Abstract

Properties of X(3872) are studied by regarding it as a DDβˆ—DD^{\ast} hadronic molecule with JPC=2βˆ’+J^{PC} = 2^{-+} in the phenomenological Lagrangian approach. We find that our model with about 97.6% isospin zero component explains the existing data nicely, for example, the ratio B(X(3872)β†’J/ΟˆΟ€+Ο€βˆ’Ο€0)/B(X(3872)β†’J/ΟˆΟ€+Ο€βˆ’)\mathcal{B}(X(3872) \to J/\psi\pi^+\pi^-\pi^0)/\mathcal{B}(X(3872) \to J/\psi\pi^+\pi^-). We predict the partial widths of the radiative decays of X(3872)β†’Ξ³J/ψX(3872) \to \gamma J/\psi, γψ(2S)\gamma \psi(2S) and the strong decays of X(3872)β†’J/ΟˆΟ€+Ο€βˆ’X(3872) \to J/\psi \pi^+ \pi^-, J/ΟˆΟ€+Ο€βˆ’Ο€0J/\psi \pi^+\pi^-\pi^0 as well as X(3872)β†’Ο‡cJΟ€0X(3872) \to \chi_{cJ}\pi^0. Our analysis shows that the measurement of the ratio B(X(3872)β†’Ο‡c0Ο€0)/B(X(3872)β†’Ο‡c1Ο€0)\mathcal{B}(X(3872) \to \chi_{c0}\pi^0)/\mathcal{B}(X(3872) \to \chi_{c1}\pi^0) may signal the nature of X(3872)

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