Observation of \psi(4040) and \psi(4160) decay into \eta J/\psi
Belle Collaboration: X. L. Wang, Y. L. Han, C. Z. Yuan, C. P. Shen, P., Wang, I. Adachi, H. Aihara, D. M. Asner, V. Aulchenko, T. Aushev, T. Aziz, A., M. Bakich, Y. Ban, B. Bhuyan, G. Bonvicini, A. Bozek, M. Bracko, J., Brodzicka, O. Brovchenko, T. E. Browder, P. Chen

TL;DR
This study measures the decay of (4040) and (4160) into ta J/, providing the first such measurements and revealing their partial widths to this mode around 1 MeV, using data from the Belle detector.
Contribution
First measurement of (4040) and (4160) decays into ta J/, revealing their partial widths and setting limits on other charmonium-like states.
Findings
Observed (4040) and (4160) in ta J/ invariant mass spectrum.
Measured partial widths to ta J/ are about 1 MeV.
No evidence found for Y(4260), Y(4360), (4415), or Y(4660) in this final state.
Abstract
The cross section for e^+e^- \to \eta J/\psi between \sqrt{s}=3.8 GeV/c^2 and 5.3 GeV/c^2 is measured via initial state radiation using 980 fb^{-1} of data on and around the \Upsilon(nS)(n=1,2,3,4,5) resonances collected with the Belle detector at KEKB. Two resonant structures at the \psi(4040) and \psi(4160) are observed in the \eta J/\psi invariant mass distribution. Fitting the mass spectrum with the coherent sum of two Breit-Wigner functions, one obtains BR(\psi(4040)\to\eta J/\psi)\cdot\Gamma_{ee}^{\psi(4040)} = (4.8\pm0.9\pm1.4) eV and BR(\psi(4160)\to\eta J/\psi)\cdot\Gamma_{ee}^{\psi(4160)} = (4.0\pm0.8\pm1.4) eV for one solution and BR(\psi(4040)\to\eta J/\psi)\cdot\Gamma_{ee}^{\psi(4040)} = (11.2\pm1.3\pm1.9) eV and BR(\psi(4160)\to\eta J/\psi)\cdot\Gamma_{ee}^{\psi(4160)} = (13.8\pm1.3\pm2.0) eV for the other solution, where the first errors are statistical and the second are…
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