Abstract

We perform calculations for the $\eta_c \to \eta \pi^+ \pi^-$ decay using elements of SU(3) symmetry to see the weight of different trios of pseudoscalars produced in this decay, prior to the final state interaction of the mesons. After that, the interaction of pairs of mesons, leading finally to $\eta \pi^+ \pi^-$, is done using the chiral unitary approach. We evaluate the $\pi^+ \pi^-$ and $\pi \eta$ mass distributions and find large and clear signals for $f_0(500)$, $f_0(980)$ and $a_0(980)$ excitation. The reaction is similar to the $\chi_{c1} \to \eta \pi^+ \pi^-$, which has been recently measured at BESIII and its implementation and comparison with these predictions will be very valuable to shed light on the nature of the low mass scalar mesons.

Highlights

  • The sector of light scalar mesons has been a topic of intense discussions for years [1,2,3,4,5]

  • The discussions in Ref. [6] reveal the large amount of empirical information favoring a dynamical picture in which the interaction of pseudoscalar mesons in coupled channels and constraints of unitarity generate scalar mesons, which would qualify as multichannel pseudoscalar-pseudoscalar molecular states

  • The successful picture incorporating the constraints of unitarity in coupled channels and the dynamics of the chiral Lagrangians [7,8,9] is known as the chiral unitary approach, and either using the inverse amplitude method [10,11,12] or the coupled channels BetheSalpeter equations [13,14,15,16], the success in providing an accurate description in the different reactions where these resonances are produced is remarkable

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Summary

INTRODUCTION

The sector of light scalar mesons has been a topic of intense discussions for years [1,2,3,4,5]. The successful picture incorporating the constraints of unitarity in coupled channels and the dynamics of the chiral Lagrangians [7,8,9] is known as the chiral unitary approach, and either using the inverse amplitude method [10,11,12] or the coupled channels BetheSalpeter equations [13,14,15,16], the success in providing an accurate description in the different reactions where these resonances are produced is remarkable Detailed reviews of such reactions can be seen in Ref. Our limitations to the range below 1200 MeV for the energies of the interacting meson pairs, induce uncertainties on the background, but we can show that these uncertainties are small in the region of π+π− or πη invariant masses below 1200 MeV, making our predictions really solid With these results and clear predictions, we can only encourage the performance of the experiment which is implementable at BESIII

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