Abstract

We perform a systematic analysis of the J/psi rightarrow gamma pi ^0pi ^0 and rightarrow gamma K_S^0 K_S^0 partial waves measured by BESIII. We use a large set of amplitude parametrizations to reduce the model bias. We determine the physical properties of seven scalar and tensor resonances in the 1–2.5 , {mathrm {GeV}} mass range. These include the well known f_0(1500) and f_0(1710), that are considered to be the primary glueball candidates. The hierarchy of resonance couplings determined from this analysis favors the latter as the one with the largest glueball component.

Highlights

  • The vast majority of observed mesons can be understood as simple qqbound states, in principle strong interactions permit a more complex spectrum

  • The mass we find for the f0(1710) is considerably larger than the Particle Data Group (PDG) average, it is still compatible with many of the determinations listed in the PDG

  • It is worth noting that our poles are compatible with the ones on the BESIII J/ψ → γ ηη decay [44], even if we do not include this channel

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Summary

Introduction

The vast majority of observed mesons can be understood as simple qqbound states, in principle strong interactions permit a more complex spectrum. In a pure Yang–Mills theory, massive gluon bound states (named “glueballs”) populate the spectrum, as shown for example in lattice calculations. The lightest glueball is expected to have J PC = 0++, and a mass between 1.5 and 2 GeV [1,2,3,4,5,6,7,8,9]. An enhanced glueball production is expected in OZI–suppressed processes, i.e

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The dataset
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Amplitude models
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Resonant poles
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Summary
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Full Text
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