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

Vectorial axion-down-strange coupling from K+→π+νν¯ data

Diego Guadagnoli1,*, Axel Iohner1,†, Cristina Lazzeroni2,‡, Diego Martínez Santos3,§, Joel C. Swallow4,∥, and Claudio Toni1,¶

  • *Contact author: diego.guadagnoli@lapth.cnrs.fr
  • †Contact author: axel.iohner@lapth.cnrs.fr
  • ‡Contact author: cristina.lazzeroni@cern.ch
  • §Contact author: diego.martinez.santos@cern.ch
  • ∥Contact author: joel.swallow@cern.ch
  • Contact author: claudio.toni@lapth.cnrs.fr

Phys. Rev. Research 8, 033262 – Published 2 September, 2026

DOI: https://doi.org/10.1103/r2rg-mc5s

Abstract

We reinterpret publicly available K+→π+νν¯ data collected by NA62 from 2016 to 2024 to constrain the fundamental vectorial coupling of the QCD axion to down and strange quarks. Using a fully reproducible likelihood analysis and a complete renormalization-group evolution of the axion couplings from the Peccei-Quinn (PQ) scale to the kaon scale, we translate the experimental limit into bounds on both the low-energy flavor-violating coupling and the fundamental UV parameters. In the generic regime where strong contributions dominate the decay amplitude, we obtain |(FV)sd(μK)|>1.6×1012GeV. The coexistence of parametrically suppressed weak contributions implies a second, conceptually distinct constraint: The fact that weak-amplitude dominance arises from highly tuned UV coupling configurations translates into a conservative general lower limit on the PQ scale, fa>4.9×104GeV. These results provide the strongest accelerator-based constraints on axion-induced d↔s transitions and establish a robust lower bound on fa, complementary to astrophysical limits.

View figure in article

Physics Subject Headings (PhySH)

Article Text

References (60)

  1. I. G. Irastorza and J. Redondo, New experimental approaches in the search for axion-like particles, Prog. Part. Nucl. Phys. 102, 89 (2018).
  2. G. Lanfranchi, M. Pospelov, and P. Schuster, The search for feebly interacting particles, Annu. Rev. Nucl. Part. Sci. 71, 279 (2021).
  3. P. Sikivie, Invisible axion search methods, Rev. Mod. Phys. 93, 015004 (2021).
  4. G. G. Raffelt, Astrophysical methods to constrain axions and other novel particle phenomena, Phys. Rep. 198, 1 (1990).
  5. G. G. Raffelt, Astrophysical axion bounds, Lect. Notes Phys. 741, 51 (2008).
  6. A. Caputo and G. Raffelt, Astrophysical axion bounds: The 2024 edition, in 1st training school of the COST action COSMIC WISPers (CA21106), Lect. Notes Phys. 741, 51 (2008).
  7. D. J. E. Marsh, Axion cosmology, Phys. Rep. 643, 1 (2016).
  8. J. E. Kim and G. Carosi, Axions and the strong CP problem, Rev. Mod. Phys. 82, 557 (2010); Erratum: 91, 049902(E) (2019).
  9. L. Di Luzio, M. Giannotti, E. Nardi, and L. Visinelli, The landscape of QCD axion models, Phys. Rep. 870, 1 (2020).
  10. K. Choi, S. H. Im, and C. Sub Shin, Recent Progress in the Physics of Axions and Axion-Like Particles, Annu. Rev. Nucl. Part. Sci. 71, 225 (2021).
  11. J. E. Kim, Weak interaction singlet and strong CP invariance, Phys. Rev. Lett. 43, 103 (1979).
  12. M. A. Shifman, A. I. Vainshtein, and V. I. Zakharov, Can confinement ensure natural CP invariance of strong interactions? Nucl. Phys. B 166, 493 (1980).
  13. M. Dine, W. Fischler, and M. Srednicki, A simple solution to the strong CP problem with a harmless axion, Phys. Lett. B 104, 199 (1981).
  14. A. R. Zhitnitsky, On possible suppression of the axion hadron interactions (in Russian), Sov. J. Nucl. Phys. 31, 260 (1980).
  15. R. D. Peccei and H. R. Quinn, CP conservation in the presence of instantons, Phys. Rev. Lett. 38, 1440 (1977).
  16. R. D. Peccei and H. R. Quinn, Constraints imposed by CP conservation in the presence of instantons, Phys. Rev. D 16, 1791 (1977).
  17. S. Weinberg, A new light boson? Phys. Rev. Lett. 40, 223 (1978).
  18. F. Wilczek, Problem of strong P and T invariance in the presence of instantons, Phys. Rev. Lett. 40, 279 (1978).
  19. J. Preskill, M. B. Wise, and F. Wilczek, Cosmology of the invisible axion, Phys. Lett. B 120, 127 (1983).
  20. L. F. Abbott and P. Sikivie, A cosmological bound on the invisible axion, Phys. Lett. B 120, 133 (1983).
  21. M. Dine and W. Fischler, The not so harmless axion, Phys. Lett. B 120, 137 (1983).
  22. C. L. Cowan, F. Reines, F. B. Harrison, H. W. Kruse, and A. D. McGuire, Detection of the free neutrino: A confirmation, Science 124, 103 (1956).
  23. J. Gasser and H. Leutwyler, Chiral perturbation theory to one loop, Ann. Phys. 158, 142 (1984).
  24. S. Weinberg, Phenomenological Lagrangians, Physica A 96, 327 (1979).
  25. H. Georgi, D. B. Kaplan, and L. Randall, Manifesting the invisible axion at low-energies, Phys. Lett. B 169, 73 (1986).
  26. Our definition of the Peccei-Quinn scale coincides with that in the review [9]. The sign difference in the defining aGG̃ term in Eq. (1) arises from our use of opposite ε-tensor conventions relative to those in Ref. [9] (see Appendix pp2).
  27. M. Bauer, M. Neubert, S. Renner, M. Schnubel, and A. Thamm, Consistent treatment of axions in the weak chiral Lagrangian, Phys. Rev. Lett. 127, 081803 (2021).
  28. M. Buschmann, C. Dessert, J. W. Foster, A. J. Long, and B. R. Safdi, Upper limit on the QCD axion mass from isolated neutron star cooling, Phys. Rev. Lett. 128, 091102 (2022).
  29. M. Cavan-Piton, D. Guadagnoli, M. Oertel, H. Seong, and L. Vittorio, Axion emission from strange matter in core-collapse SNe, Phys. Rev. Lett. 133, 121002 (2024).
  30. T. Fischer, J. Martin Camalich, H. Kochankovski, and L. Tolos, Hyperons during proto-neutron star deleptonization and the emission of dark flavored particles, J. Cosmol. Astropart. Phys. 01 (2025) 061.
  31. A. J. Buras and E. Venturini, The exclusive vision of rare K and B decays and of the quark mixing in the standard model, Eur. Phys. J. C 82, 615 (2022).
  32. G. Anzivino et al., Workshop summary: Kaons@CERN 2023, Eur. Phys. J. C 84, 377 (2024).
  33. G. D’Ambrosio, A. M. Iyer, F. Mahmoudi, and S. Neshatpour, Anatomy of kaon decays and prospects for lepton flavor universality violation, J. High Energy Phys. 09 (2022) 148.
  34. E. Cortina Gil et al. (NA62 Collaboration), First search for K+→π+νν¯ using the decay-in-flight technique, Phys. Lett. B 791, 156 (2019).
  35. E. Cortina Gil et al. (NA62 Collaboration), An investigation of the very rare K+→π+νν¯ decay, J. High Energy Phys. 11 (2020) 042.
  36. E. Cortina Gil et al. (NA62 Collaboration), Measurement of the very rare K+→π+νν¯ decay, J. High Energy Phys. 06 (2021) 093.
  37. E. Cortina Gil et al. (NA62 Collaboration), Observation of the K+→π+νν¯ decay and measurement of its branching ratio, J. High Energy Phys. 02 (2024) 191.
  38. E. Cortina Gil et al. (NA62 Collaboration), Searches for hidden sectors using K+→π+X decays, J. High Energy Phys. 11 (2025) 143.
  39. S. Alibocus et al. (NA62 Collaboration), Measurement of the branching ratio of the K+→π+νν¯ decay, arXiv:2607.16413.
  40. E. Cortina Gil et al. (NA62 Collaboration), Search for a feebly interacting particle X in the decay K+→π+X, J. High Energy Phys. 03 (2021) 058.
  41. Alternatively, one may treat K+→π+νν¯ events as a separate component nν left as a free parameter. This approach will become viable in experimental analyses as the observed nν increases. For a fixed number of d.o.f., we find that allowing nν to float strengthens the bounds by approximately 5%–10% compared to fixing it to the SM value. However, we adhere to the latter approach to align fully with the procedure outlined in Ref. [40].
  42. R. D. Cousins, J. T. Linnemann, and J. Tucker, Evaluation of three methods for calculating statistical significance when incorporating a systematic uncertainty into a test of the background-only hypothesis for a poisson process, Nucl. Instrum. Methods Phys. Res. Sect. A 595, 480 (2008).
  43. C. Cornella, A. M. Galda, M. Neubert, and D. Wyler, K±→π±a at next-to-leading order in chiral perturbation theory and updated bounds on ALP couplings, J. High Energy Phys. 06 (2024) 029.
  44. G. Isidori, F. Mescia, and C. Smith, Light-quark loops in K→πνν¯, Nucl. Phys. B 718, 319 (2005).
  45. S. Di Noi and L. Silvestrini, RGESolver: A C++ library to perform renormalization group evolution in the standard model effective theory, Eur. Phys. J. C 83, 200 (2023).
  46. H. Arason, D. J. Castano, B. Keszthelyi, S. Mikaelian, E. J. Piard, P. Ramond, and B. D. Wright, Renormalization group study of the standard model and its extensions. 1. The Standard model, Phys. Rev. D 46, 3945 (1992).
  47. M. Bauer, M. Neubert, S. Renner, M. Schnubel, and A. Thamm, The low-energy effective theory of axions and ALPs, J. High Energy Phys. 04 (2021) 063.
  48. For the QCD axion, the coupling to gluons defines the PQ scale [9] [see Eq. (1)]. For the normalization of the GG̃ operator, see Appendix pp2.
  49. In a different basis, off-diagonal entries of the axion-down-type quark coupling matrix are also induced by the misalignment between the gauge and the mass eigenstates; see e.g., the first term on the right side of Eq. (5.17) of Ref. [47] for the case of choosing the up-quark basis. More generally, the k couplings are defined up to the biunitary transformations of the up- and down-type quark fields that diagonalize the Yukawa matrices. Each of these transformations can induce off-diagonalities even starting from diagonal k matrices.
  50. Specifically, RG effects in off-diagonal k couplings are suppressed below μEW by the Fermi constant and the tiny Yukawa couplings of light quarks [47, 58]; the same effects in diagonal k couplings enter Mw only, and thus amount to contributions to the amplitude of O(GF2).
  51. Jorge Martin Camalich, M. Pospelov, P. N. H. Vuong, R. Ziegler, and J. Zupan, Quark flavor phenomenology of the QCD axion, Phys. Rev. D 102, 015023 (2020).
  52. C. O’Hare, cajohare/axionlimits: Axionlimits, 2020, https://cajohare.github.io/AxionLimits/.
  53. V. Cirigliano, G. Ecker, H. Neufeld, A. Pich, and J. Portoles, Kaon decays in the standard model, Rev. Mod. Phys. 84, 399 (2012).
  54. E. Goudzovski et al., New physics searches at kaon and hyperon factories, Rep. Prog. Phys. 86, 016201 (2023).
  55. O. G. Tchikilev et al., Search for light pseudoscalar sgoldstino in K− decays, Phys. Lett. B 602, 149 (2004).
  56. R. Ogata et al. (E391a Collaboration), Study of the KL0→π0π0νν¯ decay, Phys. Rev. D 84, 052009 (2011).
  57. J. Fry et al. (KOTO Collaboration), Proposal of the KOTO II experiment, arXiv:2501.14827.
  58. M. Bauer, M. Neubert, S. Renner, M. Schnubel, and A. Thamm, Flavor probes of axion-like particles, J. High Energy Phys. 09 (2022) 056.
  59. M. E. Peskin and D. V. Schroeder, An Introduction to Quantum Field Theory (Addison-Wesley, Reading, 1995).
  60. G. Ecker, A. Pich, and E. de Rafael, K+ —> pi Lepton+ Lepton- decays in the effective chiral Lagrangian of the standard model, Nucl. Phys. B 291, 692 (1987).

Outline

Information

Sign In to Your Journals Account

Filter

Filter

Article Lookup

Enter a citation