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Dispersive analysis of the $\boldsymbol{φ\to γπ^0 π^0}$ process

Bai-Long Hoid, Igor Danilkin, Marc Vanderhaeghen

Abstract

We present an analysis of the radiative decay $φ\to γπ^0 π^0$ in a dispersive framework, where the two-pion subsystem undergoes strong final-state interactions that cover the $f_0(500)$ and $f_0(980)$ regions. We employ a coupled-channel Muskhelishvili-Omnès framework that allows for a consistent treatment of two scalar resonances and crossed-channel singularities induced by the Born and vector-meson exchanges. We explicitly verify the equivalence between the modified and standard Muskhelishvili-Omnès representations for vector-meson pole contributions when the isoscalar Omnès matrix is chosen asymptotically bounded, and we adopt the standard representation in decay kinematics. This yields, for the first time, a parameter-free dispersive prediction for the kaon Born rescattering, which provides a dominant contribution. To obtain a good fit to the KLOE and SND data, we employ a once-subtracted coupled-channel dispersion relation with heavier left-hand cut contributions and two unknown subtraction constants. The results demonstrate the consistency among the data for $ππ$ scattering, $γγ$ fusion, and $φ$ radiative decay, thereby validating the underlying dispersive formalism and the input used for the hadronic Omnès matrix and left-hand cuts.

Dispersive analysis of the $\boldsymbol{φ\to γπ^0 π^0}$ process

Abstract

We present an analysis of the radiative decay in a dispersive framework, where the two-pion subsystem undergoes strong final-state interactions that cover the and regions. We employ a coupled-channel Muskhelishvili-Omnès framework that allows for a consistent treatment of two scalar resonances and crossed-channel singularities induced by the Born and vector-meson exchanges. We explicitly verify the equivalence between the modified and standard Muskhelishvili-Omnès representations for vector-meson pole contributions when the isoscalar Omnès matrix is chosen asymptotically bounded, and we adopt the standard representation in decay kinematics. This yields, for the first time, a parameter-free dispersive prediction for the kaon Born rescattering, which provides a dominant contribution. To obtain a good fit to the KLOE and SND data, we employ a once-subtracted coupled-channel dispersion relation with heavier left-hand cut contributions and two unknown subtraction constants. The results demonstrate the consistency among the data for scattering, fusion, and radiative decay, thereby validating the underlying dispersive formalism and the input used for the hadronic Omnès matrix and left-hand cuts.
Paper Structure (8 sections, 47 equations, 3 figures, 2 tables)

This paper contains 8 sections, 47 equations, 3 figures, 2 tables.

Figures (3)

  • Figure 1: Momentum convention in the $\pi^0 \pi^0$ center-of-mass frame.
  • Figure 2: The real and imaginary parts of the $\rho$-pole LHC (couplings set to unity) from the explicit expression and from the dispersive representation \ref{['eq:hv']}. The integrals are evaluated along the complex cuts (see e.g., Ref. Moussallam:2013una). Two evaluations fall on top of each other, while the sharp behavior at $s_\pm$ is due to the narrow width.
  • Figure 3: The differential branching ratio for $\phi\to\gamma\pi^0\pi^0$ as a function of the two-pion invariant mass $\sqrt{s}$. The top panel shows the prediction for the Born rescattering contribution. The bottom panel shows the final fit to the data: the black band represents the fit uncertainty alone, and the grey band denotes the total uncertainty. The $S$-wave contribution is indicated by the dashed line. Data points excluded from the fit are shown as open circles.