Heavy-Quark Symmetry Partners of the Pc(4450) Pentaquark
arXiv:1811.03992 · doi:10.1103/PhysRevD.98.114030
Abstract
The spectrum of heavy-hadron molecules is constrained by heavy-quark symmetry in its different manifestations. Heavy-quark spin symmetry for instance connects the properties of the ground and excited states of heavy hadrons, while heavy-antiquark-diquark symmetry connects the properties of heavy antimesons (, ) and doubly heavy baryons (, ). A prediction of these symmetries is that if the is indeed a bound state, then there should be a series of , , , and partners. The concrete application of heavy-quark spin symmetry indicates that, if the is a molecule, the existence of a partner with similar binding energy --- which we call , given its expected mass --- is likely. Conversely, the application of heavy-antiquark-diquark symmetry indicates that the , , and molecules are likely to bind too, with binding energies in the range.
5 pages; corresponds to published version
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Cited by in corpus (10)
- Pentaquark and Tetraquark states
- Emergence of a complete heavy-quark spin symmetry multiplet: seven molecular pentaquarks in light of the latest LHCb analysis
- Interpretation of the LHCb States as Hadronic Molecules and Hints of a Narrow
- Heavy-quark spin and flavour symmetry partners of the X(3872) revisited: what can we learn from the one boson exchange model?
- Isospin breaking decays as a diagnosis of the hadronic molecular structure of the
- Photoproduction of strange hidden-charm and hidden-bottom states
- New type of doubly charmed molecular pentaquarks containing most strange quarks: Mass spectra, radiative decays, and magnetic moments
- Doubly charmed dibaryon states
- Electromagnetic properties of possible triple-charm molecular hexaquarks
- Hadronic molecules and multiquark states