Any self-adjoint operator A∈Hom(E) can be written as Ax=∑aj⟨x,bj⟩bj and AΨ(g)=Ψ(g)A is equivalent to aj⟨Ψ(g)bj,bk⟩=⟨Ψ(g)Abj,bk⟩=⟨Ψ(g)bj,Abk⟩=ak⟨Ψ(g)bj,bk⟩ . By assumption we conclude that for all j,k: aj=ak, i.e. A=1.