Starting with current commutation relations and the hypothesis of partial conservation of the axial-vector current, relations are obtained for the pion-nucleon scattering amplitude considered to the second order in the energy variable ν. The structure-dependent contributions to the second-order terms in the matrix element involving the axial-vector currents are approximated by the direct and exchanged poles and resonances, particularly the N* resonances with spins {} and 3/2. The contribution of the ρ meson to this matrix element is estimated to be small. Expressions are obtained for the P-wave scattering lengths and the S-wave and P-wave phase shifts at low energies. Numerical estimates are made for these and are compared with the available data; it is found that resonable agreement with experiment can be obtained except for the P-wave scattering length a_1-^(-) and the partial-wave amplitude f_1-^(-). Some questions relating to the off-mass-shell extrapolation are discussed. We have also examined the validity of the assumption made, in the usual derivation of the relations for the S-wave scattering lengths, that the terms of higher order in ν may be neglected. We suggest that at least for the isospin-symmetric scattering length this is not a good approximation, so that this scattering length cannot be obtained adequately by using only the current commutation relations and the hypothesis of a partially conserved axial-vector current. The scalar term arising from the commutator [a⁰(x), φ(y)] is estimated; we suggest that the contribution of this term is important and cannot be ignored.
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Kalaivani Raman (1967) studied this question.
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