consider an observable, say the Hamiltonian,and the symmetry group of it, with accidental degeneracy excluded. now decompose the state space into the direct sum of eigenspaces, namely each spanned by the set of eigenvectors with the same eigenvalue.
It is often stated (e.g. A. Zee, "group in a nut", p. 163-164), that such an eigenspace is an irrep. I understand it is necessarily a representation of the group, but why it is an irrep? Also is the converse true that an irrep of the group is necessarily such an eigenspace?
To clarify the question, consider the hamiltonian of a system which has only one symmetry, $SO(3)$. then it is stated that each of the subspaces of the state space spanned by eigenvectors with the same energy eigenvalue and total angular momentum forms an irrep.