{"id":186,"date":"2016-04-12T09:51:17","date_gmt":"2016-04-12T06:51:17","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=186"},"modified":"2016-04-12T09:51:17","modified_gmt":"2016-04-12T06:51:17","slug":"paper-table-of-nuclear-electric-quadrupole-moments","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=186","title":{"rendered":"[Paper] Table of nuclear electric quadrupole moments"},"content":{"rendered":"<p><em>Table of nuclear electric quadrupole moments<\/em><\/p>\n<p>N.J. Stone<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1016\/j.adt.2015.12.002\">10.1016\/j.adt.2015.12.002<\/a><\/p>\n<p>This Table is a compilation of experimental measurements of static electric quadrupole moments of ground states and excited states of atomic nuclei throughout the periodic table. To aid identification of the states, their excitation energy, half-life, spin and parity are given, along with a brief indication of the method and any reference standard used in the particular measurement. Experimental data from all quadrupole moment measurements actually provide a value of the product of the moment and the electric field gradient [EFG] acting at the nucleus. Knowledge of the EFG is thus necessary to extract the quadrupole moment. A single recommended moment value is given for each state, based, for each element, wherever possible, upon a standard reference moment for a nuclear state of that element studied in a situation in which the electric field gradient has been well calculated. For several elements one or more subsidiary EFG\/moment reference is required and their use is specified.<\/p>\n<p>The literature search covers the period to mid-2015.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Table of nuclear electric quadrupole moments N.J. Stone doi: 10.1016\/j.adt.2015.12.002 This Table is a compilation of experimental measurements of static electric quadrupole moments of ground states and excited states of atomic nuclei throughout the periodic table. To aid identification of&#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":[3,205],"tags":[247,196],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-30","jetpack-related-posts":[{"id":139,"url":"https:\/\/magneticmoments.info\/wp\/?p=139","url_meta":{"origin":186,"position":0},"title":"[paper] Quadrupole moments of neutron-deficient 20,21Na","date":"Feb 16, 2009","format":false,"excerpt":"Quadrupole moments of neutron-deficient 20,21Na K. Minamisono et al. doi: 10.1016\/j.physletb.2009.01.006 The electric-quadrupole coupling constant of the ground states of the proton drip line nucleus 20Na (I\u03c0=2+, T1\/2=447.9 ms) and the neutron-deficient nucleus 21Na (I\u03c0=3\/2+, T1\/2=22.49 s) in a hexagonal ZnO single crystal were precisely measured to be |eqQ\/h|=690\u00b112 kHz\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":64,"url":"https:\/\/magneticmoments.info\/wp\/?p=64","url_meta":{"origin":186,"position":1},"title":"[paper] Wigner Crystals of 229Th for Optical Excitation of the Nuclear Isomer","date":"Jun 30, 2011","format":false,"excerpt":"Wigner Crystals of 229Th for Optical Excitation of the Nuclear Isomer C.J. Campbell et al. doi: 10.1103\/PhysRevLett.106.223001 We have produced laser-cooled Wigner crystals of 229Th3+ in a linear Paul trap. 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We take into account parity (P) and time-reversal (T) violation which, at\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":47,"url":"https:\/\/magneticmoments.info\/wp\/?p=47","url_meta":{"origin":186,"position":3},"title":"[paper] Nuclear charge radii and electromagnetic moments of radioactive scandium isotopes and isomers","date":"Jan 5, 2011","format":false,"excerpt":"Nuclear charge radii and electromagnetic moments of radioactive scandium isotopes and isomers M. 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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":182,"url":"https:\/\/magneticmoments.info\/wp\/?p=182","url_meta":{"origin":186,"position":5},"title":"[Paper] Spectroscopic Quadrupole Moments in 96,98Sr: Evidence for Shape Coexistence in Neutron-Rich Strontium Isotopes at N=60","date":"Jan 20, 2016","format":false,"excerpt":"Spectroscopic Quadrupole Moments in Sr96,98: Evidence for Shape Coexistence in Neutron-Rich Strontium Isotopes at N=60 E. Cl\u00e9ment et al. doi: 10.1103\/PhysRevLett.116.022701 Neutron-rich 96,98Sr isotopes have been investigated by safe Coulomb excitation of radioactive beams at the REX-ISOLDE facility. Reduced transition probabilities and spectroscopic quadrupole moments have been extracted from the\u2026","rel":"","context":"In &quot;experiment&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]}],"_links":{"self":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/186"}],"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=186"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/186\/revisions"}],"predecessor-version":[{"id":187,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/186\/revisions\/187"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=186"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=186"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=186"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}