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In physics, a global symmetry is a symmetry that holds at all points in the spacetime under consideration, as opposed to a local symmetry which varies from point to point.
Global symmetries require conservation laws, but not forces, in physics.
An example of a global symmetry is the action of the [math]\displaystyle{ U(1)=e^{i\theta} }[/math] (for [math]\displaystyle{ \theta }[/math] a constant - making it a global transformation) group on the Dirac Lagrangian:
Under this transformation the fermionic field changes as [math]\displaystyle{ \psi\rightarrow e^{i\theta}\psi }[/math] and [math]\displaystyle{ \bar{\psi}\rightarrow e^{-i\theta}\bar{\psi} }[/math][1] and so: