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Valence neutron properties relevant to the neutrinoless double-beta decay of Te-130

dc.contributor.authorKay, B.P.
dc.contributor.authorBloxham, T.
dc.contributor.authorMcAllister, S.A.
dc.contributor.authorClark, J.A.
dc.contributor.authorDeibel, C.M.
dc.contributor.authorFreedman, S.J.
dc.contributor.authorFreeman, S J
dc.contributor.authorHan, K.
dc.contributor.authorHoward, A.M.
dc.contributor.authorMitchell, Alan
dc.contributor.authorParker, P.D.
dc.contributor.authorSchiffer, J.P.
dc.contributor.authorSharp, D.K.
dc.contributor.authorThomas, J.S.
dc.date.accessioned2018-11-30T01:19:00Z
dc.date.available2018-11-30T01:19:00Z
dc.date.issued2013
dc.date.updated2018-11-29T08:18:11Z
dc.description.abstractThe valence neutron composition of the 130Te and 130Xe ground states has been studied with a view to constraining calculations of the nuclear matrix element for the neutrinoless double-β decay of 130Te. Single-neutron adding and removing reactions on 128,130Te and 130,132Xe have been used to probe the vacancy of the 0g7/2, 1d5/2, 1d3/2, 2s1/2, and 0h11/2 orbitals. The change in the vacancy of these orbitals, obtained through a self-consistent determination of spectroscopic factors utilizing the Macfarlane-French sum rules, for 130Te→130Xe is shared only between the d, s1/2, and h11/2 orbitals, with the g7/2 playing no significant role. This is in disagreement with recent calculations within both the quasiparticle random-phase approximation and shell-model frameworks, which show a role for the g7/2 orbital that should have been observable. The neutron pairing properties of 130Xe have also been explored through the 132Xe(p,t) reaction showing no evidence for pairing vibrations.
dc.format.mimetypeapplication/pdfen_AU
dc.identifier.issn2469-9985
dc.identifier.urihttp://hdl.handle.net/1885/153898
dc.publisherAmerican Physical Society
dc.sourcePhysical Review C: Nuclear Physics
dc.titleValence neutron properties relevant to the neutrinoless double-beta decay of Te-130
dc.typeJournal article
dcterms.accessRightsOpen Accessen_AU
local.bibliographicCitation.issue1
local.bibliographicCitation.lastpage6
local.bibliographicCitation.startpage1
local.contributor.affiliationKay, B.P., Argonne National Laboratory
local.contributor.affiliationBloxham, T., Lawrence Berkeley National Laboratory
local.contributor.affiliationMcAllister, S.A., University of Manchester
local.contributor.affiliationClark, J.A., Argonne National Laboratory
local.contributor.affiliationDeibel, C.M., Argonne National Laboratory
local.contributor.affiliationFreedman, S.J., University of California
local.contributor.affiliationFreeman, S J, Argonne National Laboratory
local.contributor.affiliationHan, K., University of California
local.contributor.affiliationHoward, A.M., University of Manchester
local.contributor.affiliationMitchell, Alan , College of Science, ANU
local.contributor.affiliationParker, P.D., Yale University
local.contributor.affiliationSchiffer, J.P., Argonne National Laboratory
local.contributor.affiliationSharp, D.K., University of Manchester
local.contributor.affiliationThomas, J.S., University of Manchester
local.contributor.authoruidMitchell, Alan , u1003437
local.description.notesImported from ARIES
local.identifier.absfor020202 - Nuclear Physics
local.identifier.ariespublicationU3488905xPUB17004
local.identifier.citationvolume87
local.identifier.doi10.1103/PhysRevC.87.011302
local.identifier.scopusID2-s2.0-84872699467
local.identifier.thomsonID000313943700001
local.type.statusPublished Version

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