Normalising a massive propagator?
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Explanation:
The propagator for a gauge boson in a gauge theory depends on the choice of convention to fix the gauge. For the gauge used by Feynman and Stueckelberg, the propagator.
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Answer:
If you take a propagator Greens function for a massless photon from the origin as. G(0,x)=1x2−t2+iεG(0,x)=1x2−t2+iε
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