Abstract

We investigate heavy quark symmetries for heavy meson hadronic molecules, and explore the consequences of assuming the X(3872) and Zb(10610)Z_b(10610) as an isoscalar DDˉ∗D\bar D^* and an isovector BBˉ∗B\bar B^* hadronic molecules, respectively. The symmetry allows to predict new hadronic molecules, in particular we find an isoscalar 1++1^{++} BBˉ∗B\bar B^* bound state with a mass about 10580 MeV and the isovector charmonium partners of the Zb(10610)Z_b(10610) and the Zb(10650)Z_b(10650) states. Next, we study the X(3872)→D0Dˉ0π0X(3872) \to D^0 \bar D^0π^0 three body decay. This decay mode is more sensitive to the long-distance structure of the X(3872) resonance than its J/ψππJ/ψππ and J/ψ3πJ/\psi3π decays, which are mainly controlled by the short distance part of the X(3872) molecular wave function. We discuss the D0Dˉ0D^0 \bar D^0 final state interactions, which in some situations become quite important. Indeed in these cases, a precise measurement of this partial decay width could provide precise information on the interaction strength between the D(∗)Dˉ(∗)D^{(*)}\bar D^{(*)} charm mesons.

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