While studying C-symmetry, a question about neutral pion decay came up.
The most probable channels in which neutral pion $\pi^0$ decays are:
- $\pi^0\longrightarrow\gamma+\gamma$ (98%)
- $\pi^0\longrightarrow\gamma+e^{+}+e^{-}$ (1.3%)
that are permitted as C-symmetry is conserved ($C_{\pi^0}=+1$).
The process
$$\pi^0\longrightarrow\gamma+\gamma+\gamma$$
is forbidden, as $C_\gamma\gamma\gamma=-1$.
Can anyone explain me how does the hypothetic forbidden process arise from theory (i.e. from Feynman Diagrams)?
The book says that if I study the rate
$$R={{\Gamma(\pi^0\rightarrow3\gamma)}\over{\Gamma(\pi^0\rightarrow2\gamma)}}$$
I expect that it is of the order $\alpha \approx {1\over137}$, while it is actually smaller (being a C-symmetry violating process). Why should I expect the rate to be $\alpha$?
Best Answer
Roughly: in a Feynman diagram each vertex of a gamma comes with an alpha factor. If three gammas were allowed from CP( which they are not) there would be 3 alpha factors in the nominator, and two in the denominator, so the ratio would be alpha.