Direct determination of the atomic mass difference of the pairs $^{76}$As-$^{76}$Se and $^{155}$Tb-$^{155}$Gd rules out $^{76}$As and $^{155}$Tb as possible candidates for electron (anti)neutrino mass measurements
Abstract: The first direct determination of the ground-state-to-ground-state $Q$ values of the $\beta-$ decay ${76}$As $\rightarrow$ ${76}$Se and the electron-capture decay ${155}$Tb $\rightarrow$ ${155}$Gd was performed utilizing the double Penning trap mass spectrometer JYFLTRAP. By measuring the atomic mass difference of the decay pairs via the phase-imaging ion-cyclotron-resonance (PI-ICR) technique, the $Q$ values of ${76}$As $\rightarrow$ ${76}$Se and ${155}$Tb $\rightarrow$ ${155}$Gd were determined to be 2959.265(74) keV and 814.94(18) keV, respectively. The precision was increased relative to earlier measurements by factors of 12 and 57, respectively. The new $Q$ values are 1.33 keV and 5 keV lower compared to the values adopted in the most recent Atomic Mass Evaluation 2020. With the newly determined ground-state-to-ground-state $Q$ values combined with the excitation energy from $\gamma$-ray spectroscopy, the $Q$ values for ground-state-to-excited-state transitions ${76}$As (ground state) $\rightarrow$ ${76}$Se$*$ (2968.4(7) keV) and ${155}$Tb (ground state) $\rightarrow$ ${155}$Gd$*$ (815.731(3) keV) were derived to be -9.13(70) keV and -0.79(18) keV. Thus we have confirmed that both of the $\beta{-}$-decay and EC-decay candidate transitions are energetically forbidden at a level of at least 4$\sigma$, thus definitely excluding these two cases from the list of potential candidates for the search of low-$Q$-value $\beta-$ or EC decays to determine the electron-(anti)neutrino mass.
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