Suppressed electric quadrupole collectivity in <sup>49</sup>Ti

dc.contributor.authorGray, T. J.en
dc.contributor.authorAllmond, J. M.en
dc.contributor.authorBenetti, C.en
dc.contributor.authorWibisono, C.en
dc.contributor.authorBaby, L.en
dc.contributor.authorGargano, A.en
dc.contributor.authorMiyagi, T.en
dc.contributor.authorMacchiavelli, A. O.en
dc.contributor.authorStuchbery, A. E.en
dc.contributor.authorWood, J. L.en
dc.contributor.authorAjayi, S.en
dc.contributor.authorAragon, J.en
dc.contributor.authorAsher, B. W.en
dc.contributor.authorBarber, P.en
dc.contributor.authorBhattacharya, S.en
dc.contributor.authorBoisseau, R.en
dc.contributor.authorChristie, J. M.en
dc.contributor.authorConley, A. L.en
dc.contributor.authorDe Rosa, P.en
dc.contributor.authorDowling, D. T.en
dc.contributor.authorEsparza, C.en
dc.contributor.authorGibbons, J.en
dc.contributor.authorHanselman, K.en
dc.contributor.authorHolt, J. D.en
dc.contributor.authorLopez-Caceres, S.en
dc.contributor.authorLopez Saavedra, E.en
dc.contributor.authorMcCann, G. W.en
dc.contributor.authorMorelock, A.en
dc.contributor.authorKelly, B.en
dc.contributor.authorKing, T. T.en
dc.contributor.authorRasco, B. C.en
dc.contributor.authorSitaraman, V.en
dc.contributor.authorTabor, S. L.en
dc.contributor.authorTemanson, E.en
dc.contributor.authorTripathi, V.en
dc.contributor.authorWiedenhöver, I.en
dc.contributor.authorYadav, R. B.en
dc.date.accessioned2025-05-30T20:30:38Z
dc.date.available2025-05-30T20:30:38Z
dc.date.issued2024en
dc.description.abstractSingle-step Coulomb excitation of Ti-46,Ti-48,Ti-49,Ti-50 is presented. A complete set of E2 matrix elements for the quintuplet of states in Ti-49, centred on the 2+ core excitation, was measured for the first time. A total of nine E2 matrix elements are reported, four of which were previously unknown. Ti-49(22)27 shows a 20% quenching in electric quadrupole transition strength as compared to its semi-magic Ti-50(22)28 neighbour. This 20% quenching, while empirically unprecedented, can be explained with a remarkably simple two-state mixing model, which is also consistent with other ground-state properties such as the magnetic dipole moment and electric quadrupole moment. A connection to nucleon transfer data and the quenching of single-particle strength is also demonstrated. The simplicity of the Ti-49-Ti-50 pair (i.e., approximate single-j 0f7/2 valence space and isolation of yrast states from non-yrast states) provides a unique opportunity to disentangle otherwise competing effects in the ground-state properties of atomic nuclei, the emergence of collectivity, and the role of proton-neutron interactions.en
dc.description.sponsorshipWe would like to acknowledge the Center for Accelerator Target Science (CATS) and Matt Gott for making the C and Al foils used in this study and Alfredo Poves for useful discussions on the shell-model calculations. This material is based upon work supported in part by the U.S. Department of Energy, Office of Science, Office of Nuclear Physics under Contract No. DE-AC05-00OR22725 (ORNL) . This work was also supported by the U.S. National Science Foundation under Grant No. PHY-2012522 (FSU) and the Australian Research Council un-der grant No. DP210101201. In addition, this work was supported in part by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) - Project-ID 279384907 - SFB 1245, and the European Research Council (ERC) under the European Union's Horizon 2020 re-search and innovation programme (Grant Agreement No. 101020842) . The VS-IMSRG calculations were supported by NSERC under grants SAPIN-2018-00027 and RGPAS-2018-522453 and the Arthur B. McDon-ald Canadian Astroparticle Physics Research Institute. Calculations were performed with an allocation of computing resources at the Julich Su-percomputing Center and Cedar at WestGrid with The Digital Research Alliance of Canada. The publisher acknowledges the US government li-cense to provide public access under the DOE Public Access Plan (http://energy.gov/downloads/doe-public-access-plan) .en
dc.description.statusPeer-revieweden
dc.format.extent6en
dc.identifier.issn0370-2693en
dc.identifier.otherWOS:001278285100001en
dc.identifier.otherORCID:/0000-0002-0198-9901/work/165894360en
dc.identifier.scopus85198512878en
dc.identifier.urihttp://www.scopus.com/inward/record.url?scp=85198512878&partnerID=8YFLogxKen
dc.identifier.urihttps://hdl.handle.net/1885/733755409
dc.language.isoenen
dc.rightsPublisher Copyright: © 2024 The Author(s)en
dc.sourcePhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physicsen
dc.subjectCore excitationsen
dc.subjectCoulomb-excitationen
dc.subjectEven titaniumen
dc.subjectGeneralized seniorityen
dc.subjectNpnn schemeen
dc.subjectNucleien
dc.subjectShell-model descriptionen
dc.subjectSpectroscopyen
dc.titleSuppressed electric quadrupole collectivity in <sup>49</sup>Tien
dc.typeJournal articleen
dspace.entity.typePublicationen
local.contributor.affiliationGray, T. J.; Oak Ridge National Laboratoryen
local.contributor.affiliationAllmond, J. M.; Oak Ridge National Laboratoryen
local.contributor.affiliationBenetti, C.; Florida State Universityen
local.contributor.affiliationWibisono, C.; Florida State Universityen
local.contributor.affiliationBaby, L.; Florida State Universityen
local.contributor.affiliationGargano, A.; National Institute for Nuclear Physicsen
local.contributor.affiliationMiyagi, T.; Technische Universität Darmstadten
local.contributor.affiliationMacchiavelli, A. O.; Oak Ridge National Laboratoryen
local.contributor.affiliationStuchbery, A. E.; Department of Nuclear Physics & Accelerator Applications, Research School of Physics, ANU College of Science and Medicine, The Australian National Universityen
local.contributor.affiliationWood, J. L.; Georgia Institute of Technologyen
local.contributor.affiliationAjayi, S.; Florida State Universityen
local.contributor.affiliationAragon, J.; Florida State Universityen
local.contributor.affiliationAsher, B. W.; University of Tennessee, Knoxvilleen
local.contributor.affiliationBarber, P.; Florida State Universityen
local.contributor.affiliationBhattacharya, S.; Florida State Universityen
local.contributor.affiliationBoisseau, R.; Florida State Universityen
local.contributor.affiliationChristie, J. M.; University of Tennessee, Knoxvilleen
local.contributor.affiliationConley, A. L.; Florida State Universityen
local.contributor.affiliationDe Rosa, P.; Florida State Universityen
local.contributor.affiliationDowling, D. T.; Oak Ridge National Laboratoryen
local.contributor.affiliationEsparza, C.; Florida State Universityen
local.contributor.affiliationGibbons, J.; Florida State Universityen
local.contributor.affiliationHanselman, K.; Florida State Universityen
local.contributor.affiliationHolt, J. D.; TRIUMFen
local.contributor.affiliationLopez-Caceres, S.; Louisiana State Universityen
local.contributor.affiliationLopez Saavedra, E.; Florida State Universityen
local.contributor.affiliationMcCann, G. W.; Florida State Universityen
local.contributor.affiliationMorelock, A.; Florida State Universityen
local.contributor.affiliationKelly, B.; Florida State Universityen
local.contributor.affiliationKing, T. T.; Oak Ridge National Laboratoryen
local.contributor.affiliationRasco, B. C.; Oak Ridge National Laboratoryen
local.contributor.affiliationSitaraman, V.; Florida State Universityen
local.contributor.affiliationTabor, S. L.; Florida State Universityen
local.contributor.affiliationTemanson, E.; Florida State Universityen
local.contributor.affiliationTripathi, V.; Florida State Universityen
local.contributor.affiliationWiedenhöver, I.; Florida State Universityen
local.contributor.affiliationYadav, R. B.; South Carolina State Universityen
local.identifier.citationvolume855en
local.identifier.doi10.1016/j.physletb.2024.138856en
local.identifier.pure45660426-cea9-4792-ae54-4617bffe24c4en
local.identifier.urlhttps://www.scopus.com/pages/publications/85198512878en
local.type.statusPublisheden

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