25–30 Jun 2026
Auditorium Maximum
Europe/Warsaw timezone

η and η′ Mesons as Probes of Axion-Like Particles, Hidden Sectors, and CP Violation: Experimental Status and Prospects

30 Jun 2026, 10:30
30m
Medium lecture hall (A and B) (Auditorium Maximum)

Medium lecture hall (A and B)

Auditorium Maximum

Invited Tests of fundamental symmetries and precision experiments Plenary session

Speaker

Marcin Zieliński (Jagiellonian University)

Description

Open problems in particle physics, e.g. the strong CP problem, the nature of dark matter, baryon asymmetry, and anomalies in nuclear transitions [1,2], motivate searches for light weakly coupled particles: ALPs, dark photons, and hidden sector mediators [3]. Light pseudoscalar mesons $\eta$ and $\eta'$ ($J^{PC} = 0^{-+}$) provide a uniquely clean environment for such searches, with suppressed SM backgrounds, rich radiative and leptonic decay channels, and sensitivity to CP-odd phases in the final state.

Over the past two decades, a series of dedicated experiments has established $\eta$ and $\eta'$ mesons as precision probes of BSM physics. Studies at WASA-at-COSY, KLOE-2, and BESIII have progressively refined sensitivity to CP-violating observables, dark photon production, and ALP signatures, reaching branching ratio limits at the $10^{-5}$-$10^{-7}$ level [4-7]. In parallel, the HADES experiment at GSI contributes precision dielectron spectroscopy in hadronic fixed-target collisions,probing the ALP-relevant low-mass $e^+e^-$ region [8].

The most significant future advance will come from REDTOP [9], targeting production rates of $10^{13}$~$\eta$ and $10^{12}$~$\eta'$ per year at high-intensity proton or pion beams. This would push accessible branching ratios to the $10^{-11}$-$10^{-12}$ level, probe ALP-electron couplings at $g_{Ae} \sim 10^{-7}$, and reach CP asymmetries at the $10^{-4}$ level, covering the viable QCD-axion space in the MeV range and discriminating between competing explanations for BSM physics.

This talk presents an experimental overview of current results and the physics potential of future $\eta$ and $\eta'$ programs, with emphasis on the interplay between achievable meson yields, detector performance, and sensitivity to ALPs, dark mediators, and CP violation.

References
[1] A.J. Krasznahorkay et al., Phys. Rev. Lett. 116, 042501 (2016).
[2] J.L. Feng et al., Phys. Rev. Lett. 117, 071803 (2016).
[3] B. Batell, M. Pospelov, A. Ritz, Phys. Rev. D 80, 095024 (2009).
[4] P. Adlarson et al. (WASA-at-COSY), Phys. Rev. C 94, 065206 (2016).
[5] P. Adlarson et al. (WASA-at-COSY), Phys. Lett. B 726, 187 (2013).
[6] A. Anastasi et al. (KLOE-2), JHEP 05 (2016) 019.
[7] M. Ablikim et al. (BESIII), arXiv:2501.10130 [hep-ex].
[8] G. Agakishiev et al. (HADES), Eur. Phys. J. A 41, 243 (2009).
[9] M. Zielinski, C. Gatto, Acta Phys. Polon. Suppl. 18, 4-A5 (2025).

Primary author

Marcin Zieliński (Jagiellonian University)

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