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The role of f 0 ( 1710 ) in the threshold peak of J / Ψ γ ? ω

机译: f 0 1710 < / mml:math>在?ω阈值峰值中“ si2.gif” display =“ inline” overflow =“ scroll”> J / Ψ γ ω< / mml:mi>

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We study the process J / Ψ → γ ? ω , measured by the BES experiment, where a neat peak close to the ?ω threshold is observed and is associated to a scalar meson resonance around 1800 MeV. We make the observation that a scalar resonance coupling to ?ω unavoidably couples strongly to K K ˉ , but no trace of a peak is seen in the K K ˉ spectrum of the J / Ψ → γ K K ˉ at this energy. This serves us to rule out the interpretation of the observed peak as a signal of a new resonance. After this is done, a thorough study is performed on the production of a pair of vector mesons and how its interaction leads necessarily to a peak in the J / Ψ → γ ? ω reaction close to the ?ω threshold, due to the dynamical generation of the f 0 ( 1710 ) resonance by the vector–vector interaction. We then show that both the shape obtained for the ?ω mass distribution, as well as the strength are naturally reproduced by this mechanism. The work also explains why the ?ω peak is observed in the BES experiment and not in other reactions, like B ± → K ± ? ω of Belle.
机译:我们研究过程J /Ψ→γ?通过BES实验测得的ω,可观察到接近ωω阈值的整齐峰,并与1800 MeV附近的标量介子共振有关。我们观察到,与ωω耦合的标量共振不可避免地与K K strongly强耦合,但是在此能量下,在J /Ψ→γK K the的K Kˉ谱中没有看到峰的痕迹。这有助于我们排除将观察到的峰解释为新共振的信号。完成此操作后,将对一对矢量介子的产生进行彻底的研究,以及其相互作用如何必然导致J /Ψ→γ的峰值?由于矢量之间的相互作用而动态生成了f 0(1710)共振,因此ω反应接近?ω阈值。然后我们表明,通过这种机制自然地再现了由ωω质量分布获得的形状以及强度。这项工作还解释了为什么在BES实验中而不是在其他反应(例如B±→K±?美女的ω。

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