Consider the Noether current jμ for the U(1) symmetry of eq. (32.1), and the corresponding charge Q.
a) Show that e−iαQφe+iαQ=e+iαφ.
b) Use eq. (32.5) to show that e−iαQ∣θ⟩=∣θ+α⟩.
c) Show that Q∣0⟩=0; that is, the charge does not annihilate the θ=0 vacuum. Contrast this with the case of an unbroken symmetry.