Why the f(0)(980) is mostly ssbar
arXiv:hep-ph/0009265 · doi:10.1016/S0370-2693(00)01264-8
Abstract
We exploit the W-emission process to study the measured weak decay of the D(s,+)(1.9686) meson into f(0)(980) and a positively charged pion. We conclude that the scalar f(0)(980) meson contains mostly strange-antistrange flavors, which is supported by different model studies.
5 pages, plain LaTeX, minor changes, acknowledgments
References in corpus (3)
Cited by in corpus (23)
- QCD sum rule approach for the light scalar mesons as four-quark states
- Probing the structure of through radiative decays
- Study of and from and Decays
- The structure of from charmed mesons decays
- Remarks on the f_0(400-1200) scalar meson as the dynamically generated chiral partner of the pion
- Ground-State Scalar Nonet: SU(3) Mass Splittings and Strong, Electromagnetic, and Weak Decay Rates
- Coupling and the structure of
- Identifying the quark content of the isoscalar scalar mesons f_0(980), f_0(1370), and f_0(1500) from weak and electromagnetic processes
- Determination of mixing angle through decays
- decays into and mesons
- Interference effects in the X(4260) signal
- Relating multichannel scattering and production amplitudes in a microscopic OZI-based model
- decays and final state interactions
- Probing new physics in B -> f_0(980) K decays
- The Quark-Level Linear σ Model
- The X(4260) and possible confirmation of psi(3D), psi(5S), psi(4D), psi(6S) and psi(5D) in J/psi pi+ pi-
- Dynamical SU(3) linear sigma model and the mixing of eta'-eta and sigma-f_0 mesons
- Cabibbo-Kobayashi-Maskawa-favored decays to a scalar meson and a meson
- Radiative (phi -> f_0(980) gamma) decay in light cone QCD sum rules
- Comment on Intrinsic and dynamically generated scalar meson states
- Determination of the strangeness contents of light-flavour isoscalars from its production rates in hadronic Z decays measured at LEP
- Investigation of g_f0-rho-gamma and g_a0-rho-gamma coupling constants in light cone sum rules
- Study of some B_s to f_0(980) decays in the fourth generation model