Canonical Quantization of Scalar Fields — Mark Srednicki
Physics — QFT · dispersion-relations
Problem
Dispersion relations. Consider the exact Π(k2), with ε=0. Assume that its only singularity is a branch point at k2=−4m2, that it obeys eq. (15.17), and that Π(k2) grows more slowly than ∣k2∣2 at large ∣k2∣. By recapitulating the analysis in the previous problem, show that
Π′′(k2)=π2∫4m2∞ds(k2+s)3ImΠ(−s−iε).(15.19)
This is a twice subtracted dispersion relation. It gives Π′′(k2) throughout the complex k2 plane in terms of the values of the imaginary part of Π(k2) along the branch cut.