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|a Alduino, C.
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|a Alfonso, K.
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|a Artusa, D. R
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|a Avignone III, F. T
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|a Azzolini, O.
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|a Banks, T. I
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|a Bari, G.
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|a Beeman, J. W
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|a Bellini, F.
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|a Bersani, A.
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|a Biassoni, M.
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|a Brofferio, C.
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|a Bucci, C.
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|a Camacho, A.
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|a Caminata, A.
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|a Canonica, L.
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|a Cao, X. G
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|a Capelli, S.
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|a Cappelli, L.
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|a Carbone, L.
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|a Double-beta decay of $$^{130}\hbox {Te}$$130Te to the first $$0^+$$0+ excited state of $$^{130}\hbox {Xe}$$130Xe with CUORE-0
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|b Springer Berlin Heidelberg,
|c 2021-09-20T17:29:10Z.
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|z Get fulltext
|u https://hdl.handle.net/1721.1/131632
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|a Abstract We report on a search for double beta decay of $$^{130}\hbox {Te}$$130Te to the first $$0^{+}$$0+ excited state of $$^{130}\hbox {Xe}$$130Xe using a $$9.8\,\hbox {kg}\cdot \hbox {yr}$$9.8kg·yr exposure of $$^{130}\hbox {Te}$$130Te collected with the CUORE-0 experiment. In this work we exploit different topologies of coincident events to search for both the neutrinoless and two-neutrino double beta decay modes. We find no evidence for either mode and place lower bounds on the half-lives: $$T^{0\nu }_{0^+_1}>7.9\cdot 10^{23}\hbox {yr}$$T01+0ν>7.9·1023yr and $$T^{2\nu }_{0^+_1}>2.4\cdot 10^{23}\hbox {yr}$$T01+2ν>2.4·1023yr ($$90\%\,\hbox {CL}$$90%CL). Combining our results with those obtained by the CUORICINO experiment, we achieve the most stringent constraints available for these processes: $$T^{0\nu }_{0^+_1}>1.4\cdot 10^{24}\hbox {yr}$$T01+0ν>1.4·1024yr and $$T^{2\nu }_{0^+_1}>2.5\cdot 10^{23}\hbox {yr}$$T01+2ν>2.5·1023yr ($$90\%\,\hbox {CL}$$90%CL).
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