Abstract

We study the processes $\gamma \gamma \to \eta_c \to \eta' K^+ K^-$, $\eta' \pi^+ \pi^-$, and $\eta \pi^+ \pi^-$ using a data sample of 519 $fb^{-1}$ recorded with the BaBar detector operating at the SLAC PEP-II asymmetric-energy $e^+e^-$ collider at center-of-mass energies at and near the $\Upsilon(nS)$ ($n = 2,3,4$) resonances. This is the first observation of the decay $\eta_c \to \eta' K^+ K^-$ and we measure the branching fraction $\Gamma(\eta_c \to \eta' K^+ K^-)/(\Gamma(\eta_c \to \eta' \pi^+ \pi^-)=0.644\pm 0.039_{\rm stat}\pm 0.032_{\rm sys}$. Significant interference is observed between $\gamma \gamma \to \eta_c\to \eta \pi^+ \pi^-$ and the non-resonant two-photon process $\gamma \gamma \to \eta \pi^+ \pi^-$. A Dalitz plot analysis is performed of $\eta_c$ decays to $\eta' K^+ K^-$, $\eta' \pi^+ \pi^-$, and $\eta \pi^+ \pi^-$. Combined with our previous analysis of $\eta_c \to K \bar K \pi$, we measure the $K^*_0(1430)$ parameters and the ratio between its $\eta' K$ and $\pi K$ couplings. The decay $\eta_c \to \eta' \pi^+ \pi^-$ is dominated by the $f_0(2100)$ resonance, also observed in $J/\psi$ radiative decays. A new $a_0(1700) \to \eta \pi$ resonance is observed in the $\eta_c \to \eta \pi^+ \pi^-$ channel. We also compare $\eta_c$ decays to $\eta$ and $\eta'$ final states in association with scalar mesons as they relate to the identification of the scalar glueball.

Highlights

  • Scalar mesons remain a puzzle in light meson spectroscopy: they have complex structure, and there are too many states to be accommodated within the quark model without difficulty [1].In particular, the structure of the isospin I 1⁄4Kπ S wave is still poorly understood, which limits the precision of measurements involving a Kπ system in the final state, including recent searches for CP violation in B meson decay [2], and studies of new exotic resonances [3]and charmed mesons [4].Decays of the ηc, the lightest pseudoscalar ccstate, provide a window on light meson states

  • The analysis reported the first observation of KÃ0ð1430Þ → Kη, and observed that ηc decays into three pseudoscalars are dominated by intermediate scalar mesons

  • V we report the measurement of the ηc branching fraction

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Summary

INTRODUCTION

Scalar mesons remain a puzzle in light meson spectroscopy: they have complex structure, and there are too many states to be accommodated within the quark model without difficulty [1]. The analysis reported the first observation of KÃ0ð1430Þ → Kη, and observed that ηc decays into three pseudoscalars are dominated by intermediate scalar mesons. The JPC 1⁄4 0þþ glueball is predicted to have a mass around 1.7 GeV=c2 Searches for these states have been performed using many supposed “gluon rich” reactions such as radiative decays of the heavy quarkonium states J=ψ [11,12] and Υð1SÞ [13]. We consider the three-body ηc decays to η0KþK−, η0πþπ−, and ηπþπ−, using two-photon interactions, eþe− → eþe−γÃγà → eþe−ηc If both of the virtual photons are quasireal, the allowed JPC values of any produced resonances are 0Æþ; 2Æþ; 4Æþ...

THE BABAR DETECTOR AND DATASET
EFFICIENCY AND ηc INVARIANT-MASS RESOLUTION
YIELDS AND BRANCHING FRACTIONS
Fits to the invariant-mass spectra
Branching fractions
DALITZ PLOT ANALYSES
Findings
SUMMARY

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