I'll answer this question by example. Some standard gauge choices are the Rξ gauge and axial gauge with propagators
Δξμν(k)=−ip2−iε[gμν−(1−ξ)kμkνk2]
Δaxialμν(k)=−ip2−iε[gμν−kμkν+(k⋅n)(kμnν+kνnμ)−k2nμnνk2+k⋅n]
The crucial thing is that the
μ,ν indices in the propagator are always contracted with "the rest of the amplitude" which satisfies
kμMμν=0 (in both axial and
Rξ gauges) and
nμMμν=0 (in axial gauge). Thus, the second term always vanishes upon contraction and the only non-zero contribution is the first term, which are the same in both the propagators.
This post imported from StackExchange Physics at 2014-04-13 14:32 (UCT), posted by SE-user Prahar