Abstract

We extend our recent non-perturbative chiral SU(3) coupled channel approach to pion- and photon-induced η\eta- and KK-meson production off protons by including all strong and electromagnetic p-wave multipoles. We identify the p-wave amplitudes of the next-to-leading order SU(3) chiral meson-baryon Lagrangian with a coupled channel potential which is iterated to infinite orders in a separable Lippmann-Schwinger equation. Our approach to η\eta- and KK-photoproduction introduces no additional free parameters. By adjusting a few finite range parameters and the unknown parameters in the Lagrangian, we are able to simultaneously describe a very large amount of low-energy data. These include the total and differential cross sections of the π\pi-induced reactions πpηn,K0Λ,K0Σ0,K+Σ\pi^- p \to \eta n, K^0 \Lambda, K^0 \Sigma^0, K^+ \Sigma^- and π+pK+Σ+\pi^+ p \to K^+ \Sigma^+ as well as those of photoproduction γpηp,K+Λ,K+Σ0,K0Σ+\gamma p \to \eta p, K^+\Lambda, K^+ \Sigma^0, K^0 \Sigma^+. The polarization observables measured in η\eta- and KK-photoproduction are particularly sensitive to interference terms between the s- and p-wave multipoles. The total cross section data are remarkably well reproduced in all channels. There remain, however, some open questions concerning details of angular distributions and polarization observables.Comment: 20 pages, 5 figures, accepted for publication in Nucl. Phys.

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