Determine the asymptotic isospin-zero pion-to-kaon scattering phase

Determine experimentally the asymptotic value of the isospin-zero S-wave phase shift for the inelastic scattering process \(\pi\pi\to KK\), \(\psi^0_0(+\infty)\), which is required to fix the large-energy behavior of the two-channel Muskhelishvili–Omnès determinant and associated form factors.

Background

The two-channel dispersive treatment uses the phase shift ψ00(s)\psi^0_0(s) for isospin-zero ππKK\pi\pi\to KK scattering to construct the determinant of the Muskhelishvili–Omnès matrix. Its asymptotic value controls the power-law damping of that determinant and constrains the asymptotic behavior of the individual pion- and kaon-pair form factors.

Experimental information reaches only approximately 2 GeV, where the phase is estimated to lie between 250250^\circ and 290290^\circ. The analysis therefore extrapolates it to 360360^\circ, while noting that alternative asymptotic values would modify the damping and could jeopardize the expected asymptotic behavior. Establishing the asymptotic phase experimentally would reduce this dispersive uncertainty.

References

The phase \psi0_0 (+\infty) is not known experimentally: \psi0_0 at 2~GeV is known from data to be in the range 250\circ--290\circ, and we extrapolate from \psi0_0 (2~\text{GeV}2) to a value of \psi0_0 (+\infty) equal to a multiple of 180\circ, namely $360\circ$.

Implications of two-channel rescattering for charm CP violation from precise dispersive data  (2608.21212 - Pich et al., 21 Aug 2026) in Section 3, Analyticity and evaluation of the CP asymmetries