Isospin breaking, coupled-channel effects, and X(3872)
arXiv:1207.3954 · doi:10.1103/PhysRevD.86.074022
Abstract
We re-investigate the possibility of X(3872) as a molecule with within the framework of both the one-pion-exchange (OPE) model and the one-boson-exchange (OBE) model. After careful treatment of the S-D wave mixing, the mass difference between the neutral and charged mesons and the coupling of the pair to , a loosely bound molecular state X(3872) emerges quite naturally with large isospin violation in its flavor wave function. For example, the isovector component is 26.24% if the binding energy is 0.30 MeV, where the isospin breaking effect is amplified by the tiny binding energy. After taking into account the phase space difference and assuming the and come from a virtual omega and rho meson respectively, we obtain the ratio of these two hidden-charm decay modes: for the binding energy being 0.3 MeV, which is consistent with the experimental value.
published in Phys. Rev. D
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Cited by in corpus (11)
- Pentaquark and Tetraquark states
- Isospin breaking decays as a diagnosis of the hadronic molecular structure of the
- Heavy molecules and one--exchange model
- The Spin-orbit force, recoil corrections and possible and molecular states
- Hidden-Charm Tetraquarks and Charged Zc States
- A Phenomenological analysis on isospin-violating decay of
- Strong decays of the states
- Is the newly reported a molecular state?
- Angular momentum coefficients for meson strong decay and unquenched quark models
- Searches for isospin-violating transitions
- On the origin of the narrow peak and the isospin symmetry breaking of the (3872)