Consider the annihilation of a neutron by an anti-neutron $$ n\overline{n} \rightarrow \pi^0 \pi^0 $$ so that the initial relative angular momentum is zero. Because the spin of neutrons is $1/2$, $J_i$ can take the values $0, 1$.
Now, in pions the spin is zero, so any angular momentum in the rhs should be in the form of $L_f$, which can only take (by conservation of total momentum) the values $0$ or $1$. By some sort of symmetry on bosons wavefunctions, it can be seen that $L_f = 0$, but I don't see why this is the case. Can you shed some light into it?