Searcharxiv⌕ Search

arXiv · 2610.25216

Is there gluonium in the $η^\prime$? The flavour structure of $η$ and $η^\prime$ mixing in radiative $V\to Pγ$ and $P\to Vγ$ decays

Abstract

Radiative $V\to Pγ$ and $P\to Vγ$ decays are conventionally described using constituent-quark mass differences and phenomenological wavefunction-overlap factors as sources of flavour-symmetry breaking. We investigate whether the overlap factors can instead be understood as the effect of mixing of the $η$ and $η^\prime$ with an additional pseudoscalar state, described by an $SO(4)$ rotation among four basis states. A global fit to current data yields a significantly better description than the corresponding three-state limit without overlap factors, while preserving the established $η$-$η^\prime$ and vector-meson mixing angles, and shows that the additional state mixes predominantly with the non-strange component. The conventional overlap-factor description is recovered exactly as the special case in which this mixing is purely non-strange. The non-strange pattern disfavours both a flavour-singlet admixture, as expected from mixing with a pseudoscalar glueball, and the gluonium scenario considered in previous analyses. Radiative decays therefore provide no compelling evidence for gluonium in the $η^\prime$, and the overlap factors are better interpreted in terms of a radially excited non-strange state.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Rafel Escribano, Emilio Royo. 2026-10-18. Is there gluonium in the $η^\prime$? The flavour structure of $η$ and $η^\prime$ mixing in radiative $V\to Pγ$ and $P\to Vγ$ decays. https://arxiv.org/abs/2610.25216

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

New Face of Standard Model: Neutral Magnetic Monopole

We show that the standard model has a totally new type of monopole which has the neutral magnetic charge $4π/\be$, where $\be$ is the neutral charge. This tells that the standard model has two types of monopoles, the well known Cho-Maison type which has the magnetic charge $4π/e$ and the neutral type which has the neutral magnetic charge $4π/\be$. This necessitates the new neutral charge quantization rule $\be=4πn/\bar g$, in addition to the Dirac's electric charge quantization rule $e=4πn/g$. The mass of the new monopole could be less than the Cho-Maison monopole, around 3.28 TeV. We show how to construct the neutral monopole and clarify the topological origin of the new monopole. We discuss the implications of the new monopoles in physics.

hep-ph↗

Where to find $X(17)$?

The Atomki group puts forward the hypothesis of an $X(17)$ particle to explain its anomaly observation in ${^{8}\text{Be}^{*}} \to {^{8}\text{Be}} e^+e^-$ transition. Utilizing experimental results from the Atomki experiments, measurements of the electron's anomalous magnetic moment (AMM), the parity-violating Møller scattering experiment, the NA64 experiment, the KLOE-2 experiment, and the PADME experiment, we derive constraints on the $Xee$ coupling of the hypothetical $X(17)$ boson to electrons. A joint $χ^2$ analysis of the electron's AMM (Cs and Rb measurements) and the parity-violating Møller scattering yields two mutually exclusive solutions. The Cs and Rb AMM constraints restrict the combination $(\varepsilon_e^v)^2-5(\varepsilon_e^a)^2$ with opposite signs. Cs+Møller combination favours a dominant axial-vector coupling $|\varepsilon_e^a|\approx5.3\times10^{-4}\gg|\varepsilon_e^v|$, whereas Rb+Møller favours a dominant vector coupling $|\varepsilon_e^v|\approx6.9\times10^{-4}\gg|\varepsilon_e^a|$. The Møller bound suppresses the subdominant coupling for both solutions. Incorporating NA64 and KLOE-2 limits on $(\varepsilon_e^v)^2+(\varepsilon_e^a)^2$ introduces mild tension for the Cs+Møller solution, while the Rb+Møller solution remains nearly unchanged.

hep-ph↗

Multiparameter Quantum Estimation and Degeneracy Structure in Three-Flavor Neutrino Oscillations

We investigate three-flavor neutrino oscillations within the framework of quantum estimation theory using the quantum Fisher information matrix (QFIM). We analyze all six independent elements of the QFIM for the parameters $θ_{23}$, $δ_{\mathrm{CP}}$, and $Δm^2_{31}$, together with the corresponding quantum Cramér--Rao bounds and normalized parameter correlations. To connect the intrinsic quantum sensitivity of the neutrino state with experimentally accessible information, we further compare the QFI with the classical Fisher information (CFI) associated with flavor-probability measurements. We find that the difference between the quantum and classical information bounds is strongly dependent on the oscillation parameter and $L/E$, demonstrating that the efficiency with which the available quantum information is accessed depends on the measurement. We also investigate probability-degenerate solutions in the $(θ_{23},δ_{\mathrm{CP}})$ parameter space. Although different parameter sets can produce identical $ν_μ\rightarrowν_e$ appearance probabilities at specific $L/E$ values, their corresponding quantum states can remain distinct, as demonstrated by the quantum fidelity. The QFIM differences further reveal distinct local quantum-information geometries for these probability-degenerate solutions, while the corresponding CFIM differences show a parameter and $L/E$ dependent degree of distinguishability accessible through the flavor-probability measurement. Our results demonstrate that QFI and CFI provide complementary information for neutrino parameter estimation, with the QFIM serving as a measurement-independent quantum benchmark and the CFI characterizing the information accessible through a specified measurement.

hep-ph↗