Scalar, axial-vector and tensor resonances from the rho D^*, omega D^* interaction in the hidden gauge formalism
arXiv:0903.3823 · doi:10.1103/PhysRevD.80.014025
Abstract
We study composite systems of light ( and ) and heavy () vector mesons by using the interaction within the hidden gauge formalism. We find a strong attraction in the isospin, spin channels ; ; with positive parity. The attraction is large enough to strongly bind these mesons in states with these quantum numbers, leading to states which can be identified with and probably with , the last one without experimental spin and parity assignment. In the case of one obtains repulsion and thus, no exotic mesons in this sector are generated in the approach.
References in corpus (6)
- Vector meson-vector meson interaction in a hidden gauge unitary approach
- The ρρinteraction in the hidden gauge formalism and the f_0(1370) and f_2(1270) resonances
- Hidden gauge formalism for the radiative decays of axial-vector mesons
- The s-wave charmed baryon resonances from a coupled-channel approach with heavy quark symmetry
- Study of exotic hadrons in S-wave scatterings induced by chiral interaction in the flavor symmetric limit
- Exotic hadrons in s-wave chiral dynamics
Cited by in corpus (6)
- On the nature of the K*2(1430), K*3(1780), K*4(2045), K*5(2380) and K*6 as K*--multi-rho states
- A new group of doubly charmed molecule with -doublet charmed meson pair
- , , and their bottom partners at finite temperature
- Decay of vector-vector resonances into and a pseudoscalar meson
- A helpful analogy between the covalent bond and Particle Spectroscopy
- Strong decays of , , , and resonances as dynamically generated states of two vector mesons