1. Double-beta decay of $$^{150}\hbox {Nd}$$ 150 Nd to excited levels of $$^{150}\hbox {Sm}$$ 150 Sm
- Author
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A. S. Barabash, P. Belli, R. Bernabei, R. S. Boiko, F. Cappella, V. Caracciolo, R. Cerulli, F. A. Danevich, D. L. Fang, F. Ferella, A. Incicchitti, V. V. Kobychev, S. I. Konovalov, M. Laubenstein, A. Leoncini, V. Merlo, S. Nisi, O. Niţescu, D. V. Poda, O. G. Polischuk, I. B.-K. Shcherbakov, F. Šimkovic, A. Timonina, V. S. Tinkova, V. I. Tretyak, and V. I. Umatov
- Subjects
Astrophysics ,QB460-466 ,Nuclear and particle physics. Atomic energy. Radioactivity ,QC770-798 - Abstract
Abstract The $$2\nu 2\beta $$ 2 ν 2 β decay of $$^{150}\hbox {Nd}$$ 150 Nd to the first excited 740.5 keV $$0^{+}_{1}$$ 0 1 + level of $$^{150}\hbox {Sm}$$ 150 Sm was measured over 5.845 years with the help of a four-crystal low-background HPGe $$\gamma $$ γ spectrometry system in the underground low-background laboratory STELLA of LNGS-INFN. A 2.381 kg highly purified Nd-containing sample was employed as the decay source. The expected de-excitation gamma-quanta of the $$0^{+}_{1}$$ 0 1 + level with energies 334.0 keV and 406.5 keV were observed both in one-dimensional spectrum and in coincidence data resulting in the half-life $$T_{1/2}=[0.83^{+0.18}_{-0.13}\mathrm {(stat)}^{+0.16}_{-0.19}\mathrm {(syst)}]\times 10^{20}$$ T 1 / 2 = [ 0 . 83 - 0.13 + 0.18 ( stat ) - 0.19 + 0.16 ( syst ) ] × 10 20 year. Interpreting an excess of the 334.0-keV peak area as an indication of the $$2\beta $$ 2 β decay of $$^{150}\hbox {Nd}$$ 150 Nd to the 334.0 keV $$2^+_1$$ 2 1 + excited level of $$^{150}\hbox {Sm}$$ 150 Sm with a half-life of $$T_{1/2}=[1.5^{+2.3}_{-0.6}\mathrm {(stat)}\pm 0.4\mathrm {(syst)}]\times 10^{20}$$ T 1 / 2 = [ 1 . 5 - 0.6 + 2.3 ( stat ) ± 0.4 ( syst ) ] × 10 20 year, the $$2\nu 2\beta $$ 2 ν 2 β half-life of $$^{150}\hbox {Nd}$$ 150 Nd for the transition to the 0 $$^{+}_{1}$$ 1 + level is $$T_{1/2}=[1.03^{+0.35}_{-0.22}\mathrm {(stat)}^{+0.16}_{-0.19}\mathrm {(syst)}]\times 10^{20}$$ T 1 / 2 = [ 1 . 03 - 0.22 + 0.35 ( stat ) - 0.19 + 0.16 ( syst ) ] × 10 20 year, in agreement with the previous experiments. Both half-life values reasonably agree with the theoretical calculations in the framework of proton-neutron QRPA with isospin restoration combined with like nucleon QRPA for description of excited states in the final nuclei. For $$2\nu 2\beta $$ 2 ν 2 β and $$0\nu 2\beta $$ 0 ν 2 β transitions of $$^{150}\hbox {Nd}$$ 150 Nd and $$^{148}\hbox {Nd}$$ 148 Nd to several excited levels of $$^{150}\hbox {Sm}$$ 150 Sm and $$^{148}\hbox {Sm}$$ 148 Sm , limits were set at level of $$T_{1/2}>10^{20}-10^{21}$$ T 1 / 2 > 10 20 - 10 21 year.
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- 2025
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