Are Y(4260) and {rm Z₂⁺(4250)} {rm D₁D} or {rm D₀D^(*)} Hadronic Molecules?
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In this work, we have investigated whether Y(4260) and ${\rm Z^{+}_2(4250)}$ could be ${\rm D_1D}$ or ${\rm D_0D^{*}}$ molecules in the framework of meson exchange model. The off-diagonal interaction induced by $\pi$ exchange plays a dominant role. The $\sigma$ exchange has been taken into account, which leads to diagonal interaction. The contribution of $\sigma$ exchange is not favorable to the formation of molecular state ${\rm with I^{G}(J^{PC})=0^{-}(1^{--})}$, however, it is beneficial to the binding of molecule ${\rm with I^{G}(J^{P})=1^{-}(1^{-})}$. Light vector meson exchange leads to diagonal interaction as well. For ${\rm Z^{+}_2(4250)}$, the contribution from $\rho$ and $\omega$ exchange almost cancels each other. For the currently allowed values of the effective coupling constants and a reasonable cutoff $\Lambda$ in the range 1-2 GeV, We find that Y(4260) could be accommodated as a ${\rm D_1D}$ and ${\rm D_0D^{*}}$ molecule, whereas the interpretation of ${\rm Z^{+}_2(4250)}$ as a ${\rm D_1D}$ or ${\rm D_0D^{*}}$ molecule is disfavored. The bottom analog of Y(4260) and ${\rm Z^{+}_2(4250)}$ may exist, and the most promising channels to discovery them are $\pi^{+}\pi^{-}\Upsilon$ and $\pi^{+}\chi_{b1}$ respectively.
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