Double-beta decay of $^{150}$Nd to excited levels of $^{150}$Sm
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. Nitescu, D. V. Poda, O. G. Polischuk, I. B. -K. Shcherbakov, F. Simkovic, A. Timonina, V. S. Tinkova, V. I. Tretyak, V. I. Umatov
TL;DR
The study measures the $2\nu2\beta$ decay of $^{150}$Nd to excited levels of $^{150}$Sm using a highly purified Nd-containing source and a four-HPGe detector array in the STELLA laboratory, achieving a robust $T_{1/2}$ determination for the $0^+_1$ state and an indication for the $2^+_1$ state. A complementary maximum-likelihood analysis incorporating potential multi-channel decays yields $T_{1/2}(^{150}\mathrm{Nd}\rightarrow ^{150}\mathrm{Sm}(0^+_1))=[1.03^{+0.35}_{-0.22}(stat)^{+0.16}_{-0.19}(syst)]\times10^{20}$ yr, with a possible $2^+_1$ channel around $1.5^{+2.3}_{-0.6}\times10^{20}$ yr. The work also presents state-of-the-art theoretical calculations using pn-QRPA with isospin restoration, including exchange and radiative corrections in the phase-space factors, and provides NMEs and PSFs for multiple transitions to excited states. Overall, the results offer stringent benchmarks for nuclear matrix elements relevant to $2\nu2\beta$ processes and inform predictions for neutrinoless modes in related systems.
Abstract
The $2\nu2β$ decay of $^{150}$Nd to the first excited 740.5 keV $0^{+}_{1}$ level of $^{150}$Sm was measured over 5.845 yr with the help of a four-crystal low-background HPGe $γ$ 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 $0^{+}_{1}$ 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 $T_{1/2}=[0.83^{+0.18}_{-0.13}\mathrm{(stat)}^{+0.16}_{-0.19}\mathrm{(syst)}]\times 10^{20}$ yr. Interpreting an excess of the 334.0-keV peak area as an indication of the $2β$ decay of $^{150}$Nd to the 334.0 keV $2^+_1$ excited level of $^{150}$Sm with a half-life of $T_{1/2}=[1.5^{+2.3}_{-0.6}\mathrm{(stat)}\pm 0.4\mathrm{(syst)}]\times10^{20}$ yr, the $2\nu2β$ half-life of $^{150}$Nd for the transition to the 0$^{+}_{1}$ level is $T_{1/2}=[1.03^{+0.35}_{-0.22}\mathrm{(stat)}^{+0.16}_{-0.19}\mathrm{(syst)}]\times 10^{20}$ yr, 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 $2\nu2β$ and $0\nu2β$ transitions of $^{150}$Nd and $^{148}$Nd to several excited levels of $^{150}$Sm and $^{148}$Sm, limits were set at level of $T_{1/2}>10^{20}-10^{21}$ yr.
