Prediction of a state and relationship to the claimed
arXiv:1401.2076 · doi:10.1140/epja/i2014-14103-1
Abstract
After discussing the OZI suppression of one light meson exchange in the interaction of with isospin I=1, we study the contribution of two pion exchange to the interaction and the exchange of a heavy vector . We find this latter mechanism weak but enough to barely bind the system in J=2 with a mass around 4000 MeV, while the effect of the two pion exchange is a net attraction but weaker than that from exchange. We discuss this state and try to relate it to the state, above the threshold, claimed in an experiment at BES from and enhancement of the distribution close to threshold. Together with the results from a recent reanalysis of the BES experiment showing that it is compatible with a J=2 state below threshold around 3990 MeV, we conclude that the BES experiment could be showing the existence of the state that we find in our approach.
References in corpus (17)
- Heavy quarkonium: progress, puzzles, and opportunities
- Prediction of narrow and resonances with hidden charm above 4 GeV
- Dynamically Generated Open and Hidden Charm Meson Systems
- Vector meson-vector meson interaction in a hidden gauge unitary approach
- The Heavy Quark Spin Symmetry Partners of the X(3872)
- Nature of the f_0(600) from its N_c dependence at two loops in unitarized Chiral Perturbation Theory
- The ρρinteraction in the hidden gauge formalism and the f_0(1370) and f_2(1270) resonances
- Search for new charmonium states in the processes e+ e- --> J/psi D(*) D(*) at sqrt{s} ~ 10.6 GeV
- Hidden gauge formalism for the radiative decays of axial-vector mesons
- Analysis of the , , and as vector tetraquark states with QCD sum rules
- Possible S-wave Bound-States of Two Pseudoscalar Mesons
- Couplings in coupled channels versus wave functions in the case of resonances: application to the two states
- Baryon states with open beauty in the extended local hidden gauge approach
- Hidden charm dynamically generated resonances and the , reactions
- The radiative decay of into the predicted scalar state X(3700)
- Brief Review of Charm Physics
- Possible and Molecular states in a chiral quark model
Cited by in corpus (31)
- The hidden-charm pentaquark and tetraquark states
- Weak decays of heavy hadrons into dynamically generated resonances
- Heavy-quark spin and flavour symmetry partners of the X(3872) revisited: what can we learn from the one boson exchange model?
- Observation of and a neutral charmoniumlike structure
- BB interactions with static bottom quarks from Lattice QCD
- QCD Sum Rules Approach to the and States
- Employing spin symmetry to disentangle different models for the XYZ states
- Baryon states with open charm in the extended local hidden gauge approach
- The line shapes of the and in the elastic and inelastic channels revisited
- Study of and interactions in and relationship to the , states
- On production in high energy heavy ion collisions
- General considerations on the nature of and from their pole positions
- The structures in a coupled-channels model
- Implications of the and as two different states
- Axial meson exchange and the and resonances as heavy hadron molecules
- The hidden-charm strong decays of the states
- Photoproduction of the charged charmoniumlike
- regeneration in a hadron gas: an update
- The low-lying hidden- and double-charm tetraquark states in a constituent quark model with Instanton-induced Interaction
- -wave coupled channel effects in electron-positron annihilation
- Hadronic molecular states from the interaction
- and scattering from decay
- Understanding the decay mode of via the triangle loop mechanism
- Hadronic molecules with four charm or beauty quarks
- On the two-body decay processes of the predicted three-body resonance
- Enhancement near the threshold in the reaction
- The ground states of hidden-charm tetraquarks and their radial excitations
- Investigating -wave bound states composed of two pseudoscalar mesons
- Pole analysis for the - coupled-channel system
- Signature of an state from and theoretical description of the and as and molecular states
- X, Y and Z States