{"id":424,"date":"2024-02-17T20:44:00","date_gmt":"2024-02-17T18:44:00","guid":{"rendered":"https:\/\/magneticmoments.info\/wp\/?p=424"},"modified":"2024-02-17T20:51:48","modified_gmt":"2024-02-17T18:51:48","slug":"g-factor-of-chiral-doublets-with-%cf%801h_11-21%e2%8a%97%ce%bd1h_11-2%e2%88%921-configuration","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=424","title":{"rendered":"g factor of chiral doublets with $\u03c0{(1{h}_{11\/2})}^{1}\u2297\u03bd{(1{h}_{11\/2})}^{\u22121}$ configuration"},"content":{"rendered":"<p>Q.B. Chen<\/p>\n<p>DOI: <a href=\"https:\/\/doi.org\/10.1103\/PhysRevC.109.024308\">10.1103\/PhysRevC.109.024308<\/a><\/p>\n<p><strong>Abstract<\/strong><\/p>\n<p>The g factor of chiral doublet bands has been extensively studied within the framework of the particle rotor model. Specifically, these investigations have focused on systems characterized by the particle-hole configuration \u03c0(1h<sub>11\/2<\/sub>)<sup>1<\/sup>\u2297\u03bd(1h<sub>11\/2<\/sub>)<sup>\u22121<\/sup>. Comprehensive examinations have been carried out to assess the influence of deformation parameters \u03b2 and \u03b3, the moment of inertia j<sub>0<\/sub>, the total spin I, and the angular momentum of the collective rotor j<sub>R<\/sub> on the g factor. The findings reveal that the g factor exhibits insensitivity to variations in J<sub>0<\/sub> and \u03b2 values, while its behavior is highly sensitive to changes in the \u03b3 parameter. Moreover, it has been observed that the g factors and the g(j<sub>R<\/sub>) plots associated with the doublet bands demonstrate remarkable similarity in the static chirality region. However, noticeable differences arise in regions characterized by chiral vibration or lacking chirality.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Q.B. Chen DOI: 10.1103\/PhysRevC.109.024308 Abstract The g factor of chiral doublet bands has been extensively studied within the framework of the particle rotor model. Specifically, these investigations have focused on systems characterized by the particle-hole configuration \u03c0(1h11\/2)1\u2297\u03bd(1h11\/2)\u22121. Comprehensive examinations have&#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":true,"jetpack_social_options":{"image_generator_settings":{"template":"highway","enabled":false}}},"categories":[1,4],"tags":[317,318],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-6Q","jetpack-related-posts":[{"id":264,"url":"https:\/\/magneticmoments.info\/wp\/?p=264","url_meta":{"origin":424,"position":0},"title":"[paper] Perturbed angular distributions with LaBr3  detectors: The $g$ factor of the first 10$^+$  state in $^{110}$Cd reexamined","date":"Nov 29, 2017","format":false,"excerpt":"Perturbed angular distributions with LaBr3 \u00a0detectors: The g factor of the first 10+ \u00a0state in 110Cd reexamined T.J. 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