Don't forget that the polarization tensors depend on the gauge choice via reference vectors (call them q, q′) Now you have to check what happen when you chance the reference vectors from q,q′ to some new vectors r,r′. The change of the vectors will lead to the new polarization vectors aquire a term proportional to its momentum p.
ϵ(p,r)μ∼ϵ(p,q)μ+pμ
The contraction of the last term with Mμν vanishes, i.e. you have shown gauge invariance.
Do you also have to show that Mμν contracted into one of its momenta vanishes?
This post imported from StackExchange Physics at 2014-04-15 16:46 (UCT), posted by SE-user A friendly helper