Let GG be a group, let kk be an algebraically closed field (e.g. k=Ck=\mathbb C), and let

ρ:GGL(V)\rho: G \to \mathrm{GL}(V)

be a finite-dimensional .

Corollary of Schur's lemma

If zz lies in the Z(G)Z(G), then ρ(z)\rho(z) is a scalar operator:

ρ(z)  =  λzIdVfor some λzk.\rho(z) \;=\; \lambda_z\,\mathrm{Id}_V \quad \text{for some }\lambda_z\in k.

More generally, if aa lies in the center Z(k[G])Z(k[G]) of the , then the kk-linear operator “action by aa” on VV commutes with ρ(G)\rho(G) and hence is also scalar on VV.

Consequence: abelian groups have only 11-dimensional irreps

If GG is , then every gGg\in G is central, so every ρ(g)\rho(g) is scalar. If dim(V)>1\dim(V)>1, every line in VV would be GG-stable, contradicting irreducibility. Hence any irreducible representation of an abelian group over kk has dim(V)=1\dim(V)=1.

Examples
  1. CnC_n. Since CnC_n is abelian, every irreducible complex representation is 11-dimensional. Concretely, if Cn=gC_n=\langle g\rangle and ζ=e2πi/n\zeta=e^{2\pi i/n}, the irreducibles are the characters
    χj(g)=ζj(j=0,1,,n1).\chi_j(g)=\zeta^j \qquad (j=0,1,\dots,n-1).
  1. D8D_8 (order 88). For the dihedral group of the square, the center is Z(D8)={1,r2}Z(D_8)=\{1,r^2\} where rr is rotation by 9090^\circ. In the 22-dimensional “geometric” irreducible representation on C2\mathbb C^2, r2r^2 acts as rotation by 180180^\circ, i.e.
    ρ(r2)=I,\rho(r^2) = -I,
    a scalar operator. In every 11-dimensional representation, ρ(r2)=+1\rho(r^2)=+1 (also a scalar, necessarily).
  1. S3S_3. Z(S3)={e}Z(S_3)=\{e\} is trivial, so the corollary imposes no nontrivial scalar constraints—consistent with the existence of a 22-dimensional irreducible representation.