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    Triangle singularity in the J/ψ→K+K−f0(980)(a0(980))J/\psi \rightarrow K^+ K^- f_0(980)(a_0(980)) decays

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    We study the J/ψ→K+K−f0(980)(a0(980))J/\psi \rightarrow K^+ K^- f_0(980)(a_0(980)) reaction and find that the mechanism to produce this decay develops a triangle singularity around Minv(K−f0/K−a0)≈1515M_{\rm inv}(K^- f_0/K^- a_0) \approx 1515~MeV. The differential width dΓ/dMinv(K−f0/K−a0)d\Gamma / dM_{\rm inv}(K^- f_0/K^- a_0) shows a rapid growth around the invariant mass being 1515~MeV as a consequence of the triangle singularity of this mechanism, which is directly tied to the nature of the f0(980)f_0(980) and a0(980)a_0(980) as dynamically generated resonances from the interaction of pseudoscalar mesons. The branching ratios obtained for the J/ψ→K+K−f0(980)(a0(980))J/\psi \rightarrow K^+ K^- f_0(980)(a_0(980)) decays are of the order of 10−510^{-5}, accessible in present facilities, and we argue that their observation should provide relevant information concerning the nature of the low-lying scalar mesons.Comment: 12 pages, 8 figures, published in EPJ
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