Abstract
Relativistic dispersion relations are used to derive equations for low-energy -, -, and -wave meson-nucleon scattering under the assumption that the (3,3) resonance dominates the dispersion integrals. The -wave equations so obtained differ only slightly from those of the static fixed-source theory. The conclusions of the static theory are re-examined in the light of their new derivation.
- Received 21 February 1957
DOI:https://doi.org/10.1103/PhysRev.106.1337
©1957 American Physical Society