{"id":200,"date":"2016-07-20T11:39:09","date_gmt":"2016-07-20T08:39:09","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=200"},"modified":"2016-07-20T11:39:09","modified_gmt":"2016-07-20T08:39:09","slug":"paper-microscopic-description-of-ground-state-magnetic-moment-and-low-lying-magnetic-dipole-excitations-in-heavy-odd-mass-181ta-nucleus","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=200","title":{"rendered":"[paper] Microscopic description of ground state magnetic moment and low-lying magnetic dipole excitations in heavy odd-mass <sup>181<\/sup>Ta nucleus"},"content":{"rendered":"<p><em>Microscopic description of ground state magnetic moment and low-lying magnetic dipole excitations in heavy odd-mass<sup>181<\/sup>Ta nucleus<\/em><\/p>\n<p>E. Tabar et al.<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1142\/S0218301316500531\">http:\/\/dx.doi.org\/10.1142\/S0218301316500531<\/a><\/p>\n<p>The ground state magnetic moments and the low-lying magnetic dipole (Ml) transitions from the ground to excited states in heavy deformed odd-mass <sup>181<\/sup>Ta have been microscopically investigated on the basis of the quasiparticle-phonon nuclear model (QPNM). The problem of the spurious state mixing in M1 excitations is overcome by a restoration method allowing a self-consistent determination of the separable effective restoration forces. Due to the self-consistency of the method, these effective forces contain no arbitrary parameters. The results of calculations are compared with the available experimental data, the agreement being reasonably satisfactory.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Microscopic description of ground state magnetic moment and low-lying magnetic dipole excitations in heavy odd-mass181Ta nucleus E. Tabar et al. doi: http:\/\/dx.doi.org\/10.1142\/S0218301316500531 The ground state magnetic moments and the low-lying magnetic dipole (Ml) transitions from the ground to excited states&#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":[4],"tags":[257,258,8,259],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-3e","jetpack-related-posts":[{"id":426,"url":"https:\/\/magneticmoments.info\/wp\/?p=426","url_meta":{"origin":200,"position":0},"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. We used a computational scheme that treats relativistic and high-order electronic correlation effects within the coupled cluster with single, double, triple, and perturbative quadruple excitations\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":168,"url":"https:\/\/magneticmoments.info\/wp\/?p=168","url_meta":{"origin":200,"position":1},"title":"[Paper] Magnetic moments in odd-A Cd isotopes and coupling of particles with zero-point vibrations","date":"Oct 28, 2015","format":false,"excerpt":"Magnetic moments in odd-A Cd isotopes and coupling of particles with zero-point vibrations S. Mishev and V. V. 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