Search for missing ψ(4S)ψ(4S) in the e+e−→π+π−ψ(2S)e^+e^-\to π^+π^-ψ(2S) process

preprint2016arXivOpen access

Abstract

A detailed analysis to find a missing ψ(4S)ψ(4S) is made by utilizing the recent precise mesurements of the cross section for the process e+e−→ψ(2S)π+π−e^+e^-\to ψ(2S)π^+π^- by Belle. Assuming three resonances Y(4360)Y(4360), Y(4660)Y(4660), and ψ(4S)ψ(4S) to fit the data, we obtain the resonance parameters for ψ(4S)ψ(4S) as m=4243m=4243 MeV and Γ=16±31Γ=16 \pm 31 MeV showing a narrow state as predicted before. A combined fit to the data e+e−→ψ(2S)π+π−, hcπ+π−e^+ e^- \to ψ(2S) π^+ π^-, \ h_c π^+ π^-, and χc0ωχ_{c0} ω is also performed to obtain the similar resonance parameters of ψ(4S)ψ(4S). The upper limit of the branching ratio is fitted to be B(ψ(4S)→ψ(2S)π+π−)<3×10−3\mathcal{B}(ψ(4S)\toψ(2S)π^+π^-) < 3\times 10^{-3}, which can be understood by hadronic loop contributions in reasonable parameters range. In addition, the ratios of the branching ratios of the ψ(4S)ψ(4S) dipion transition to the one of ψ(4S)→χc0ωψ(4S)\toχ_{c0}ω are fitted, which can be further measured by BESIII and forthcoming BelleII to confirm the existence of ψ(4S)ψ(4S).

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