Abstract
Renormalization prescriptions are given for the covariant integral equations of meson-nucleon scattering, taking into account the difficulties of overlapping divergences. The covariant wave equations, corresponding to the iteration of second-order irreducible processes, are solved approximately and renormalized in closed form (in the case of the pseudoscalar theory with pseudoscalar coupling). The S-phase shifts corresponding to the states of isotopic spin ½ and 32 are computed, and their variation with energy is compared with experiment. The only parameter which can be adjusted is the meson-nucleon coupling constant G. It is found that a good agreement with experiment is obtained when G24π=7.5. The possibility of this agreement being purely coincidental cannot be ruled out, but other interpretations of this result are discussed.