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The Possible Interpretations of Y(4260)

High Energy Physics - Phenomenology 2008-11-26 v2 High Energy Physics - Experiment High Energy Physics - Lattice

Abstract

The recently observed Y(4260) lies far above the decay threshold with a width less than 100 MeV. We argue that it's very difficult to accommodate Y(4260) as a conventional ccˉc\bar c radial excitation or a D-wave state. It can't be a hadronic molecule. Its production mechanism and special decay pattern do not favor the glueball interpretation. If Y(4260) is a scalar tetraquark, it must be produced by the I=0 component of the virtual photon. Then the I=1,Iz=0I=1, I_z=0 component of the virtual photon should have produced its isovector partner Y(4260)Y^\prime (4260), which may be searched for in the decay channel π+ππ0J/ψ\pi^+\pi^-\pi^0 J/\psi using exactly the same database from the initial state radiation process. The observation/non-observation of Y(4260)Y^\prime (4260) can easily confirm/reject the tetraquark hypothesis. However, a tetraquark far above threshold can fall apart into DDˉ,DDˉD\bar D, D^\ast\bar D very easily. Its not-so-large width and the non-observation of DDˉD\bar D mode tend to disfavor the tetraquark hypothesis. Hence the only feasible interpretation is a hybrid charmonium if Y(4260) is {\sl NOT} an experimental artifact. At present, none of the experimental information from BABAR measurement is in conflict with the hybrid charmonium picture.

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Cite

@article{arxiv.hep-ph/0507025,
  title  = {The Possible Interpretations of Y(4260)},
  author = {Shi-Lin Zhu},
  journal= {arXiv preprint arXiv:hep-ph/0507025},
  year   = {2008}
}

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