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.
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1For local symmetries, one uses Noether's second theorem, while Noether's first theorem is for global symmetries, cf. https://physics.stackexchange.com/a/13881/2451 , https://physics.stackexchange.com/q/66092/2451 and links therein. – Qmechanic Sep 26 '18 at 15:46
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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.

ACuriousMind
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Could you please elaborate on the global symmetry associated to a gauge symmetry? (e.g. what it is, how to find it, does it always exist..) – ersbygre1 Oct 19 '18 at 03:11
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2@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
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1That makes sense, thank you! So for the case of U(1), the center of the group coincides with the group itself, so that's why we have the additional U(1)? – ersbygre1 Oct 20 '18 at 12:36