{"id":172,"date":"2015-11-12T10:34:22","date_gmt":"2015-11-12T08:34:22","guid":{"rendered":"http:\/\/magneticmoments.info\/wp\/?p=172"},"modified":"2015-11-12T10:34:23","modified_gmt":"2015-11-12T08:34:23","slug":"preprint-effective-field-theory-for-nuclear-vibrations-with-quantified-uncertainties","status":"publish","type":"post","link":"https:\/\/magneticmoments.info\/wp\/?p=172","title":{"rendered":"[preprint] Effective field theory for nuclear vibrations with quantified uncertainties"},"content":{"rendered":"<p><em>Effective field theory for nuclear vibrations with quantified uncertainties<\/em><\/p>\n<p>E.A. Coello P\u00e9rez and T. Papenbrock<\/p>\n<p>arXiv: <a href=\"http:\/\/arxiv.org\/abs\/1510.02401\">1510.02401<\/a><\/p>\n<p>We develop an effective field theory (EFT) for nuclear vibrations. The key ingredients &#8211; quadrupole degrees of freedom, rotational invariance, and a breakdown scale around the three-phonon level &#8211; are taken from data. The EFT is developed for spectra and electromagnetic moments and transitions. We employ tools from Bayesian statistics for the quantification of theoretical uncertainties. The EFT consistently describes spectra and electromagnetic transitions for 62Ni, 98,100Ru, 106,108Pd, 110,112,114Cd, and 118,120,122Te within the theoretical uncertainties. This suggests that these nuclei can be viewed as anharmonic vibrators.<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Effective field theory for nuclear vibrations with quantified uncertainties E.A. Coello P\u00e9rez and T. Papenbrock arXiv: 1510.02401 We develop an effective field theory (EFT) for nuclear vibrations. The key ingredients &#8211; quadrupole degrees of freedom, rotational invariance, and a breakdown&#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":false,"jetpack_social_options":{"image_generator_settings":{"template":"highway","enabled":false}}},"categories":[4],"tags":[227,228,229,230,231,232,233,234,235,225,226,236,34],"jetpack_publicize_connections":[],"jetpack_featured_media_url":"","jetpack_sharing_enabled":true,"jetpack_shortlink":"https:\/\/wp.me\/p6YIb0-2M","jetpack-related-posts":[{"id":206,"url":"https:\/\/magneticmoments.info\/wp\/?p=206","url_meta":{"origin":172,"position":0},"title":"[Paper] Sensitivities and correlations of nuclear structure observables emerging from chiral interactions","date":"Jul 31, 2016","format":false,"excerpt":"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 model for ab initio calculations of excitation energies as well\u2026","rel":"","context":"In &quot;theory&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":138,"url":"https:\/\/magneticmoments.info\/wp\/?p=138","url_meta":{"origin":172,"position":1},"title":"[paper] Deuteron magnetic quadrupole moment from chiral effective field theory","date":"Jul 18, 2012","format":false,"excerpt":"Deuteron magnetic quadrupole moment from chiral effective field theory C.-P. Liu et al. doi: 10.1016\/j.physletb.2012.06.024 We calculate the magnetic quadrupole moment (MQM) of the deuteron at leading order in the systematic expansion provided by chiral effective field theory. 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":77,"url":"https:\/\/magneticmoments.info\/wp\/?p=77","url_meta":{"origin":172,"position":2},"title":"The importance of magnetic moments to nuclear structure &#8211; a comment by N.D. Cook","date":"Jan 24, 2012","format":false,"excerpt":"I have received the following as a comment to the website. I strongly believe this is an important advocate of our website and motivation behind organizing it, as well as a good read for all people in the field of nuclear physics. Here it is: Dear Theo, I have previously\u2026","rel":"","context":"In &quot;g factor&quot;","img":{"alt_text":"","src":"","width":0,"height":0},"classes":[]},{"id":57,"url":"https:\/\/magneticmoments.info\/wp\/?p=57","url_meta":{"origin":172,"position":3},"title":"[paper] Magnetic moments of 33Mg in the time-odd relativistic mean field approach","date":"Oct 10, 2009","format":false,"excerpt":"Magnetic moments of 33Mg in the time-odd relativistic mean field approach Jian Li et al. doi: 10.1007\/s11433-009-0194-y The configuration-fixed deformation constrained relativistic mean field approach with time-odd component has been applied to investigate the ground state properties of 33Mg with effective interaction PK1. The ground state of 33Mg has been\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":172,"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":164,"url":"https:\/\/magneticmoments.info\/wp\/?p=164","url_meta":{"origin":172,"position":5},"title":"[Paper] Investigation into the semimagic nature of the tin isotopes through electromagnetic moments","date":"Oct 19, 2015","format":false,"excerpt":"Investigation into the semimagic nature of the tin isotopes through electromagnetic moments J.M. Allmond et al. DOI: 10.1103\/PhysRevC.92.041303 A complete set of electromagnetic moments, B(E2;0+1\u21922+1),Q(2+1), and g(2+1), have been measured from Coulomb excitation of semi magic 112,114,116,118,120,122,124Sn (Z=50) on natural carbon and titanium targets. The magnitude of the B(E2) values,\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\/172"}],"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=172"}],"version-history":[{"count":1,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/172\/revisions"}],"predecessor-version":[{"id":173,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=\/wp\/v2\/posts\/172\/revisions\/173"}],"wp:attachment":[{"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=172"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=172"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/magneticmoments.info\/wp\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=172"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}