Observation of the phi to pi+pi-pi+pi- Decay
arXiv:hep-ex/0008019 · doi:10.1016/S0370-2693(00)01001-7
Abstract
Using 11.6 pb^{-1} of data collected in the energy range 0.984--1.06 GeV by CMD-2 at VEPP-2M, the cross section of the reaction e+e- to pi+pi-pi+pi- has been studied. For the first time an interference pattern was observed in the energy dependence of the cross section near the phi meson. The branching ratio of the phi to pi+pi-pi+pi- decay double suppressed by the G-parity and OZI rule is measured Br(phi to pi+pi-pi+pi-) = (3.93 +- 1.74 +- 2.14) \cdot 10^{-6}. The upper limits have been placed for the decays phi to pi+pi-pi+pi-pi0 and phi to eta pi+pi- Br(phi to pi+pi-pi+pi-pi0) < 4.6 \cdot 10^{-6} 90% CL, Br(phi to eta pi+pi-) < 1.8 \cdot 10^{-5} 90% CL.
arXiv comment17 pages, 5 figures
References in corpus (5)
Cited by in corpus (19)
- The states: experimental and theoretical status and perspectives
- Glueballs, Hybrids, Multiquarks. Experimental facts versus QCD inspired concepts
- Predictions for g-2 of the muon and alpha_QED(M_Z^2)
- Present Status of Inclusive Rare B Decays
- First observation of the decay
- Search for D+(s) to pi+ mu+ mu- and D+(s) to pi- mu+ mu+ decays
- Measurement of the meson lifetime using decays
- Measurement of associated production of a W boson and a charm quark in proton-proton collisions at 13 TeV
- Initial-State Radiation Measurement of the e+e- -> pi+pi-pi+pi- Cross Section
- Observation of the decay
- Charm Production and QCD Analysis at HERA and LHC
- Evidence for the decay
- Study of the Process IN THE C.M. Energy Range 920--1060 MeV with the CMD-3 Detector
- Observation of the phi to eta' gamma decay with four charged particles and photons in the final state
- Forward-backward Asymmetry and Branching Ratio of $B \rar K_1 \ell^+ \ell^-$ Transition in Supersymmetric Models
- The decays omega(782), phi(1020) to 5 pi in the hidden local symmetry approach
- Study of the decay with the perturbative QCD approach
- CMD-2 and SND results on the rho, omega and phi
- Understanding and its decays in the extended Friedrichs scheme