Strong and radiative decays of X(3872) as a hadronic molecule with a negative parity

Abstract

Properties of X(3872) are studied by regarding it as a $D{D}^{\ast }$ hadronic molecule with $J^{PC}=2^{-+}$ 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 $\mathcal{B}(X(3872)\to J/\psi {\pi }^{+}{\pi }^{-}{\pi }^0)/\mathcal{B}(X(3872)\to J/\psi {\pi }^{+}{\pi }^{-})$. We predict the partial widths of the radiative decays of $X(3872)\to \gamma J/\psi$, $\gamma \psi (2S)$ and the strong decays of $X(3872)\to J/\psi {\pi }^{+}{\pi }^{-}$, $J/\psi {\pi }^{+}{\pi }^{-}{\pi }^0$ as well as $X(3872)\to {\chi }_{cJ}{\pi }^0$. Our analysis shows that the measurement of the ratio $\mathcal{B}(X(3872)\to {\chi }_{c0}{\pi }^0)/\mathcal{B}(X(3872)\to {\chi }_{c1}{\pi }^0)$ may signal the nature of X(3872).

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• The hidden-charm pentaquark and tetraquark states
• Heavy hadronic molecules with pion exchange and quark core couplings: a guide for practitioners
• The $X(3872)\to J/\psi \gamma$ decay in the $D{\bar{D}}^{\ast }$ molecular picture
• X(3872) as a hybrid state of the charmonium and the hadronic molecule
• A Phenomenological analysis on isospin-violating decay of $X(3872)$
• What do the radiative decays of X(3872) tell us
• Unquenched quark-model calculation of X(3872) electromagnetic decays
• Possible hadronic molecular states composed of $S$-wave heavy-light mesons
• Decay properties of the $X(3872)$ through the Fierz rearrangement
• ${\bar{D}}^0{D}^{0\ast }$ $(D^0{\bar{D}}^{0\ast })$ System in QCD-Improved Many Body Potential