European Physical Journal C: Particles and Fields (Jul 2025)

Direct measurement of the $$^{39}$$ 39 Ar half-life from 3.4 years of data with the DEAP-3600 detector

  • P. Adhikari,
  • R. Ajaj,
  • M. Alpízar-Venegas,
  • P.-A. Amaudruz,
  • J. Anstey,
  • D. J. Auty,
  • M. Batygov,
  • B. Beltran,
  • M. A. Bigentini,
  • C. E. Bina,
  • W. M. Bonivento,
  • M. G. Boulay,
  • J. F. Bueno,
  • M. Cadeddu,
  • B. Cai,
  • M. Cárdenas-Montes,
  • S. Cavuoti,
  • Y. Chen,
  • S. Choudhary,
  • B. T. Cleveland,
  • R. Crampton,
  • S. Daugherty,
  • P. DelGobbo,
  • P. Di Stefano,
  • G. Dolganov,
  • L. Doria,
  • F. A. Duncan,
  • M. Dunford,
  • E. Ellingwood,
  • A. Erlandson,
  • S. S. Farahani,
  • N. Fatemighomi,
  • G. Fiorillo,
  • R. J. Ford,
  • D. Gahan,
  • D. Gallacher,
  • A. Garai,
  • P. García Abia,
  • S. Garg,
  • P. Giampa,
  • A. Giménez-Alcázar,
  • D. Goeldi,
  • V. V. Golovko,
  • P. Gorel,
  • K. Graham,
  • A. Grobov,
  • A. L. Hallin,
  • M. Hamstra,
  • S. Haskins,
  • J. Hu,
  • J. Hucker,
  • T. Hugues,
  • A. Ilyasov,
  • B. Jigmeddorj,
  • C. J. Jillings,
  • A. Joy,
  • G. Kaur,
  • A. Kemp,
  • M. Khoshraftar Yazdi,
  • M. Kuźniak,
  • F. La Zia,
  • M. Lai,
  • S. Langrock,
  • B. Lehnert,
  • J. LePage-Bourbonnais,
  • N. Levashko,
  • M. Lissia,
  • L. Luzzi,
  • I. Machulin,
  • A. Maru,
  • J. Mason,
  • A. B. McDonald,
  • T. McElroy,
  • J. B. McLaughlin,
  • C. Mielnichuk,
  • L. Mirasola,
  • A. Moharana,
  • J. Monroe,
  • A. Murray,
  • C. Ng,
  • G. Oliviéro,
  • M. Olszewski,
  • S. Pal,
  • D. Papi,
  • B. Park,
  • M. Perry,
  • V. Pesudo,
  • T. R. Pollmann,
  • F. Rad,
  • C. Rethmeier,
  • F. Retière,
  • I. Rodríguez García,
  • L. Roszkowski,
  • R. Santorelli,
  • F. G. Schuckman II,
  • S. Seth,
  • V. Shalamova,
  • P. Skensved,
  • T. Smirnova,
  • K. Sobotkiewich,
  • T. Sonley,
  • J. Sosiak,
  • J. Soukup,
  • R. Stainforth,
  • M. Stringer,
  • J. Tang,
  • R. Turcotte-Tardif,
  • E. Vázquez-Jáuregui,
  • S. Viel,
  • B. Vyas,
  • M. Walczak,
  • J. Walding,
  • M. Ward,
  • S. Westerdale,
  • R. Wormington,
  • A. Zuñiga-Reyes,
  • DEAP Collaboration

DOI
https://doi.org/10.1140/epjc/s10052-025-14289-5
Journal volume & issue
Vol. 85, no. 7
pp. 1 – 11

Abstract

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Abstract The half-life of $$^{39}$$ 39 Ar is measured using the DEAP-3600 detector located 2 km underground at SNOLAB. Between 2016 and 2020, DEAP-3600 used a target mass of (3269 ± 24) kg of liquid argon distilled from the atmosphere in a direct-detection dark matter search. Such an argon mass also enables direct measurements of argon isotope properties. The decay of $$^{39}$$ 39 Ar in DEAP-3600 is the dominant source of triggers by two orders of magnitude, ensuring high statistics and making DEAP-3600 well-suited for measuring this isotope’s half-life. Use of the pulse-shape discrimination technique in DEAP-3600 allows powerful discrimination between nuclear recoils and electron recoils, resulting in the selection of a clean sample of $$^{39}$$ 39 Ar decays. Observing over a period of 3.4 years, the $$^{39}$$ 39 Ar half-life is measured to be $$(302 \pm 8_\textrm{stat} \pm 6_\textrm{sys})$$ ( 302 ± 8 stat ± 6 sys ) years. This new direct measurement suggests that the half-life of $$^{39}$$ 39 Ar is significantly longer than the accepted value, with potential implications for measurements using this isotope’s half-life as input.