# Is there a way to compute (trivalent) Feynman integrals inductively from smaller diagrams?

Suppose that I would like to compute the Feynman integral associated to the trivalent graph

One can argue that this diagram comes from two copies of the smaller diagram

glued together at the external vertices.

We could argue even further that it really comes from two copies of the following diagram

where we instead cut one of the edges on each diagram, yielding the second, and then gluing them together.

Suppose that I know how to compute the integral associated to either this second (or preferably third) diagram. Is there some sort of algorithm for reducing the integral of the first diagram to some combination of integrals for the second and third diagrams?

I should remark perhaps that I am being deliberately vague about what the context of this computation is. I'm mostly hoping that there is some formal way to combine the smaller integrals to produce the larger ones, something that would look like, say, a multiplicative structure on an $R$-algebra freely generated by diagrams, for some ring $R$. Or something like that.

Edit: I feel that I should note that one hope that I have (which may prove ill-founded) is that this will in some sense be computable in a manner akin to the gluing or other type formulae in Gromov-Witten theory. It'd be really nice if we could write something like $$I_{\Gamma_g} = \sum_{g_1+g_2 = g} C_{g_1,g_2} I_{\Gamma_{g_1}}I_{\Gamma_{g_2}}$$ or something.

• It is not possible to compute integrals recursively like that. Otherwise there would not be yearly conference about computing feynman integrals. There are however, properties which recurse with the topology of the graph. Apr 24, 2023 at 22:32

I'm not sure of the level at which you're looking for answers. Two avenues (which are continuing to be researched actively) to check out:

1. Work on amplitudes by Zvi Bern and co, starting in the 90s.
2. BCFW recursion relations for gauge theory amplitudes recursively generate all diagrams from 3 point amplitudes.

In general, if a theory "fundamentally" has a 4-valent vertex, it is not clear if one could break all Feynman diagrams into 3-point amplitudes. However, in some interesting classes of theories, one can.

Generally useful resources on progress in amplitude techniques:

You might want to read up on the optical theorem and unitarity cuts.

• My theory should not have a 4-valent vertex, since it is coming from a cubic action. Apr 29, 2014 at 17:36
• For the diagrams you've drawn, sure. Fwiw, I tried to keep my comments fairly general.
– Siva
Apr 29, 2014 at 19:39
• I've downloaded the two references you suggested; I'll take a look through them. Thanks! Apr 30, 2014 at 2:32