TheoremComplete

Schur's Lemma

Schur's Lemma is one of the most fundamental results in representation theory, providing crucial information about morphisms between irreducible representations and the structure of endomorphism algebras.

TheoremSchur's Lemma (Basic Form)

Let VV and WW be irreducible representations of a group GG over an algebraically closed field F\mathbb{F}.

  1. Distinctness: If VV and WW are non-isomorphic, then HomG(V,W)={0}\text{Hom}_G(V, W) = \{0\}
  2. Self-maps: If V=WV = W, then every intertwining map ϕ:VV\phi: V \to V is a scalar multiple of the identity: EndG(V)=FidV\text{End}_G(V) = \mathbb{F} \cdot \text{id}_V

In other words, HomG(V,W){Fif VW0otherwise\text{Hom}_G(V, W) \cong \begin{cases} \mathbb{F} & \text{if } V \cong W \\ 0 & \text{otherwise} \end{cases}

Proof sketch: For (1), if ϕ:VW\phi: V \to W is a non-zero morphism, then ker(ϕ)\ker(\phi) and im(ϕ)\text{im}(\phi) are subrepresentations. By irreducibility of VV and WW, we have ker(ϕ)={0}\ker(\phi) = \{0\} and im(ϕ)=W\text{im}(\phi) = W, so ϕ\phi is an isomorphism.

For (2), let ϕ:VV\phi: V \to V be an intertwining map. Since F\mathbb{F} is algebraically closed, ϕ\phi has an eigenvalue λF\lambda \in \mathbb{F}. Then ϕλidV\phi - \lambda \text{id}_V is an intertwining map with non-trivial kernel, hence by irreducibility must be zero. Thus ϕ=λidV\phi = \lambda \text{id}_V.

ExampleApplications

For finite groups over C\mathbb{C}: If χ\chi is the character of an irreducible representation, then: χ,χ=1GgGχ(g)2=1\langle \chi, \chi \rangle = \frac{1}{|G|} \sum_{g \in G} |\chi(g)|^2 = 1

Matrix representations: If ρ:GGLn(C)\rho: G \to GL_n(\mathbb{C}) is irreducible and MM is a matrix commuting with all ρ(g)\rho(g), then M=λInM = \lambda I_n for some λC\lambda \in \mathbb{C}.

Multiplicity formula: In a decomposition V=iVimiV = \bigoplus_i V_i^{\oplus m_i} where ViV_i are distinct irreducibles, the multiplicity mi=dimHomG(Vi,V)m_i = \dim \text{Hom}_G(V_i, V).

Remark

The algebraically closed field assumption in part (2) is essential. Over R\mathbb{R}, the rotation group SO(2)SO(2) has a two-dimensional irreducible representation (rotations of R2\mathbb{R}^2), and rotation by any angle provides a non-scalar endomorphism. However, over C\mathbb{C}, this representation becomes reducible.

TheoremSchur's Lemma (Refined Form)

For finite-dimensional representations over C\mathbb{C}:

If VV is irreducible, then EndG(V)C\text{End}_G(V) \cong \mathbb{C} is a division algebra. If additionally the field is algebraically closed and dimV<\dim V < \infty, then EndG(V)=CidV\text{End}_G(V) = \mathbb{C} \cdot \text{id}_V by the spectral theorem.

For infinite-dimensional representations, EndG(V)\text{End}_G(V) can be a larger division algebra (e.g., quaternions for certain real representations).

Schur's Lemma underlies the orthogonality relations for characters, the decomposition of tensor products, and Frobenius reciprocity. It is the foundation upon which much of the representation theory of finite groups and compact Lie groups is built.