Abstract

Reactor neutrino experiments provide a rich environment for the study of axionlike particles (ALPs). Using the intense photon flux produced in the nuclear reactor core, these experiments have the potential to probe ALPs with masses below 10 MeV. We explore the feasibility of these searches by considering ALPs produced through Primakoff and Compton-like processes as well as nuclear transitions. These particles can subsequently interact with the material of a nearby detector via inverse Primakoff and inverse Compton-like scatterings, via axio-electric absorption, or they can decay into photon or electron-positron pairs. We demonstrate that reactor-based neutrino experiments have a high potential to test ALP-photon couplings and masses, currently probed only by cosmological and astrophysical observations, thus providing complementary laboratory-based searches. We furthermore show how reactor facilities will be able to test previously unexplored regions in the ∼MeV ALP mass range and ALP-electron couplings of the order of gaee ∼ 10−8 as well as ALP-nucleon couplings of the order of {g}_{ann}^{(1)} ∼ 10−9, testing regions beyond TEXONO and Borexino limits.

Highlights

  • axionlike particles (ALPs) have been searched for as well in reactor experiments, motivated by theoretical arguments pointed out first by Weinberg and subsequently by Donnelly, Freedman, Lytel, Peccei and Schwartz [3, 30].1 To the best of our knowledge, Axionlike particles (ALP) reactor searches looking for various nuclear magnetic transitions were pioneered at the Bugey reactor [31], and followed by searches carried out by Zehnder and Lehmann et al in which instead ALPs were searched for in nuclear magnetic transitions of 127Ba∗ and 65Cu∗ [32, 33]

  • Nuclear reactor power plants produce a large amount of photons and so they are suitable sources for ALPs production

  • Motivated by the current CEνNS experimental program, which aims at observing CEνNS induced by reactor neutrino fluxes using various low-threshold technologies, we have analyzed the prospects for detection of ALPs in such experiments

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Summary

Axionlike particle interactions

Axionlike particles (ALP) are pseudoscalars that feebly couple to the SM particles They arise in a variety of new physics scenarios, including those related with dark matter in which the pseudoscalar mediates interactions between the dark and visible sectors [57, 58]. In terms of the decay constant and fermion masses, the couplings in the Lagrangian (2.3) are given by gaγγ α 2π. This expression combined with eq (2.4) leads to relations which can be mapped into the axion mass-coupling plane in the form of stripes whose widths depend on the UV completion accounting for the axion effective Lagrangian, namely gaγγ = 2.0 × 10−10 Caγ gaff = 1.8 × 10−7 Caf ma eV mf GeV.

ALPs production and detection mechanisms at reactors
Production and detection through photon-ALP coupling
Production and detection through electron-ALP coupling
Production through nucleon-ALP coupling
Experimental sensitivities
DRU: Xe LEP
Conclusions
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