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  • Search for ultralight axion...
    Abel, C.; Ayres, N. J.; Ban, G.; Bison, G.; Bodek, K.; Bondar, V.; Chanel, E.; Crawford, C. B.; Daum, M.; Dechenaux, B.; Emmenegger, S.; Flaux, P.; Griffith, W. C.; Harris, P. G.; Kermaidic, Y.; Kirch, K.; Komposch, S.; Koss, P. A.; Krempel, J.; Lauss, B.; Lefort, T.; MohanMurthy, Prajwal; Naviliat Cuncic, Oscar; Pais, D.; Piegsa, F. M.; Pignol, Guillaume; Rawlik, M.; Ries, D.; Roccia, Stephanie; Rozpedzik, D.; Schmidt-Wellenburg, Philipp; Severijns, N.; Stadnik, Y. V.; Thorne, J. A.; Weis, A.; Wursten, E.; Zejma, Jacek; Zsigmond, Geza

    SciPost physics, 08/2023, Letnik: 15, Številka: 2
    Journal Article

    Ultra-low-mass axions are a viable dark matter candidate and may form a coherently oscillating classical field. Nuclear spins in experiments on Earth might couple to this oscillating axion dark-matter field, when propagating on Earth’s trajectory through our Galaxy. This spin coupling resembles an oscillating pseudo-magnetic field which modulates the spin precession of nuclear spins. Here we report on the null result of a demonstration experiment searching for a frequency modulation of the free spin-precession signal of 199Hg in a magnetic field. Our search covers the axion mass range 10^{-16} \textrm{eV} \lesssim m_a \lesssim 10^{-13} \textrm{eV} 10 − 16 eV ≲ m a ≲ 10 − 13 eV and achieves a peak sensitivity to the axion-nucleon coupling of g_{aNN} \approx 3.5 \times 10^{-6} \textrm{GeV}^{-1} g a N N ≈ 3.5 × 10 − 6 GeV − 1 .