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Oct 30, 2019 at 10:08 history edited jak CC BY-SA 4.0
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Oct 30, 2019 at 9:44 comment added jak @ohneVal Thanks. If post this comment as an answer I can accept it.
Oct 30, 2019 at 9:21 comment added ohneVal Virtual is usually a term used to describe propagators that are not subject to the on-shell condition, these appear in intermediate states in Feynman diagrams but that's the only difference. One normally calls particles that are on shell, I.e. they follow $E^2-m^2=p^2$, real. So the simple answer is, it is the Feynman propagator plus the on-shell condition, that means integrating four momenta subject to $k_0 = \sqrt{p^2+m^2}$.
Oct 30, 2019 at 8:56 history answered jak CC BY-SA 4.0