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dc.contributor.author | Bernabeu Alberola, José | |
dc.contributor.author | Rújula, Álvaro de | |
dc.contributor.author | Jarlskog, Cecilia | |
dc.date.accessioned | 2016-05-03T10:27:07Z | |
dc.date.available | 2016-05-03T10:27:07Z | |
dc.date.issued | 1983 | |
dc.identifier.citation | Bernabeu Alberola, José; Rújula, Álvaro de; Jarlskog, Cecilia (1993) Neutrinoless double electron-capture as a tool to measure the electron neutrino mass Nuclear Physics B 223 1 15 28 | |
dc.identifier.uri | http://hdl.handle.net/10550/53250 | |
dc.description.abstract | A nucleus (Z, A) may capture two atomic electrons to become (Z − 2, A). For Majorana neutrinos this may occur with no neutrino emission, the process is a virtual mixing of the parent atom and the daughter atom with two electron holes. The process becomes real as the daughter atom de-excites. In some cases where the daughter nucleus is excited, the neutrinoless decay may be enhanced by its proximity to a virtual resonance. We identify the 112Sn → 112Cd transition as a good case. The no-neutrino lifetime for mν = 30 eV ranges from 1022 to 1027 years as a function of the insufficiently well determined distance to resonance. The signatures of the two- or no-neutrino modes are very different. | |
dc.language.iso | eng | |
dc.relation.ispartof | Nuclear Physics B, 1993, vol. 223, num. 1, p. 15-28 | |
dc.subject | Física | |
dc.title | Neutrinoless double electron-capture as a tool to measure the electron neutrino mass | |
dc.type | journal article | es_ES |
dc.date.updated | 2016-05-03T10:27:07Z | |
dc.identifier.doi | 10.1016/0550-3213(83)90089-5 | |
dc.identifier.idgrec | 069088 | |
dc.rights.accessRights | open access | es_ES |