4,237 research outputs found

    Search for β+\beta^+EC and ECEC processes in 112^{112}Sn and ββ\beta^-\beta^- decay of 124^{124}Sn to the excited states of 124^{124}Te

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    Limits on β+\beta^+EC and ECEC processes in 112^{112}Sn and on ββ\beta^-\beta^- decay of 124^{124}Sn to the excited states of 124^{124}Te have been obtained using a 380 cm3^3 HPGe detector and an external source consisting of natural tin. A limit with 90% C.L. on the 112^{112}Sn half-life of 0.92×10200.92\times 10^{20} y for the ECEC(0ν\nu) transition to the 03+0^+_3 excited state in 112^{112}Cd (1871.0 keV) has been established. This transition is discussed in the context of a possible enhancement of the decay rate by several orders of magnitude given that the ECEC(0ν)(0\nu) process is nearly degenerate with an excited state in the daughter nuclide. Prospects for investigating such a process in future experiments are discussed. The ββ\beta^-\beta^- decay limits for 124^{124}Sn to the excited states of 124^{124}Te were obtained on the level of (0.81.2)×1021(0.8-1.2)\times 10^{21} y at the 90% C.L.Comment: 17 pages, 5 figure

    Average and recommended half-life values for two neutrino double beta decay: upgrade-2013

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    All existing positive results on two neutrino double beta decay in different nuclei were analyzed. Using the procedure recommended by the Particle Data Group, weighted average values for half-lives of 48^{48}Ca, 76^{76}Ge, 82^{82}Se, 96^{96}Zr, 100^{100}Mo, 100^{100}Mo - 100^{100}Ru (01+0^+_1), 116^{116}Cd, 130^{130}Te, 136^{136}Xe, 150^{150}Nd, 150^{150}Nd - 150^{150}Sm (01+0^+_1) and 238^{238}U were obtained. Existing geochemical data were analyzed and recommended values for half-lives of 128^{128}Te and 130^{130}Ba are proposed. I recommend the use of these results as the most currently reliable values for half-lives.Comment: 9 p, Invited talk at MEDEX'13 (Prague, Czech Republic, June 11-14, 2013

    Main features of detectors and isotopes to investigate double beta decay with increased sensitivity

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    The current situation in double beta decay experiments , the characteristics of modern detectors and the possibility of increasing the sensitivity to neutrino mass in future experiments are discussed. The issue of the production and use of enriched isotopes in double beta decay experiments is discussed in addition.Comment: 25 pages, 2 figures, 10 table
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