πN→ηN and ηN→ηN partial-wave T matrices in a coupled, three-channel model

Mijo Batinić, Ivo Šlaus, Alfred Švarc, and B. M. K. Nefkens
Phys. Rev. C 51, 2310 – Published 1 May 1995; Erratum Phys. Rev. C 57, 1004 (1998)
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Abstract

The πN→ηN and ηN→ηN partial-wave T matrices for the eight lowest partial waves have been obtained in a three-coupled-channel model with unitarity manifestly imposed. The two physical channels are πN and ηN, and the third channel, ππN is an effective, but unphysical two-body channel which represents all remaining processes. The πN elastic phase shifts and the weighted data base of the πN→ηN total and differential cross sections are chosen as the input for the fitting procedure. A model containing a single resonance in each of the three partial waves that dominates the η production at lower energies is compared with previous analyses, based on similar assumptions. A multiresonance coupled-channel model is introduced which significantly improves the agreement with all input data. Our results are compared with a complementary multiresonance coupled-channel analysis that is constrained with elastic and continuum production channels. The inclusion of the fourth P11 resonance in the 1440–2200 MeV region further improves the agreement between the analysis and the data.

  • Received 12 August 1994

DOI:https://doi.org/10.1103/PhysRevC.51.2310

©1995 American Physical Society

Erratum

Erratum: πNηN and ηNηN partial-wave T matrices in a coupled, three-channel model [Phys. Rev. C 51, 2310 (1995)]

M. Batinić, I. Šlaus, A. Švarc, and B. M. K. Nefkens
Phys. Rev. C 57, 1004 (1998)

Authors & Affiliations

Mijo Batinić, Ivo Šlaus, and Alfred Švarc

  • Rudjer Bošković Institute, 41001 Zagreb, Croatia

B. M. K. Nefkens

  • University of California Los Angeles, Los Angeles, California 90024

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Issue

Vol. 51, Iss. 5 — May 1995

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