I know for a (free) complex scalar field $\psi$ the Lagrangian is: $$ \mathcal{L} = \partial^\mu \psi^\ast\partial_\mu \psi$$ and that Noether's theorem from the $U(1)$ symmetry of the system gives a conserved current $j_\mu \propto iq(\psi\partial_\mu\psi^\ast-\psi^\ast\partial_\mu\psi)$, which can be interpreted as the difference of the number of particles and anti-particles and hence as the conservation of electrical charge.
For real scalar field, though, I would have: $$ \mathcal{L} = \partial^\mu \phi\partial_\mu \phi$$ so there is not $U(1)$ symmtry... but I still expect particle number to be conserved? Shouldn't particle number be the conserved charge?