Polarizations of vector/tensor fields

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SUMMARY

The discussion focuses on the polarization states of vector and tensor fields, specifically in the context of quantum field theory (QFT). Vector fields possess 4 polarizations, which reduce to 3 when gauge conditions are applied and further to 2 for massless fields. Tensor fields, such as those representing linearized gravitons, have 10 polarizations, which reduce to 6 under gauge conditions and to 3 for massless fields. The consensus is that when summing over polarizations in the field operator, one typically sums over all 4 polarizations for vector fields and all 10 for tensor fields, particularly for internal lines in Feynman diagrams.

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michael879
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ok this is a really simple question but I've spent 30 minutes searching and can't find a definitive answer. I'm working with a tensor field right now (linearized graviton) and I'm trying to generalize all the vector field stuff to it. One thing I'm confused about is the polarization states.

I understand that vector fields have 4 polarizations, and (symmetric) tensor fields have 10.
Setting the gauge reduces this to 3 and 6
Setting the fields massless reduces this to 2 and 3

My question is in the field operator, which polarization states do you sum over? Is it 3 or 4 for vector fields, and is it 6 or 10 for tensor fields? I understand why its not 2 and 3 respectively, but my QFT book sums over 4 photon polarizations in the definition of A and I just can't understand why.
 
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Setting the fields massless reduces this to 2 and 3
Actually, the number of polarizations is reduced to 2 and 2. Free massless fields always have two helicity states. For gravity after imposing the covariant gauge condition (four conditions) the remaining freedom is ◻ξμ = 0 (four more conditions).
which polarization states do you sum over?
Answer depends on which framework you're using, but in the usual approach the gauge condition is imposed only on the mass shell (external lines only) and internal lines are summed over all 4 (or 10) polarizations.
 

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