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Disclaimer: I am not a Physicist. So please correct any misunderstanding that I may have.

From what I understand, a $2$-point Green function can be interpreted as the response at $x_2$, when you have a delta function source at point $x_1$. Is there a similar interpretation for $n$-point Green's functions, as in QFT for instance? I know they are defined as vacuum expectation values of a product of $n$-operators, possibly ordered in some way, but I don't understand how to relate the definition, with the much simpler description above.

Can anyone please clear my confusion?

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The $n$-point correlation function has an analogous interpretation to the 2-point correlation function: it gives the probability amplitude ('response') for finding some number $n-p$ of (delta function-shaped) particles at positions $x_{(p+1)}..x_n$, starting from $p$ (delta function-shaped) particles at initial positions $x_1..x_p$.

Here, the number $p$ does not really matter: mathematically, we are only associating some amplitude to a configuration of $n$ delta-function sources, and the split in $p$ and $n-p$ sources is arbitrary.

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  • $\begingroup$ Thinking. This is interesting, and leads me to ask many more questions. But I guess they should be topics of other posts. Some of these questions are: what is a nice general class of linear differential operators for which one can define "propagators"? For which subclass do we have that the propagator is symmetric? Is being symmetric for a propagator a consequence of some symmetry of the differential operators? I guess I should ask, or look for answers before creating new posts. In any case, thank you! $\endgroup$ – Malkoun Sep 20 '18 at 13:48

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