Dy159 Electron-Capture: A New Candidate for Neutrino Mass Determination

Z. Ge, T. Eronen, K. S. Tyrin, J. Kotila, J. Kostensalo, D. A. Nesterenko, O. Beliuskina, R. de Groote, A. de Roubin, S. Geldhof, W. Gins, M. Hukkanen, A. Jokinen, A. Kankainen, Á. Koszorús, M. I. Krivoruchenko, S. Kujanpää, I. D. Moore, A. Raggio, S. Rinta-Antila, J. Suhonen, V. Virtanen, A. P. Weaver, and A. Zadvornaya
Phys. Rev. Lett. 127, 272301 – Published 29 December 2021

Abstract

The ground state to ground state electron-capture Q value of Dy159 (3/2) has been measured directly using the double Penning trap mass spectrometer JYFLTRAP. A value of 364.73(19) keV was obtained from a measurement of the cyclotron frequency ratio of the decay parent Dy159 and the decay daughter Tb159 ions using the novel phase-imaging ion-cyclotron resonance technique. The Q values for allowed Gamow-Teller transition to 5/2 and the third-forbidden unique transition to 11/2+ state with excitation energies of 363.5449(14) keV and 362.050(40) keV in Tb159 were determined to be 1.18(19) keV and 2.68(19) keV, respectively. The high-precision Q value of transition 3/25/2 from this work, revealing itself as the lowest electron-capture Q value, is used to unambiguously characterize all the possible lines that are present in its electron-capture spectrum. We performed atomic many-body calculations for both transitions to determine electron-capture probabilities from various atomic orbitals and found an order of magnitude enhancement in the event rates near the end point of energy spectrum in the transition to the 5/2 nuclear excited state, which can become very interesting once the experimental challenges of identifying decays into excited states are overcome. The transition to the 11/2+ state is strongly suppressed and found unsuitable for measuring the neutrino mass. These results show that the electron-capture in the Dy159 atom, going to the 5/2 state of the Tb159 nucleus, is a new candidate that may open the way to determine the electron-neutrino mass in the sub-eV region by studying electron-capture. Further experimental feasibility studies, including coincidence measurements with realistic detectors, will be of great interest.

  • Figure
  • Figure
  • Received 14 July 2021
  • Revised 22 September 2021
  • Accepted 30 November 2021

DOI:https://doi.org/10.1103/PhysRevLett.127.272301

© 2021 American Physical Society

Physics Subject Headings (PhySH)

Accelerators & BeamsNuclear Physics

Authors & Affiliations

Z. Ge1,*, T. Eronen1,†, K. S. Tyrin2, J. Kotila3,4, J. Kostensalo1, D. A. Nesterenko1, O. Beliuskina1, R. de Groote1, A. de Roubin5, S. Geldhof1,§, W. Gins1, M. Hukkanen1,5, A. Jokinen1, A. Kankainen1, Á. Koszorús6, M. I. Krivoruchenko2,7,‡, S. Kujanpää1, I. D. Moore1, A. Raggio1, S. Rinta-Antila1, J. Suhonen1, V. Virtanen1, A. P. Weaver8, and A. Zadvornaya1

  • 1Department of Physics, University of Jyväskylä, P.O. Box 35, FI-40014 Jyväskylä, Finland
  • 2National Research Centre “Kurchatov Institute,” Ploschad’ Akademika Kurchatova 1, 123182 Moscow, Russia
  • 3Finnish Institute for Educational Research, University of Jyväskylä, P.O. Box 35, FI-40014 Jyväskylä, Finland
  • 4Center for Theoretical Physics, Sloane Physics Laboratory Yale University, New Haven, Connecticut 06520-8120, USA
  • 5Centre d’Etudes Nucléaires de Bordeaux Gradignan, UMR 5797 CNRS/IN2P3—Université de Bordeaux, 19 Chemin du Solarium, CS 10120, F-33175 Gradignan Cedex, France
  • 6Department of Physics, University of Liverpool, Liverpool L69 7ZE, United Kingdom
  • 7Institute for Theoretical and Experimental Physics, NRC “Kurchatov Institute,” B. Cheremushkinskaya 25, 117218 Moscow, Russia
  • 8School of Computing, Engineering and Mathematics, University of Brighton, Brighton BN2 4JG, United Kingdom

  • *Corresponding author. zhuang.z.ge@jyu.fi
  • Corresponding author. tommi.eronen@jyu.fi
  • Corresponding author. mikhail.krivoruchenko@itep.ru
  • §Present address: KU Leuven, Instituut voor Kern- en Stralingsfysica, B-3001 Leuven, Belgium.

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Vol. 127, Iss. 27 — 31 December 2021

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