi magic 112,114,116,118,120,122,124Sn (Z=50) on natural carbon and titanium targets. 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":76,"url":"https:\/\/magneticmoments.info\/wp\/?p=76","url_meta":{"origin":22,"position":1},"title":"[paper] Magnetic moments of the first excited 2+ states in the semi-magic 112,114,116,122,124Sn isotopes","date":"Jul 19, 2011","format":false,"excerpt":"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 transient field technique in combination with Coulomb excitation in inverse\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":22,"position":2},"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":[]},{"id":147,"url":"https:\/\/magneticmoments.info\/wp\/?p=147","url_meta":{"origin":22,"position":3},"title":"[paper] Nuclear moments and charge radii of neutron-deficient francium isotopes and isomers","date":"Apr 12, 2015","format":false,"excerpt":"Nuclear moments and charge radii of neutron-deficient francium isotopes and isomers A. Voss et al. doi: http:\/\/dx.doi.org\/10.1103\/PhysRevC.91.044307 Collinear laser fluorescence spectroscopy has been performed on the ground and isomeric states of 204,206Fr in order to determine their spins, nuclear moments, and changes in mean-squared charge radii. A new experimental technique\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":128,"url":"https:\/\/magneticmoments.info\/wp\/?p=128","url_meta":{"origin":22,"position":4},"title":"[paper] Hyperfine structure anomaly and magnetic moments of neutron deficient Tl isomers with I=9\/2","date":"Jul 18, 2012","format":false,"excerpt":"Hyperfine structure anomaly and magnetic moments of neutron deficient Tl isomers with I=9\/2 A.E. Barzakh et al. doi: 10.1103\/PhysRevC.86.014311 The hyperfine structure of 276.9-nm atomic transition has been studied by the resonant ionization spectroscopy method at mass-separator IRIS (Investigation of Radioactive Isotopes on Synchrocyclotron), Petersburg Nuclear Physics Institute (PNPI) for\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":110,"url":"https:\/\/magneticmoments.info\/wp\/?p=110","url_meta":{"origin":22,"position":5},"title":"[paper] First g(2+) measurement on neutron-rich 72Zn, and the high-velocity transient field technique for radioactive heavy-ion beams","date":"Mar 29, 2012","format":false,"excerpt":"First g(2+) measurement on neutron-rich 72Zn, and the high-velocity transient field technique for radioactive heavy-ion beams E. Fiori et al. doi: 10.1103\/PhysRevC.85.034334 The high-velocity transient-field (HVTF) technique was used to measure the g factor of the 2+ state of 72Zn produced as a radioactive beam. The transient-field strength was probed\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/22"}],"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=22"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/22\/revisions"}],"predecessor-version":[{"id":23,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/22\/revisions\/23"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=22"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=22"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=22"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}