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258 November 7, 2013<br />

10.2 More on symmetry factors<br />

10.2.1 The origin of symmetry factors<br />

In this section we shall return to the ‘simple’ world of zero dimensions, since<br />

symmetry factors do not depend on the dimensionality of the theory. Let us<br />

consider again the ϕ 3/4 theory, with a path integrand<br />

exp ( −S(ϕ) + Jϕ ) (<br />

= exp − µ 2! ϕ2 − λ )<br />

3<br />

∑<br />

(<br />

= e −µϕ2 /2! 1 −λ3 ϕ 3<br />

n<br />

n 3 ! 3!<br />

1,3,4≥0<br />

3! ϕ3 − λ 4<br />

4! ϕ4 + Jϕ<br />

) n3 ( 1 −λ4 ϕ 4<br />

n 4 ! 4!<br />

) n4<br />

1<br />

n 1 !<br />

(<br />

Jϕ<br />

) n1<br />

(10.20)<br />

We see that a diagram with n 3 three-vertices, n 4 four-vertices and n 1 source<br />

vertices carries an a priori factor of<br />

1<br />

n 1 ! n 3 ! n 4 ! (3!) n3 (4!) n4 .<br />

10.2.2 Explicit computation of symmetry factors

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