Abstract
Theoretical values for D(ω) in the theory of pion dispersion relations have been recalculated with a suitable modification of the experimental values for σtot. This modification is supported by the results obtained from a recent phase-shift analysis. Agreement with the experimental values for D(ω) is achieved for pion kinetic energies ≲220 Mev. It may be concluded that the theoretical values for D(ω) have a strong dependence on the detailed shape of the peak of σtot near the resonance.