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dc.contributor.authorDelion, Doru Sabin
dc.contributor.authorSuhonen, Jouni
dc.date.accessioned2015-07-14T10:51:02Z
dc.date.available2015-07-14T10:51:02Z
dc.date.issued2015
dc.identifier.citationDelion, D. S., & Suhonen, J. (2015). Double-β decay within a consistent deformed approach. <i>Physical Review C</i>, <i>91</i>(5), Article 054329. <a href="https://doi.org/10.1103/PhysRevC.91.054329" target="_blank">https://doi.org/10.1103/PhysRevC.91.054329</a>
dc.identifier.otherCONVID_24771196
dc.identifier.otherTUTKAID_66484
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/46508
dc.description.abstractIn this paper we present a timely application of the proton-neutron deformed quasiparticle random-phase approximation (pn-dQRPA), designed to describe in a consistent way the 1+ Gamow-Teller states in oddodd deformed nuclei. For this purpose we apply a projection before variation procedure by using a singleparticle basis with projected angular momentum, provided by the diagonalization of a spherical mean field plus quadrupole-quadrupole interaction. The residual Hamiltonian contains pairing plus proton-neutron dipole terms in particle-hole and particle-particle channels, with constant strengths. As an example we describe the two-neutrino double-beta (2νββ) decay of 150Nd to the ground state of 150Sm. The experimental (p,n) type of strength in 150Nd and the (n,p) type of strength in 150Sm are reasonably reproduced and the 2νββ decay matrix element depicts a strong dependence upon the particle-particle strength gpp. The experimental half-life is reproduced for gpp = 0.05. It turns out that the measured half-lives for 2νββ transitions between other deformed superfluid partners with mass numbers A = 82,96,100,128,130,238 are reproduced with fairly good accuracy by using this value of gpp.fi
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review C
dc.subject.otherdouble-beta decay
dc.titleDouble-β decay within a consistent deformed approach
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201507012489
dc.contributor.laitosFysiikan laitosfi
dc.contributor.laitosDepartment of Physicsen
dc.contributor.oppiaineFysiikkafi
dc.contributor.oppiainePhysicsen
dc.type.urihttp://purl.org/eprint/type/JournalArticle
dc.date.updated2015-07-01T09:15:02Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn0556-2813
dc.relation.numberinseries5
dc.relation.volume91
dc.type.versionpublishedVersion
dc.rights.copyright© American Physical Society 2015. This is a version of an article whose final and definitive form has been published by American Physical Society.
dc.rights.accesslevelopenAccessfi
dc.relation.doi10.1103/PhysRevC.91.054329
dc.type.okmA1


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