As far as I know, absorbing of the positive coefficient of iϵ in a propagator seems to be a trivial operation without even the need of justification.
In Peskin page 286, he did this:
k0→k0(1+iϵ)
(k2−m2)→(k2−m2+iϵ)
In M. Srednicki's Quantum Field Theory, page 51,
The factor in large parentheses is equal to E2−ω2+i(E2+ω2)ϵ, and we can absorb the positive coefficient in to ϵ to get E2−ω2+iϵ.
Why and does this kind of manipulation affect the final result of calculation?
Although 1k2−m2+iϵk2−1k2−m2+iϵ is infinitesimal, but the integration of such terms may lead to divergences, and this is my worry.
Also the presence of k0 in the coefficient of iϵ could potentially influence the poles of an integrand and consequently influence the validity of Wick Rotation.
This post imported from StackExchange Physics at 2014-05-04 11:30 (UCT), posted by SE-user LYg