High-precision measurements of the atomic mass and electron-capture decay Q value of 95Tc
Ge, Z., Eronen, T., Sevestrean, V. A., Niţescu, O., Stoica, S., Ramalho, M., Suhonen, J., de Roubin, A., Nesterenko, D., Kankainen, A., Ascher, P., Ayet, S. A. S., Beliuskina, O., Delahaye, P., Flayol, M., Gerbaux, M., Grévy, S., Hukkanen, M., Jaries, A., . . . Virtanen, V. (2024). High-precision measurements of the atomic mass and electron-capture decay Q value of 95Tc. Physics Letters B, 859, Article 139094. https://doi.org/10.1016/j.physletb.2024.139094
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Physics Letters BAuthors
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2024Copyright
© 2024 The Author(s). Published by Elsevier B.V. Funded by SCOAP³
A direct measurement of the ground-state-to-ground-state electron-capture decay Q value of 95Tc has been performed utilizing the double Penning trap mass spectrometer JYFLTRAP. The Q value was determined to be 1695.92(13) keV by taking advantage of the high resolving power of the phase-imaging ion-cyclotron-resonance technique to resolve the low-lying isomeric state of 95Tc (excitation energy of 38.910(40) keV) from the ground state. The mass excess of 95Tc was measured to be −86015.95(18) keV/c2, exhibiting a precision of about 28 times higher and in agreement with the value from the newest Atomic Mass Evaluation (AME2020). Combined with the nuclear energy-level data for the decay-daughter 95Mo, two potential ultra-low Q-value transitions are identified for future long-term neutrino-mass determination experiments. The atomic self-consistent many-electron Dirac–Hartree–Fock–Slater method and the nuclear shell model have been used to predict the partial half-lives and energy-release distributions for the two transitions. The dominant correction terms related to those processes are considered, including the exchange and overlap corrections, and the shake-up and shake-off effects. The normalized distribution of the released energy in the electron-capture decay of 95Tc to excited states of 95Mo is compared to that of 163Ho currently being used for electron-neutrino-mass determination.
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https://converis.jyu.fi/converis/portal/detail/Publication/243640160
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European Commission; Research Council of FinlandFunding program(s)
ERC Consolidator Grant; Research costs of Academy Research Fellow, AoF; Academy Research Fellow, AoF; MSCA Innovative Training Networks (ITN); Academy Project, AoF
The content of the publication reflects only the author’s view. The funder is not responsible for any use that may be made of the information it contains.
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We acknowledge the staff of the Accelerator Laboratory of University of Jyväskylä (JYFL-ACCLAB) for providing stable online beam. We thank the support by the Academy of Finland under the Finnish Centre of Excellence Programme 2012–2017 (Nuclear and Accelerator Based Physics Research at JYFL) and projects No. 306980, 312544, 275389, 284516, 295207, 314733, 315179, 327629, 320062, 354589, 345869 and 354968. The support by the EU Horizon 2020 research and innovation program under grant No. 771036 (ERC CoG MAIDEN) is acknowledged. This project has received funding from the European Union's Horizon 2020 research and innovation programme under grant agreement No. 861198–LISA–H2020-MSCA-ITN-2019. V.A.S., O.N., S.S., J.S., and J.K. acknowledge support from project PNRR-I8/C9-CF264, Contract No. 760100/23.05.2023 of the Romanian Ministry of Research, Innovation and Digitization. The work leading to this publication was supported by the Deutsche Forschungsgemeinschaft (DFG, German Research Foundation) - AY 155/2-1. The paper was supported by the DAAD Grant No. 57610603. ...License
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