Pion nucleon scattering up to 600 MeV laboratory kinetic energy is described by a manifestly covariant wave equation in which the pion is restricted to its mass shell. The kernel of the equation includes nucleon (N), Roper (N*), delta ({Δ}), and D₁₃ poles, with their corresponding crossed pole terms approximated by contact interactions, and contact {σ}- and {ρ}-like exchange terms. The {π}NN vertex is treated as a mixture of γ⁵ and γ^μ{{γ}}⁵$ coupling, with a mixing parameter {λ} chosen so that the dressed nucleon pole will be unshifted by the interaction. Chiral symmetry is maintained at threshold. The resonance contributions are fully unitarized by the equation, with their widths determined by the dynamics included in the model. The {Δ} and D₁₃ are treated as pure spin 3/2 particles, with no spin 1/2 amplitude in the S channel. The complete development of this model, which gives a very good fit to all the data up to 600 MeV, is presented.
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Gross et al. (1993) studied this question.
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