Reuse & Permissions

It is not necessary to obtain permission to reuse this article or its components as it is available under the terms of the Creative Commons Attribution 4.0 International license. This license permits unrestricted use, distribution, and reproduction in any medium, provided attribution to the author(s) and the published article's title, journal citation, and DOI are maintained. Please note that some figures may have been included with permission from other third parties. It is your responsibility to obtain the proper permission from the rights holder directly for these figures.

Export citation

Export citation

Choose format for download:

Download Citation
  • Open Access

Testing the Dark Origin of Neutrino Masses with Oscillation Experiments

Andrew Cheek1,*, Luca Visinelli2,3,†, and Hong-Yi Zhang1,‡

  • *Contact author: acheek@sjtu.edu.cn
  • †Contact author: lvisinelli@unisa.it
  • ‡Contact author: hongyi18@sjtu.edu.cn

Phys. Rev. Lett. 135, 031801 – Published 16 July, 2025

DOI: https://doi.org/10.1103/wyns-m4y5

Abstract

The origin of neutrino masses remains unknown to date. One popular idea involves interactions between neutrinos and ultralight dark matter, described as fields or particles with masses mϕ≪10  eV. Due to the large phase-space number density, this type of dark matter exists in coherent states and can be effectively described by an oscillating classical field. As a result, neutrino mass-squared differences undergo field-induced interference in spacetime, potentially generating detectable effects in oscillation experiments. We demonstrate that if mϕ≫10−14  eV, the mechanism becomes sensitive to dark matter density fluctuations, which suppresses the oscillatory behavior of flavor-changing probabilities as a function of neutrino propagation distance in a model-independent way, thereby ruling out this regime. Furthermore, by analyzing data from the Kamioka Liquid Scintillator Antineutrino Detector (KamLAND), a benchmark long-baseline reactor experiment, we show that the hypothesis of a dark origin for the neutrino masses is disfavored for mϕ≪10−14  eV, compared to the case of constant mass values in vacuum. This result holds at more than the 4σ level across different datasets and parameter choices. The mass range 10−17  eV≲mϕ≲10−14  eV can be further tested in current and future oscillation experiments by searching for time variations (rather than periodicity) in oscillation parameters.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (57)

  1. B. Pontecorvo, Neutrino experiments and the problem of conservation of leptonic charge, Zh. Eksp. Teor. Fiz. 53, 1717 (1967), http://www.jetp.ras.ru/cgi-bin/dn/e_026_05_0984.pdf.
  2. T. Yanagida, Horizontal gauge symmetry and masses of neutrinos, Conf. Proc. C 7902131, 95 (1979), https://inspirehep.net/files/19a4de25a11cc3ea4ec4e0bd0f45bdbd.
  3. M. Gell-Mann, P. Ramond, and R. Slansky, Complex spinors and unified theories, Conf. Proc. C 790927, 315 (1979), https://inspirehep.net/files/0408ff479a315fb43d9e4574ad06e98e.
  4. R. N. Mohapatra and G. Senjanovic, Neutrino mass and spontaneous parity nonconservation, Phys. Rev. Lett. 44, 912 (1980).
  5. J. Schechter and J. W. F. Valle, Neutrino masses in SU(2)×U(1) theories, Phys. Rev. D 22, 2227 (1980).
  6. V. Trimble, Existence and nature of dark matter in the universe, Annu. Rev. Astron. Astrophys. 25, 425 (1987).
  7. N. Aghanim et al. (Planck Collaboration), Planck 2018 results. I. Overview and the cosmological legacy of Planck, Astron. Astrophys. 641, A1 (2020).
  8. H. Davoudiasl, G. Mohlabeng, and M. Sullivan, Galactic dark matter population as the source of neutrino masses, Phys. Rev. D 98, 021301(R) (2018).
  9. S.-F. Ge and S. J. Parke, Scalar nonstandard interactions in neutrino oscillation, Phys. Rev. Lett. 122, 211801 (2019).
  10. K.-Y. Choi, E. J. Chun, and J. Kim, Neutrino oscillations in dark matter, Phys. Dark Universe 30, 100606 (2020).
  11. M. Sen and A. Y. Smirnov, Refractive neutrino masses, ultralight dark matter and cosmology, J. Cosmol. Astropart. Phys. 01 (2024) 040.
  12. F. Capozzi, I. M. Shoemaker, and L. Vecchi, Neutrino oscillations in dark backgrounds, J. Cosmol. Astropart. Phys. 07 (2018) 004.
  13. J.-W. Lee, Neutrino mass and ultralight dark matter mass from the Higgs mechanism, arXiv:2410.02842.
  14. G.-Y. Huang, M. Lindner, P. Martínez-Miravé, and M. Sen, Cosmology-friendly time-varying neutrino masses via the sterile neutrino portal, Phys. Rev. D 106, 033004 (2022).
  15. R. Plestid and S. Tevosyan, The cosmology of ultralight scalar dark matter coupled to right-handed neutrinos, arXiv:2409.17396.
  16. Y. L. ChoeJo, Y. Kim, and H.-S. Lee, Dirac-Majorana neutrino type oscillation induced by a wave dark matter, Phys. Rev. D 108, 095028 (2023).
  17. Y. Kim and H.-S. Lee, Oscillating scalar potential and its implications for cosmic neutrino background searches, arXiv:2503.04949.
  18. S.-F. Ge, C.-F. Kong, and A. Y. Smirnov, Testing the origins of neutrino mass with supernova-neutrino time delay, Phys. Rev. Lett. 133, 121802 (2024).
  19. J. Liao, D. Marfatia, and K. Whisnant, Light scalar dark matter at neutrino oscillation experiments, J. High Energy Phys. 04 (2018) 136.
  20. Y. Farzan, M. Lindner, W. Rodejohann, and X.-J. Xu, Probing neutrino coupling to a light scalar with coherent neutrino scattering, J. High Energy Phys. 05 (2018) 066.
  21. Neutrinos with a bare mass mi can induce loop corrections to mϕ. For instance, the one-loop radiative correction due to a Yukawa coupling is approximately Δmϕ2∼gi2mi2/(8π2). To maintain a small mϕ without fine-tuning, the coupling constant must satisfy gi≲10−7(mϕ/10−9  eV)(0.1  eV/mi). Since this constraint is model dependent, we do not elaborate further.

  22. N. Dalal and A. Kravtsov, Excluding fuzzy dark matter with sizes and stellar kinematics of ultrafaint dwarf galaxies, Phys. Rev. D 106, 063517 (2022).
  23. M. A. Amin and M. Mirbabayi, A Lower bound on dark matter mass, Phys. Rev. Lett. 132, 221004 (2024).
  24. L. Hui, Wave dark matter, Annu. Rev. Astron. Astrophys. 59, 247 (2021).
  25. E. G. M. Ferreira, Ultra-light dark matter, Astron. Astrophys. Rev. 29, 7 (2021).
  26. G. Dvali and S. Zell, Classicality and quantum break-time for cosmic axions, J. Cosmol. Astropart. Phys. 07 (2018) 064.
  27. I. J. Allali and M. P. Hertzberg, General relativistic decoherence with applications to dark matter detection, Phys. Rev. Lett. 127, 031301 (2021).
  28. A. H. Guth, M. P. Hertzberg, and C. Prescod-Weinstein, Do dark matter axions form a condensate with long-range correlation?, Phys. Rev. D 92, 103513 (2015).
  29. G. Krnjaic, P. A. N. Machado, and L. Necib, Distorted neutrino oscillations from time varying cosmic fields, Phys. Rev. D 97, 075017 (2018).
  30. V. Brdar, J. Kopp, J. Liu, P. Prass, and X.-P. Wang, Fuzzy dark matter and nonstandard neutrino interactions, Phys. Rev. D 97, 043001 (2018).
  31. A. Dev, P. A. N. Machado, and P. Martínez-Miravé, Signatures of ultralight dark matter in neutrino oscillation experiments, J. High Energy Phys. 01 (2021) 094.
  32. A. Berlin, Neutrino oscillations as a probe of light scalar dark matter, Phys. Rev. Lett. 117, 231801 (2016).
  33. S. Navas et al. (Particle Data Group), Review of particle physics, Phys. Rev. D 110, 030001 (2024).
  34. A. Abusleme et al. (JUNO Collaboration), Sub-percent precision measurement of neutrino oscillation parameters with JUNO, Chin. Phys. C 46, 123001 (2022).
  35. F. An et al. (JUNO Collaboration), Neutrino physics with JUNO, J. Phys. G 43, 030401 (2016).
  36. J. F. Navarro, C. S. Frenk, and S. D. M. White, A universal density profile from hierarchical clustering, Astrophys. J. 490, 493 (1997).
  37. P. Salucci, F. Nesti, G. Gentile, and C. F. Martins, The dark matter density at the Sun’s location, Astron. Astrophys. 523, A83 (2010).
  38. M. Pato, F. Iocco, and G. Bertone, Dynamical constraints on the dark matter distribution in the Milky Way, J. Cosmol. Astropart. Phys. 12 (2015) 001.
  39. J. Bovy and S. Tremaine, On the local dark matter density, Astrophys. J. 756, 89 (2012).
  40. H. Nakatsuka, S. Morisaki, T. Fujita, J. Kume, Y. Michimura, K. Nagano, and I. Obata, Stochastic effects on observation of ultralight bosonic dark matter, Phys. Rev. D 108, 092010 (2023).
  41. G. P. Centers et al., Stochastic fluctuations of bosonic dark matter, Nat. Commun. 12, 7321 (2021).
  42. M. Lisanti, M. Moschella, and W. Terrano, Stochastic properties of ultralight scalar field gradients, Phys. Rev. D 104, 055037 (2021).
  43. B. Eggemeier, C. A. J. O’Hare, G. Pierobon, J. Redondo, and Y. Y. Y. Wong, Axion minivoids and implications for direct detection, Phys. Rev. D 107, 083510 (2023).
  44. J. Chen and H.-Y. Zhang, Novel structures and collapse of solitons in nonminimally gravitating dark matter halos, J. Cosmol. Astropart. Phys. 10 (2024) 005.
  45. N. Dalal, J. Bovy, L. Hui, and X. Li, Don’t cross the streams: Caustics from fuzzy dark matter, J. Cosmol. Astropart. Phys. 03 (2021) 076.
  46. J. Chen, X. Du, E. W. Lentz, D. J. E. Marsh, and J. C. Niemeyer, New insights into the formation and growth of boson stars in dark matter halos, Phys. Rev. D 104, 083022 (2021).
  47. G. Bak et al. (RENO Collaboration), Measurement of reactor antineutrino oscillation amplitude and frequency at RENO, Phys. Rev. Lett. 121, 201801 (2018).
  48. H. de Kerret et al. (Double Chooz Collaboration), Double Chooz θ13 measurement via total neutron capture detection, Nat. Phys. 16, 558 (2020).
  49. F. P. An et al. (Daya Bay Collaboration), Precision measurement of reactor antineutrino oscillation at kilometer-scale baselines by Daya Bay, Phys. Rev. Lett. 130, 161802 (2023).
  50. A. Gando et al. (KamLAND Collaboration), Reactor on-off antineutrino measurement with KamLAND, Phys. Rev. D 88, 033001 (2013).
  51. C. Bemporad, G. Gratta, and P. Vogel, Reactor based neutrino oscillation experiments, Rev. Mod. Phys. 74, 297 (2002).
  52. J. Buchner, A statistical test for nested sampling algorithms, Stat. Comput. 26, 383 (2016).
  53. J. Buchner, Collaborative nested sampling: Big data versus complex physical models, Publ. Astron. Soc. Pac. 131, 108005 (2019).
  54. J. Buchner, UltraNest—A robust, general purpose Bayesian inference engine, J. Open Source Software 6, 3001 (2021).
  55. I. Esteban, M. C. Gonzalez-Garcia, M. Maltoni, I. Martinez-Soler, J. a. P. Pinheiro, and T. Schwetz, NuFit-6.0: Updated global analysis of three-flavor neutrino oscillations, J. High Energy Phys. 12 (2024) 216.
  56. Note that a more rigorous treatment of the θ12 effect would involve recomputing the solar neutrino fit for each tested value of δm122, since small correlations do exist, e.g. through the mixing in the resonance region. However, the published global solar+KamLAND results show that sin2θ12 remains stable at the level of 0.01 even when δm122 shifts by its current uncertainty of ∼1σ [57]. This subtle dependence has a small numerical impact on our analysis. A fully consistent solar reanalysis is beyond the scope of this Letter.

  57. J. N. Bahcall, M. C. Gonzalez-Garcia, and C. Pena-Garay, Solar neutrinos before and after neutrino 2004, J. High Energy Phys. 08 (2004) 016.

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation