The integrals of interest in Physics have the form
If U is a polynomial in the coordinate functions v^{1}, ...v^{d}, then each term in the sum of integrals is a sum of mpoint functions, and can be evaluated by our method, which can be written symbolically as:
Example: This example is formally like the `` theory.'' We take and analyze
Let us compute the terms of degree 2 in .
These terms will involve 6 derivatives; their sum is:
By Wick's Theorem we can rewrite this sum as
These pairings can also be represented by graphs, very much in the same way that we used for mpoint functions: there will be one trivalent vertex for each u factor, and one edge for each A^{1}. In this case there will be exactly two distinct graphs, according as the number of (unprimed, primed) index pairs is 1 or 3.
Summing over all possible labellings of these graphs will give some duplication, since each graph has symmetries that make different labellings correspond to the same pairing.
All six of these labelings, and their six leftright mirror images,
correspond to the same product:
u_{123} u_{456} A^{1}_{14} A^{1}_{25} A^{1}_{36}.
Keeping this in mind, we may rewrite the coefficient of as:
In general, the ``Feynman rules'' for computing the coefficient of in the expansion of Z_{U} are stated in exactly this way, except that the sum is over trivalent graphs with 2n vertices (and 3n edges).

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