mesons with hidden charm arising from and dynamics
arXiv:1805.08330 · doi:10.1016/j.physletb.2018.08.034
Abstract
Inspired by the recent discovery of the pentaquark states and , which can be viewed as excited nucleon states with hidden charm, we study the three-body interaction of a kaon and a pair of in isospin 0 and 1. We show that the two body interactions stringently constrained by the existence of the , , , and , which are widely believed to contain large , , and components, inevitably lead to the existence of a heavy meson with hidden charm. Concrete coupled channel three-body calculations yield its mass and width as MeV with . This state, if found experimentally, definitely cannot be accommodated in a picture, and therefore presents a clear case of an exotic hadron.
updated version
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- Excited meson, , with hidden charm as a bound state
- Strong decays of the explicitly exotic doubly charmed bound state
- Faddeev fixed-center approximation to the system and the hidden charm state
- Prediction of possible exotic states in the system
- Molecular states of nature
- One way to verify the molecular picture of exotic hadrons --from to
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- Tri-meson bound state via delocalized ~Bond
- Theoretical investigation of the molecular nature of and and the possibility of observing the bound state in inclusive collisions
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- Binding of the three-hadron system from the lattice effective field theory
- Analysis of the system with QCD sum rules
- Constraining the three-body bound state via the pole
- Faddeev fixed-center approximation to the , and systems
- and its interactions with a kaon: open charm states with strangeness
- The Three-Body System
- Production of the (predicted) in decays
- Electromagnetic properties of the molecular hexaquark state
- Tri-meson state
- Dynamically generated states from the , , and systems within the fixed-center approximation
- states with hidden charm and a three-body nature