{"id":24,"date":"2009-05-18T23:15:20","date_gmt":"2009-05-18T20:15:20","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=24"},"modified":"2011-01-01T23:21:23","modified_gmt":"2011-01-01T21:21:23","slug":"paper-nuclear-structure-of-the-even-even-argon-isotopes-with-a-focus-on-magnetic-moments","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=24","title":{"rendered":"[paper] Nuclear structure of the even-even argon isotopes with a focus on magnetic moments"},"content":{"rendered":"

Nuclear structure of the even-even argon isotopes with a focus on magnetic moments<\/em><\/p>\n

S.J.Q. Robinson et al.<\/em><\/p>\n

10.1103\/PhysRevC.79.054322″<\/a><\/p>\n

We study the role of configuration mixing in the heavier even-even isotopes of argon. We begin by limiting the configurations of the even-even Ar isotopes to (d3\/2<\/sub>2<\/sup>)&pi<\/sub>\u2002(f7\/2<\/sub>n<\/sup>)ν<\/sub>. There, due to the particular location in this shell-model space of 40<\/sup>Ar and 44<\/sup>Ar, we find that the spectra, B(E2)’s, and magnetic moments of these two nuclei are identical. Any deviation from this equality is direct evidence of configuration mixing. In a larger shell-model space there are significant differences between these two nuclei, with 44<\/sup>Ar being more collective. We also consider other even-even isotopes of argon and study how their nuclear structure effects evolve with N. We compare in the full 0\u210f\u2002ω space (sd<\/em>)π<\/sub>\u2002(fp<\/em>)ν<\/sub> the results of calculations with the WBT interaction and with the newer SDPF, denoted SDPF-U, interaction.<\/p>\n","protected":false},"excerpt":{"rendered":"

Nuclear structure of the even-even argon isotopes with a focus on magnetic moments S.J.Q. Robinson et al. 10.1103\/PhysRevC.79.054322″ We study the role of configuration mixing in the heavier even-even isotopes of argon. We begin by limiting the configurations of the...<\/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":[4],"tags":[45,46,47,8,5,6,31],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-o","jetpack-related-posts":[{"id":115,"url":"https:\/\/magneticmoments.info\/wp\/?p=115","url_meta":{"origin":24,"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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