Mass of Y(3940) in Bethe-Salpeter equation for quarks
arXiv:1411.3424 · doi:10.1140/epjc/s10052-015-3315-y
Abstract
The general form of the Bethe-Salpeter wave functions for the bound states composed of two vector fields of arbitrary spin and definite parity is corrected. Using the revised general formalism, we investigate the observed \emph{Y}(3940) state which is considered as a molecule state consisting of . Though the attractive potential between and including one light meson (, , , ) exchange is considered, we find that in our approach the contribution from one- exchange is equal to zero and consider SU(3) symmetry breaking. The obtained mass of \emph{Y}(3940) is consistent with the experimental value.
arXiv comment19 pages, 4 figures, 1 table
References in corpus (7)
- Big-Bang Nucleosynthesis
- Observation of a near-threshold omega-J/psi mass enhancement in exclusive B-->K omega J/psi decays
- Evidence for a Narrow Near-Threshold Structure in the Mass Spectrum in Decays
- Observation of Y(3940) -> J/psi omega in B -> J/psi omega K at BABAR
- Survey of heavy-meson observables
- Y(4143) is probably a molecular partner of Y(3930)
- A global fit to determine the pseudoscalar mixing angle and the gluonium content of the eta' meson
Cited by in corpus (8)
- The hidden-charm pentaquark and tetraquark states
- Non-Standard Heavy Mesons and Baryons, an Experimental Review
- Observation of structures consistent with exotic states from amplitude analysis of decays
- Amplitude analysis of decays
- Analysis of the data at low invariant masses and the and resonances
- Radiative decay of hadronic molecule state for quarks
- Development of Bethe-Salpeter theory for dealing with unstable system
- Calculation of mass and width of unstable molecular state using the developed Bethe-Salpeter theory