Are Y(4260) and {\rm Z$_2^{+}$(4250)} ${\rm D_1D}$ or ${\rm D_0D^{*}}$ 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 $π$ exchange plays a dominant role. The $σ$ exchange has been taken into account, which leads to diagonal interaction. The contribution of $σ$ 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 $ρ$ and $ω$ exchange almost cancels each other. For the currently allowed values of the effective coupling constants and a reasonable cutoff $Λ$ 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 $π^{+}π^{-}Υ$ and $π^{+}χ_{b1}$ respectively.
21 pages, 3 figures and 7 tables

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