{"id":206,"date":"2016-07-31T13:20:11","date_gmt":"2016-07-31T10:20:11","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=206"},"modified":"2016-07-31T13:20:11","modified_gmt":"2016-07-31T10:20:11","slug":"paper-sensitivities-and-correlations-of-nuclear-structure-observables-emerging-from-chiral-interactions","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=206","title":{"rendered":"[Paper] Sensitivities and correlations of nuclear structure observables emerging from chiral interactions"},"content":{"rendered":"<p><em>Sensitivities and correlations of nuclear structure observables emerging from chiral interactions<\/em><\/p>\n<p>Angelo Calci and Robert Roth<\/p>\n<p>doi: <a href=\"http:\/\/dx.doi.org\/10.1103\/PhysRevC.94.014322\">10.1103\/PhysRevC.94.014322<\/a><\/p>\n<p>Abstract<\/p>\n<p>Starting from a set of different two- and three-nucleon interactions from chiral effective field theory, we use the importance-truncated no-core shell model for ab initio calculations of excitation energies as well as electric quadrupole (E2) and magnetic dipole (M1) moments and transition strengths for selected p-shell nuclei. We explore the sensitivity of the excitation energies to the chiral interactions as a first step towards and systematic uncertainty propagation from chiral inputs to nuclear structure observables. The uncertainty band spanned by the different chiral interactions is typically in agreement with experimental excitation energies, but we also identify observables with notable discrepancies beyond the theoretical uncertainty that reveal insufficiencies in the chiral interactions. For electromagnetic observables we identify correlations among pairs of E2 or M1 observables based on the ab initio calculations for the different interactions. We find extremely robust correlations for E2 observables and illustrate how these correlations can be used to predict one observable based on an experimental datum for the second observable. In this way we circumvent convergence issues and arrive at far more accurate results than any direct ab initio calculation. A prime example for this approach is the quadrupole moment of the first 2+ state in C12, which is predicted with an drastically improved accuracy.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Sensitivities and correlations of nuclear structure observables emerging from chiral interactions Angelo Calci and Robert Roth doi: 10.1103\/PhysRevC.94.014322 Abstract Starting from a set of different two- and three-nucleon interactions from chiral effective field theory, we use the importance-truncated no-core shell&#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":[264,194,196,8],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-3k","jetpack-related-posts":[{"id":30,"url":"https:\/\/magneticmoments.info\/wp\/?p=30","url_meta":{"origin":206,"position":0},"title":"[paper] Up to N3LO heavy-baryon chiral perturbation theory calculation for the M1 properties of three-nucleon systems","date":"Jun 22, 2009","format":false,"excerpt":"Up to N3LO heavy-baryon chiral perturbation theory calculation for the M1 properties of three-nucleon systems Y.-H. 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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":204,"url":"https:\/\/magneticmoments.info\/wp\/?p=204","url_meta":{"origin":206,"position":2},"title":"[Paper] Radii and Binding Energies in Oxygen Isotopes: A Challenge for Nuclear Forces","date":"Jul 29, 2016","format":false,"excerpt":"Radii and Binding Energies in Oxygen Isotopes: A Challenge for Nuclear Forces V. Lapoux et al. doi: 10.1103\/PhysRevLett.117.052501 We present a systematic study of both nuclear radii and binding energies in (even) oxygen isotopes from the valley of stability to the neutron drip line. 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Martinez Torres et al doi: 10.1140\/epja\/i2012-12185-3 The magnetic moments of the low-lying spin-parity JP = 1\/2-, 3\/2- \u039b resonances, like, for example, \u039b(1405)1\/2-, \u039b(1520) 3\/2-, as well as their transition\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":426,"url":"https:\/\/magneticmoments.info\/wp\/?p=426","url_meta":{"origin":206,"position":4},"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":424,"url":"https:\/\/magneticmoments.info\/wp\/?p=424","url_meta":{"origin":206,"position":5},"title":"g factor of chiral doublets with $\u03c0{(1{h}_{11\/2})}^{1}\u2297\u03bd{(1{h}_{11\/2})}^{\u22121}$ configuration","date":"Feb 17, 2024","format":false,"excerpt":"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 been carried out to assess the influence of deformation parameters\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\/206"}],"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=206"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/206\/revisions"}],"predecessor-version":[{"id":207,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/206\/revisions\/207"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=206"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=206"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=206"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}