Observation Of J-Psi Radiative Decay To Pseudoscalar-Omega-Omega

Rm Baltrusaitis,Jj Becker,Gt Blaylock,Js Brown,Ko Bunnell,Th Burnett,Re Cassell, D Coffman, V Cook,Dh Coward, H Cui, C Delpapa,De Dorfan,Al Duncan,Kf Einsweiler,Bi Eisenstein, R Fabrizio, G Gladding, F Grancagnolo,Rp Hamilton, J Hauser,Ca Heusch,Dg Hitlin, L Kopke,Pm Mockett, L Moss,Rf Mozley, A Nappi, A Odian, R Partridge, J Perrier,Sa Plaetzer,Jd Richman,Jr Roehrig, Jj Russell,Hfw Sadrozinski, M Scarlatella,Tl Schalk, Rh Schindler, A Seiden,Jc Sleeman,Al Spadafora,Jj Thaler, W Toki, Y Unno, F Villa, A Wattenberg, N Wermes,Hj Willutzki, D Wisinski,Wj Wisniewski

PHYSICAL REVIEW LETTERS(1985)

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摘要
We present evidence for the radiative decay J/\\ensuremath{\\psi}\\ensuremath{\\rightarrow}\\ensuremath{\\gamma}\\ensuremath{\\omega}\\ensuremath{\\omega} with a branching fraction of (1.76\\ifmmode\\pm\\else\\textpm\\fi{}0.09\\ifmmode\\pm\\else\\textpm\\fi{}0.45)\\ifmmode\\times\\else\\texttimes\\fi{}${10}^{\\mathrm{\\ensuremath{-}}3}$. The \\ensuremath{\\omega}\\ensuremath{\\omega} invariant-mass distribution peaks at 1.8 GeV/${c}^{2}$, just above threshold. Analysis of angular correlations indicates that \\ensuremath{\\omega}\\ensuremath{\\omega} system below 2 GeV/${c}^{2}$ is predominantly pseudoscalar. Upper limits are presented for the branching fractions of \\ensuremath{\\omega}\\ensuremath{\\omega} decays of the \\ensuremath{\\theta}(1690), the ${g}_{T}$ states near 2.2 GeV/${c}^{2}$, and the ${\\ensuremath{\\eta}}_{c}$.
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