# What is the Noether charge associated with the the color $SU(3)$ symmetry of QCD?

A version of the Noether's theorem applies to local gauge symmetries. What is the Noether's charge associated with a non-abelian gauge symmetry such as the color $$SU(3)$$ and how is that derived? I want an expression for the color charge operator like we have an expression for the electric charge operator. Please see Eq. (9) and (11) of the answer here.

The $$\mathrm{SU}(3)$$ gauge symmetry is a local symmetry, and therefore it is not Noether's first, but Noether's second theorem that applies to it, which does not yield conserved quantities.
For $$\mathrm{U}(1)$$ gauge symmetries like the electromagnetic symmetry, there is also a global $$\mathrm{U}(1)$$ symmetry, and hence a conserved quantity. But the global symmetry associated to a non-Abelian gauge symmetry is just the center of the gauge group, which is discrete for $$\mathrm{SU}(3)$$, and hence there is no conserved quantity associated to it. This center symmetry has physical significance e.g. in models of confinement, see this question and its answer.
• @Stephan Note that a non-Abelian gauge transformation acts as $A\mapsto gAg^{-1} + \mathrm{d}g$, so constant transformations that are not in the center still change the gauge field, and are therefore still gauge transformations between physically identical states. In this answer, by "global symmetry" I mean a symmetry that does not change the gauge field and therefore transforms between physically distinct states, since these are the symmetries to which one can meaningfully apply Noether's theorem. – ACuriousMind Oct 20 '18 at 10:58