- #1
gobbles
- 17
- 1
Homework Statement
Why does the symmetry ##\phi\rightarrow-\phi## mean that an amplitude can be written as
##\alpha + \beta p^2 + \gamma p^4 + ...##
without the odd terms in ##p##?
Homework Equations
I understand that, due to this symmetry, any diagram in ##\phi^4## has an even number of external legs, because otherwise the correlation function of the external fields is zero. So any diagram can be written in the form
##V(p^2)\left(\frac{i}{p^2-m^2}\right)^{n}##
where ##n## is even and ##V(p^2)## is the expression for the amplitude without the external legs. Expanding ##V(p^2)## in ##p## will, of course, give only even powers of ##p##, as will the expansion of ##\left(\frac{i}{p^2-m^2}\right)^n##, but that is true also for ##n## odd, corresponding to an odd number of external legs. So where does this symmetry play a role here?
The Attempt at a Solution
Outlined in (2).