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dc.contributor.authorHyvärinen, Juhani
dc.contributor.authorSuhonen, Jouni
dc.date.accessioned2016-02-15T06:18:33Z
dc.date.available2016-02-15T06:18:33Z
dc.date.issued2015
dc.identifier.citationHyvärinen, J., & Suhonen, J. (2015). Nuclear matrix elements for 0νββ decays with light or heavy Majorana-neutrino exchange. <i>Physical Review C</i>, <i>91</i>(2), Article 024613. <a href="https://doi.org/10.1103/PhysRevC.91.024613" target="_blank">https://doi.org/10.1103/PhysRevC.91.024613</a>
dc.identifier.otherCONVID_24592930
dc.identifier.otherTUTKAID_65478
dc.identifier.urihttps://jyx.jyu.fi/handle/123456789/48768
dc.description.abstractWe compute the nuclear matrix elements (NMEs) corresponding to the neutrinoless double beta (0νββ) decays of nuclei which attract current experimental interest. We concentrate on ground-state-to-ground-state decay transitions mediated by light (l-NMEs) or heavy (h-NMEs) Majorana neutrinos. The computations are done in realistic single-particle model spaces using the proton-neutron quasiparticle random-phase approximation (pnQRPA) with two-nucleon interactions based on the Bonn one-boson-exchange G matrix. Both the l-NMEs and the h-NMEs include the appropriate short-range correlations, nucleon form factors, and higher-order nucleonic weak currents. In addition, both types of NMEs are corrected for the isospin symmetry by the recently proposed method in which the particle-particle proton-neutron interaction parameter (gpp) is decomposed into isoscalar (gT =0 pp ) and isovector (gT =1 pp ) parts. A detailed analysis of the l-NMEs and the h-NMEs is performed to benchmark our computer code and to compare with other recent calculations which produce h-NMEs that are in tension with each other.
dc.language.isoeng
dc.publisherAmerican Physical Society
dc.relation.ispartofseriesPhysical Review C
dc.subject.otherneutrinoless double beta decay
dc.titleNuclear matrix elements for 0νββ decays with light or heavy Majorana-neutrino exchange
dc.typearticle
dc.identifier.urnURN:NBN:fi:jyu-201601221245
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.updated2016-01-22T07:15:02Z
dc.type.coarhttp://purl.org/coar/resource_type/c_2df8fbb1
dc.description.reviewstatuspeerReviewed
dc.relation.issn0556-2813
dc.relation.numberinseries2
dc.relation.volume91
dc.type.versionpublishedVersion
dc.rights.copyright© 2015 American Physical Society. Published in this repository with the kind permission of the publisher.
dc.rights.accesslevelopenAccessfi
dc.relation.doi10.1103/PhysRevC.91.024613
dc.type.okmA1


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