Mechanism of the close-to-threshold production of the eta meson
arXiv:hep-ex/0611015 · doi:10.1103/PhysRevLett.98.122003
Abstract
Measurements of the analysing power for the p(pol)p --> ppeta reaction have been performed in the close-to-threshold energy region at beam momenta of p_{beam}=2.010 and 2.085 GeV/c, corresponding to excess energies of Q=10 and 36 MeV, respectively. The determined analysing power is essentially consistent with zero implying that the eta meson is produced predominantly in the s-wave at both excess energies. The angular dependence of the analysing power, combined with the hitherto determined isospin dependence of the total cross section for the eta meson production in nucleon-nucleon collisions, reveal a statistically significant indication that the excitation of the nucleon to the S_{11}(1535) resonance, the process which intermediates the production of the eta meson, is predominantly due to the exchange of the pi meson between the colliding nucleons.
4 pages, 4 figures, content added
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Cited by in corpus (19)
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- Interaction of eta mesons with nuclei
- The role of in production
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- Novel detector systems for the Positron Emission Tomography
- Near threshold production of the eta meson via the quasi-free pn --> pn eta reaction
- Coupling Constant for
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- Invariant mass distributions for the pp to p p eta reaction at Q=10 MeV
- Few-body aspects of the near threshold pseudoscalar meson production
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- Near-threshold production in collisions
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- Production and interaction of the eta meson with nucleons and nuclei
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