- Open Access
Vectorial axion-down-strange coupling from data
Phys. Rev. Research 8, 033262 – Published 2 September, 2026
DOI: https://doi.org/10.1103/r2rg-mc5s
Abstract
We reinterpret publicly available 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 . 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, . These results provide the strongest accelerator-based constraints on axion-induced transitions and establish a robust lower bound on , complementary to astrophysical limits.
Physics Subject Headings (PhySH)
Article Text
References (60)
- I. G. Irastorza and J. Redondo, New experimental approaches in the search for axion-like particles, Prog. Part. Nucl. Phys. 102, 89 (2018).
- G. Lanfranchi, M. Pospelov, and P. Schuster, The search for feebly interacting particles, Annu. Rev. Nucl. Part. Sci. 71, 279 (2021).
- P. Sikivie, Invisible axion search methods, Rev. Mod. Phys. 93, 015004 (2021).
- G. G. Raffelt, Astrophysical methods to constrain axions and other novel particle phenomena, Phys. Rep. 198, 1 (1990).
- G. G. Raffelt, Astrophysical axion bounds, Lect. Notes Phys. 741, 51 (2008).
- 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).
- D. J. E. Marsh, Axion cosmology, Phys. Rep. 643, 1 (2016).
- J. E. Kim and G. Carosi, Axions and the strong problem, Rev. Mod. Phys. 82, 557 (2010); Erratum: 91, 049902(E) (2019).
- L. Di Luzio, M. Giannotti, E. Nardi, and L. Visinelli, The landscape of QCD axion models, Phys. Rep. 870, 1 (2020).
- 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).
- J. E. Kim, Weak interaction singlet and strong CP invariance, Phys. Rev. Lett. 43, 103 (1979).
- M. A. Shifman, A. I. Vainshtein, and V. I. Zakharov, Can confinement ensure natural invariance of strong interactions? Nucl. Phys. B 166, 493 (1980).
- 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).
- A. R. Zhitnitsky, On possible suppression of the axion hadron interactions (in Russian), Sov. J. Nucl. Phys. 31, 260 (1980).
- R. D. Peccei and H. R. Quinn, CP conservation in the presence of instantons, Phys. Rev. Lett. 38, 1440 (1977).
- R. D. Peccei and H. R. Quinn, Constraints imposed by CP conservation in the presence of instantons, Phys. Rev. D 16, 1791 (1977).
- S. Weinberg, A new light boson? Phys. Rev. Lett. 40, 223 (1978).
- F. Wilczek, Problem of strong and invariance in the presence of instantons, Phys. Rev. Lett. 40, 279 (1978).
- J. Preskill, M. B. Wise, and F. Wilczek, Cosmology of the invisible axion, Phys. Lett. B 120, 127 (1983).
- L. F. Abbott and P. Sikivie, A cosmological bound on the invisible axion, Phys. Lett. B 120, 133 (1983).
- M. Dine and W. Fischler, The not so harmless axion, Phys. Lett. B 120, 137 (1983).
- 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).
- J. Gasser and H. Leutwyler, Chiral perturbation theory to one loop, Ann. Phys. 158, 142 (1984).
- S. Weinberg, Phenomenological Lagrangians, Physica A 96, 327 (1979).
- H. Georgi, D. B. Kaplan, and L. Randall, Manifesting the invisible axion at low-energies, Phys. Lett. B 169, 73 (1986).
- Our definition of the Peccei-Quinn scale coincides with that in the review [9]. The sign difference in the defining term in Eq. (1) arises from our use of opposite -tensor conventions relative to those in Ref. [9] (see Appendix pp2).
- 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).
- 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).
- 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).
- 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.
- A. J. Buras and E. Venturini, The exclusive vision of rare and decays and of the quark mixing in the standard model, Eur. Phys. J. C 82, 615 (2022).
- G. Anzivino et al., Workshop summary: Kaons@CERN 2023, Eur. Phys. J. C 84, 377 (2024).
- 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.
- E. Cortina Gil et al. (NA62 Collaboration), First search for using the decay-in-flight technique, Phys. Lett. B 791, 156 (2019).
- E. Cortina Gil et al. (NA62 Collaboration), An investigation of the very rare decay, J. High Energy Phys. 11 (2020) 042.
- E. Cortina Gil et al. (NA62 Collaboration), Measurement of the very rare → decay, J. High Energy Phys. 06 (2021) 093.
- E. Cortina Gil et al. (NA62 Collaboration), Observation of the decay and measurement of its branching ratio, J. High Energy Phys. 02 (2024) 191.
- E. Cortina Gil et al. (NA62 Collaboration), Searches for hidden sectors using decays, J. High Energy Phys. 11 (2025) 143.
- S. Alibocus et al. (NA62 Collaboration), Measurement of the branching ratio of the decay, arXiv:2607.16413.
- E. Cortina Gil et al. (NA62 Collaboration), Search for a feebly interacting particle in the decay , J. High Energy Phys. 03 (2021) 058.
- Alternatively, one may treat events as a separate component left as a free parameter. This approach will become viable in experimental analyses as the observed increases. For a fixed number of d.o.f., we find that allowing 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].
- 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).
- C. Cornella, A. M. Galda, M. Neubert, and D. Wyler, at next-to-leading order in chiral perturbation theory and updated bounds on ALP couplings, J. High Energy Phys. 06 (2024) 029.
- G. Isidori, F. Mescia, and C. Smith, Light-quark loops in , Nucl. Phys. B 718, 319 (2005).
- S. Di Noi and L. Silvestrini, RGESolver: A library to perform renormalization group evolution in the standard model effective theory, Eur. Phys. J. C 83, 200 (2023).
- 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).
- 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.
- For the QCD axion, the coupling to gluons defines the PQ scale [9] [see Eq. (1)]. For the normalization of the operator, see Appendix pp2.
- 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 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 matrices.
- Specifically, RG effects in off-diagonal couplings are suppressed below by the Fermi constant and the tiny Yukawa couplings of light quarks [47, 58]; the same effects in diagonal couplings enter only, and thus amount to contributions to the amplitude of .
- 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).
- C. O’Hare, cajohare/axionlimits: Axionlimits, 2020, https://cajohare.github.io/AxionLimits/.
- V. Cirigliano, G. Ecker, H. Neufeld, A. Pich, and J. Portoles, Kaon decays in the standard model, Rev. Mod. Phys. 84, 399 (2012).
- E. Goudzovski et al., New physics searches at kaon and hyperon factories, Rep. Prog. Phys. 86, 016201 (2023).
- O. G. Tchikilev et al., Search for light pseudoscalar sgoldstino in decays, Phys. Lett. B 602, 149 (2004).
- R. Ogata et al. (E391a Collaboration), Study of the decay, Phys. Rev. D 84, 052009 (2011).
- J. Fry et al. (KOTO Collaboration), Proposal of the KOTO II experiment, arXiv:2501.14827.
- M. Bauer, M. Neubert, S. Renner, M. Schnubel, and A. Thamm, Flavor probes of axion-like particles, J. High Energy Phys. 09 (2022) 056.
- M. E. Peskin and D. V. Schroeder, An Introduction to Quantum Field Theory (Addison-Wesley, Reading, 1995).
- G. Ecker, A. Pich, and E. de Rafael, — pi Lepton+ Lepton- decays in the effective chiral Lagrangian of the standard model, Nucl. Phys. B 291, 692 (1987).