I am not sure what you mean.
The charges are the q.m. generators of the gauge group. Look at a simple example, the n-dim. harmonic oscillator with
a_i;\;i=1\ldotsN
[T^a, T^b] = if^{abc}T^c
If you define the charges (in an SU(N) gauge theory you can derive them from the Noether theorem instead of introducing them by hand)
Q^a = a^\dagger_i (T^a)_{ik} a_k
you can check easily that they generate the same algebra.
[Q^a, Q^b] = if^{abc}Q^c
Therefore you can classify all states according to the su(N) algebra and all equations that are valid on the algebraic level carry over to the q.m. states.
Quantum gauge theory gives you additional equations, e.g. the requirements that in an unbroken SU(N) gauge theory all physical states are SU(N) singulets, but these constraints are due to additional dynamical considerations and cannot be derived frome purely algebraic reasoning.