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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.

Double-beta decay of $^{150}$Nd to excited levels of $^{150}$Sm

TL;DR

The study measures the decay of Nd to excited levels of Sm using a highly purified Nd-containing source and a four-HPGe detector array in the STELLA laboratory, achieving a robust determination for the state and an indication for the state. A complementary maximum-likelihood analysis incorporating potential multi-channel decays yields yr, with a possible channel around 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 processes and inform predictions for neutrinoless modes in related systems.

Abstract

The decay of Nd to the first excited 740.5 keV level of Sm was measured over 5.845 yr with the help of a four-crystal low-background HPGe 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 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 yr. Interpreting an excess of the 334.0-keV peak area as an indication of the decay of Nd to the 334.0 keV excited level of Sm with a half-life of yr, the half-life of Nd for the transition to the 0 level is 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 and transitions of Nd and Nd to several excited levels of Sm and Sm, limits were set at level of yr.

Paper Structure

This paper contains 24 sections, 39 equations, 19 figures, 14 tables.

Figures (19)

  • Figure 1: A simplified decay scheme of $^{150}$Nd NDS150. The energies of the excited levels and of the emitted $\gamma$ quanta are in keV (the relative intensities of the $\gamma$ quanta are given in parentheses). The $Q_{2\beta}$-value for double-$\beta$ decay energy of $^{150}$Nd is taken from Wang:2021, the energies of the excited levels and of the $\gamma$ transitions are taken from the National Nuclear Data Center NuDat database NuDat3.0 accessed December 2024.
  • Figure 2: A simplified decay scheme of $^{148}$Nd NDS148. The energies of the excited levels and of the emitted $\gamma$ quanta are given in keV (the relative intensities of the $\gamma$ quanta are shown in parentheses). The $Q_{2\beta}$-value for double-$\beta$ decay energy of $^{148}$Nd is taken from Wang:2021, the energies of the excited levels and of the $\gamma$ transitions are taken from the National Nuclear Data Center NuDat database NuDat3.0 accessed December 2024.
  • Figure 3: Left: schematic view of the set-up with Nd-containing samples (1) installed in the HPGe-detector system: coaxial HPGe detectors (2), aluminium part of the detector system endcap (3), copper part of the endcap (4), position of radioactive $\gamma$-ray sources (5) during the calibration campaign. Right: photograph of the set-up with the Nd-containing sample installed (the shield is open).
  • Figure 4: Energy spectra in the energy intervals (250–850) keV (a) and (850–2700) keV (b) measured with the Nd-containing sample over 5.845 yr (solid histogram) and without sample for 0.8969 yr (normalized to 5.845 yr, dots) by the low-background HPGe-detector system. The energy of the $\gamma$ peaks is in keV.
  • Figure 5: Accuracy of the energy scale in the spectrum measured with the Nd-containing sample over 5.845 yr in the energy interval 250--630 keV. The ratio $E_{\mathrm{exp}}/E_{\mathrm{Tab}}$ was built for several intense $\gamma$ peaks present in the spectrum. The fit of the data by linear function is shown by a solid line. The positions of $\gamma$ peaks expected after $2\beta$ decay of $^{150}$Nd to the $0_1^+$ ($2_1^+$) excited levels of $^{150}$Sm are shown by blue arrows. Energy of the $\gamma$ transitions NuDat3.0 are in keV.
  • ...and 14 more figures