High-precision direct decay energy measurements of the electron-capture decay of
Phys. Rev. C 112, 035501 – Published 17 September, 2025
DOI: https://doi.org/10.1103/g393-xx1w
Abstract
A direct measurement of the ground-state-to-ground-state electron-capture decay () value of has been conducted employing the high-resolving-power phase-imaging ion-cyclotron-resonance technique with the double Penning trap mass spectrometer JYFLTRAP. The resulting value for is 324.82(21) keV, exhibiting a precision approximately 19 times higher than the value adopted in the newest Atomic Mass Evaluation (AME2020) and differing by . Furthermore, by combining this refined value with nuclear energy-level data for the decay-daughter , a potential ultralow -value transition (, ground state) [320(1) keV] was detected. The ground-state-to-excited-state electron-capture decay value () of this transition was determined to be 4.8(10) keV, confirming it to be energetically allowed with a confidence level of exceeding . The captures of electrons occupying the L and higher shells for this transition are energetically allowed, giving a value of 2.0(10) keV for the closest distance of to the allowed binding energy of the L1 shell. To predict partial half-lives and energy-release distributions for this transition, the atomic self-consistent many-electron Dirac-Hartree-Fock-Slater method and the nuclear shell model have been employed. Dominant correction terms such as exchange and overlap corrections, as well as shake-up and shake-off effects, were included in the final results. Moreover, in the case of a possible allowed transition, the normalized distribution of released energy in the electron-capture decay of to the excited 320-keV state of , is compared with that of , which is being used for electron-neutrino-mass determination. A pseudoexperiment technique was introduced to calculate error propagation in half-life and the 68% confidence interval for normalized energy distributions.