1. Investigation of near-threshold eta-meson production in the reaction π − p→ ηn
- Author
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D. E. Bayadilov, N. G. Kozlenko, E. A. Filimonov, Yu. A. Beloglazov, A. A. Kulbardis, S. P. Kruglov, V. V. Sumachev, D. V. Novinskiy, A. V. Shvedchikov, A. K. Radkov, I. V. Lopatin, and A. B. Gridnev
- Subjects
Physics ,Nuclear and High Energy Physics ,Meson ,Branching fraction ,Nuclear Theory ,Eta meson ,Hadron ,Resonance (particle physics) ,Atomic and Molecular Physics, and Optics ,Nuclear physics ,Particle decay ,Pion ,High Energy Physics::Experiment ,Atomic physics ,Nuclear Experiment ,Nucleon - Abstract
Differential and total cross sections for eta-meson production in the reaction π−p → ηn were measured within the experimental program eta-meson physics implemented in the pion channel of the synchrocyclotron of the Petersburg Nuclear Physics Institute (PNPI, Gatchina). These measurements were performed at incident-pion momenta (700, 710, 720, and 730 MeV/c) in the vicinity of the threshold for the process under study by using the neutral-meson spectrometer designed and created at the Meson Physics Laboratory of PNPI. It is shown that, in the immediate vicinity of the threshold (685 MeV/c), the process of eta-meson production proceeds predominantly via S11(1535)-resonance formation followed by the decay S11(1535) → ηn (the respective branching fraction is Br ≈ 60%), but that, as the momentum of incident pions increases, the role of the D wave becomes ever more important. A detailed analysis of this effect indicates that it is due to the increasing contribution of the D13(1520) resonance. Although the branching fraction of the decay of this resonance through the ηn channel is assumed to be very small (BR ≈ 0.24%), the effect is enhanced owing to the interference between the D wave and the dominant resonance S11(1535).
- Published
- 2012