Global U(1) symmetry
= Global U(1) symmetry
A <global phase symmetry> sends a complex field to $e^{i\alpha}\phi$ with the same constant real $\alpha$ everywhere. It is distinct from allowing a spacetime-dependent phase together with a compensating gauge-field transformation. A <global phase symmetry> can produce a conserved <Noether current> and, in an appropriate ordered mean-field state, a continuum of degenerate phase choices.