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arXiv 2201.12573nucl-ex
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高精度电子俘获测量$^{111}$ In的$Q$值用于电子中微子质量测定

High-precision electron-capture $Q$ value measurement of $^{111}$In for electron-neutrino mass determination

Z. Ge, T. Eronen, A. deRoubin, K. S. Tyrin, L. Canete, S. Geldhof, A. Jokinen, A. Kankainen, J. Kostensalo, J. Kotila, M. I. Krivoruchenko, I. D. Moore, D. A. N… 展开作者

Z. Ge, T. Eronen, A. deRoubin, K. S. Tyrin, L. Canete, S. Geldhof, A. Jokinen, A. Kankainen, J. Kostensalo, J. Kotila, M. I. Krivoruchenko, I. D. Moore, D. A. Nesterenko, J. Suhonen, M. Vilén

摘要:

用双潘宁阱质谱仪JYFLTRAP精确测定了$^{111}$ Cd($1/2^+$)的基态$^{111}$ In($9/2^+$)电子俘获到基态的$Q$值。获得的值为857.63(17)keV,比原子质量评估2020(AME 2020)中提取的值精确近20倍。使用高精度电子捕获$Q$值测量以及$^{111}$ Cd的866.60(6)keV、864.8(3)keV、855.6(10)keV和853.94(7)keV的核能级数据来确定这四种状态在能量上是否允许潜在的超低$Q$值$β^{}$衰变或电子捕获衰变。我们的结果证实了866.60(6)keV的激发态与自旋宇称($J^π$)为3/2 $^{+}$和864.8(3)keV的$J^π$ = 3/2 $^{+}$被排除,因为它们的电子捕获$Q$值小于0 keV,在大约20 $σ$和50 $σ$,分别。在能量上允许电子捕获衰减到853.94(7)keV($J^π$ = 7/2 $^+$)和855.6(10)keV($J^π$ = 3/2 $^+$)的激发态,其中$Q$值分别为3.69(19)keV和2.0(10)keV。允许衰变跃迁$^{111}$ In(9/2 $^{+}$)$\rightarrow$ $^{111}$ Cd(7/2 $^{+}$),其$Q$值为3.69(19)keV,是未来EC实验测量中微子质量的一个潜在的新候选者。结果表明,铟的水平$2p_{1/2}$为这个衰变分支导致一个显着增加的EC事件的数量在能量区域的电子中微子质量敏感。

英文摘要:

A precise determination of the ground state $^{111}$In ($9/2^+$) electron capture to ground state of $^{111}$Cd ($1/2^+$) $Q$ value has been performed utilizing the double Penning trap mass spectrometer, JYFLTRAP. A value of 857.63(17) keV was obtained, which is nearly a factor of 20 more precise than the value extracted from the Atomic Mass Evaluation 2020 (AME2020). The high-precision electron-capture $Q$ value measurement along with the nuclear energy level data of 866.60(6) keV, 864.8(3) keV, 855.6(10) keV, and 853.94(7) keV for $^{111}$Cd was used to determine whether the four states are energetically allowed for a potential ultra-low $Q$-value $β^{}$ decay or electron-capture decay. Our results confirm that the excited states of 866.60(6) keV with spin-parity ($J^π$) of 3/2$^{+}$ and 864.8(3) keV with $J^π$ = 3/2$^{+}$ are ruled out due to their deduced electron-capture $Q$ value being smaller than 0 keV at the level of around 20$σ$ and 50$σ$, respectively. Electron-capture decays to the excited states at 853.94(7) keV ($J^π$ = 7/2$^+$) and 855.6(10) keV ($J^π$ = 3/2$^+$), are energetically allowed with $Q$ values of 3.69(19) keV and 2.0(10) keV, respectively. The allowed decay transition $^{111}$In (9/2$^{+}$) $\rightarrow$ $^{111}$Cd (7/2$^{+}$), with a $Q$ value of 3.69(19) keV, is a potential a new candidate for neutrino-mass measurements by future EC experiments featuring new powerful detection technologies. The results show that the indium level $2p_{1/2}$ for this decay branch leads to a significant increase in the number of EC events in the energy region sensitive to the electron neutrino mass.

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