Schur's lemma

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This fact is related to: linear representation theory
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Statement

Here, G is a group and k is a field. In the abstract formulation, V1,V2 are vector spaces over k.

Statement no. Condition Conclusion in abstract formulation for vector spaces: ρ1:GGL(V1),ρ2:GGL(V2) are linear representations of G over a field k. f:V1V2 is a homomorphism from ρ1 to ρ2. Conclusion in concrete matrix formulation: ρ1:GGL(m,k), ρ2:GGL(n,k) are representations. FMatn×m is a homomorphism of representations
1 ρ1 is irreducible f is either the zero map or is injective F is either the zero matrix or has full column rank, and nm
2 ρ2 is irreducible f is either the zero map or is surjective F is either the zero matrix or has full row rank, and mn
3 ρ1,ρ2 are both irreducible f is either the zero map or is bijective and hence an isomorphism of representations F is either the zero matrix or is invertible, and m=n
4 ρ1=ρ2, it is irreducible, and k is an algebraically closed field f is a scalar multiplication map F is a scalar matrix and m=n

Applications

Proof

Verbal proof

  1. For this, we use the fact that the kernel of any homomorphism of representations is an invariant subspace. If ρ1 is irreducible, the kernel is either the whole of V1 (in which case we have the zero map) or the zero subspace (in which case we have an injective map).
  2. For this, we use the fact that the image of any homomorphism of representations is an invariant subspace. If ρ2 is irreducible, the image is either the whole of V2 (in which case we have a surjective map) or the zero subspace (in which case we have the zero map).
  3. This follows from the previous two parts.
  4. Any homomorphism from a representation on that field to itself can be represented by a linear operator from the vector space to itself. This linear operator must have an eigenvalue, because the field is algebraically closed. Subtracting that eigenvalue times the identity matrix, we now get a linear operator that has zero as an eigenvalue, which is also a homomorphism of representations. But part (3) tells us that any homomorphism of representations is either the zero map or an isomorphism. An isomorphism cannot have zero as an eigenvalue (since it is an invertible linear operator) and hence the new linear operator we get must be the zero map. Thus the original linear operator must have been a scalar times the identity.