Jun 23 – 27, 2025
Institute of Experimental and Applied Physics, CTU in Prague
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Double beta decay of $^{150}$Nd to the excited levels of $^{150}$Sm

Jun 25, 2025, 2:15 PM
30m
Conference room (Institute of Experimental and Applied Physics, CTU in Prague)

Conference room

Institute of Experimental and Applied Physics, CTU in Prague

Husova 240/5, 11000 Prague 1, Czech Republic
Oral presentation Experiment Experiment

Speaker

Fedir Danevych (INFN sez. Tor Vergata, Rome, Italy)

Description

The search for double beta decay of $^{150}$Nd to the excited levels of $^{150}$Sm was performed at the Gran Sasso underground laboratory of INFN (Italy) with a four-crystal HPGe gamma spectrometer over 5.845 yr by using a highly purified neodymium-containing sample. The two-neutrino double beta transition of $^{150}$Nd to the first 740.5 keV $0^+$ level of $^{150}$Sm was detected in both one-dimensional and coincidence spectra taken, with a half-life $T_{1/2}=[0.83^{+0.18}_{-0.13}(\rm{stat})^{+0.16}_{-0.19}(\rm{syst})] \times 10^{20}$ yr, in agreement with the results of the previous experiments. Some excess of the 334.0-keV peak is observed that is an indication of the $2\nu2\beta$ decay of $^{150}$Nd to the 334.0 keV $2^+$ excited level of $^{150}$Sm with the half-life $T_{1/2} = [1.5^{+2.3}_{-0.6}(\rm{stat}) \pm0.4(\rm{syst})] \times 10^{20}$ yr, that leads also to slightly higher half-life for the $0^+$ to $0^+_1$ transition: of $T_{1/2}=[1.03^{+0.35}_{-0.22}(\rm{stat})^{+0.16}_{-0.19}(\rm{syst})] \times 10^{20}$ yr. The half-life value for the $0^+$ to $2^+_1$ decay does not contradict the existing limits and agrees with the half-life range calculated in the framework of proton-neutron QRPA with isospin restoration combined with like-nucleon QRPA for a description of excited states in the final nuclei. A possible advancement in experimental sensitivity will be briefly discussed.

Primary author

Fedir Danevych (INFN sez. Tor Vergata, Rome, Italy)

Co-authors

Alexander Barabash (Affiliated with an Institute Taking Part in the Experiment) Alice Leoncini (INFN sezione Roma “Tor Vergata”, 00133 Rome, Italy) Antonella Incicchitti (INFN sezione Roma, 00185 Rome, Italy) Anvar Timonina (State Scientific Institution “Institute for Single Crystals” of NASU, Kharkiv 61072, Ukraine) Denys Poda (Université Paris-Saclay, CNRS/IN2P3, IJCLab, 91405 Orsay, France) Dong-Liang Fang Fang (Institute of Modern Physics, Chinese Academy of Sciences, Lanzhou 730000, China) Fabio Cappella (INFN sezione Roma, 00185 Rome, Italy) Fedor Šimkovic (Faculty of Mathematics, Physics and Informatics, Comenius University in Bratislava, 842 48 Bratislava, Slovakia) Francesco Ferella (INFN Laboratori Nazionali del Gran Sasso, 67100 Assergi, AQ, Italy) Ilias Shcherbakov (State Scientific Institution “Institute for Single Crystals” of NASU, Kharkiv 61072, Ukraine) Matthias Laubenstein (INFN Laboratori Nazionali del Gran Sasso, 67100 Assergi, AQ, Italy) Oksana Polischuk (Institute for Nuclear Research of NASU, 03028 Kyiv, Ukraine) Ovidiu Nitescu (Faculty of Mathematics, Physics and Informatics, Comenius University in Bratislava, 842 48 Bratislava, Slovakia) Pierluigi Belli (INFN sezione Roma “Tor Vergata”, 00133 Rome, Italy) Riccardo Cerulli (INFN sezione Roma “Tor Vergata”, 00133 Rome, Italy) Rita Bernabei (INFN sezione Roma “Tor Vergata”, 00133 Rome, Italy) Roman Boiko (Institute for Nuclear Research of NASU, 03028 Kyiv, Ukraine) Stefano Nisi (INFN Laboratori Nazionali del Gran Sasso, 67100 Assergi, AQ, Italy) V.I. Umatov (Affiliated with an Institute Taking Part in the Experiment) Vera Tinkova (Institute for Scintillation Materials of NASU, Kharkiv 61072, Ukraine) Vincenzo Caracciolo (Dipartimento di Fisica, Università di Roma “Tor Vergata”, 00133 Rome, Italy) Vittorio Merlo (INFN sezione Roma “Tor Vergata”, 00133 Rome, Italy) Vladislav Kobychev (Institute for Nuclear Research of NASU, 03028 Kyiv, Ukraine) Volodymyr Tretyak (INFN Laboratori Nazionali del Gran Sasso, 67100 Assergi, AQ, Italy)

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