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Are Y(4260) and {\rm Z$_2^{+}$(4250)} ${\rm D_1D}$ or ${\rm D_0D^{*}}$ Hadronic Molecules?

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arxiv 0809.4818 v2 pith:P7RQB3G4 submitted 2008-09-28 hep-ph

classification hep-ph
keywords exchangeinteractionmoleculecontributiondiagonalleadsmesonmolecules
verification ladder T0 review T1 audit T2 compute T3 formal

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abstract

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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Cited by 5 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Systematic Study of Coupled-Channel Dynamics in Doubly Heavy Hadronic Molecules

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    Explicit coupled-channel dynamics modifies pole structures and can eliminate or shift higher-lying states in doubly heavy systems, while single-channel models suffice only for near-threshold states like T_cc.

  2. Searching for the pseudoscalar partner of $G(3900)$ via radiative $Y(4230)$ decays

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    Calculates B(Y(4230) → γ G0(3900)) = 3.8×10^{-5}–3.3×10^{-4} assuming P-wave molecular interpretations for both states and a triangle mechanism.

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    A coupled-channel framework is developed and fitted to BESIII data on vector charmonium-like states in the 4.1-4.6 GeV range, concluding that coupled-channel effects with dynamically generated poles explain the line shapes.

  4. Discovery potential of charmonium $2P$ states through the $e^+e^- \to \gamma D\bar{D}$ processes

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    Using the measured e+e- -> gamma X(3872) cross section as a reference, the authors predict measurable e+e- -> gamma chi_c0(2P) and e+e- -> gamma chi_c2(2P) production and propose the gamma D Dbar final state as a sear...

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    Constituent quark model with imported meson parameters predicts lowest 1-- P-wave tetraquark mass near 4.15 GeV and proposes that ψ(4230), ψ(4360), ψ(4660), and Υ(10753) may be such states with possible multiples near...

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