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REPTHEORY · 1

Representations

4 concepts · 22 questions

Representations as homomorphisms to GL(V), examples (trivial, sign, permutation, regular, dihedral), G-homomorphisms, invariant subspaces, irreducibility, equivalence and direct sums.

Definition 1.1Representation

A (complex) representation of GG is a homomorphism ρ:G→GL(V)\rho : G\to GL(V) with VV a finite-dimensional complex vector space; dim⁡V\dim V is its degree. Choosing a basis gives matrices ρ(g)∈GLn(C)\rho(g)\in GL_n(\mathbb{C}) with ρ(gh)=ρ(g)ρ(h)\rho(gh) = \rho(g)\rho(h). Equivalently, GG acts on VV by linear maps. Examples: trivial ρ(g)=1\rho(g) = 1; sign of SnS_n; permutation representation of SnS_n on Cn\mathbb{C}^n by permuting coordinates; regular representation on CG\mathbb{C}G (basis ehe_h, g⋅eh=eghg\cdot e_h = e_{gh}); Cn=⟨g⟩C_n = \langle g\rangle with ρ(g)=e2πik/n\rho(g) = e^{2\pi ik/n}.

Representation: realise the group as matrices; each element becomes an invertible linear map, compatibly with multiplication.

Why: turns group theory into linear algebra, where we have traces, eigenvalues and dimensions.

Tiny example: D8D_8 acting on R2\mathbb{R}^2 by the rotations and reflections of a square.

Definition 1.2Subrepresentations, irreducibility and equivalence

A subspace W≤VW\le V is GG-invariant if ρ(g)W⊆W\rho(g)W\subseteq W for all gg; it is then a subrepresentation. VV is irreducible if V≠0V\ne0 and its only invariant subspaces are 00 and VV. V⊕WV\oplus W is a representation via block-diagonal matrices. Representations ρ,ρ′\rho, \rho' are equivalent (≅\cong) if ρ′(g)=Tρ(g)T−1\rho'(g) = T\rho(g)T^{-1} for a fixed invertible TT (a change of basis intertwining them). Example: in the permutation representation of SnS_n, the line ⟨(1,…,1)⟩\langle(1, \dots, 1)\rangle and the hyperplane {∑xi=0}\{\sum x_i = 0\} are invariant.

Invariant subspace: every group element maps it into itself (as for invariant subspaces in Linear Algebra II, but for a whole group at once).

Irreducible: no proper non-zero invariant subspace; the "atoms" of representation theory.

Permutation rep of SnS_n = trivial line ⊕ (n−1)(n - 1)-dimensional "standard" representation.

Example 1.3The dihedral representation

D2n=⟨r,s∣rn=s2=e,srs−1=r−1⟩D_{2n} = \langle r, s\mid r^n = s^2 = e, srs^{-1} = r^{-1}\rangle acts on C2\mathbb{C}^2 by

ρ(r)=(cos⁡2πn−sin⁡2πnsin⁡2πncos⁡2πn),ρ(s)=(100−1).\rho(r) = \begin{pmatrix}\cos\frac{2\pi}n & -\sin\frac{2\pi}n\\ \sin\frac{2\pi}n & \cos\frac{2\pi}n\end{pmatrix},\qquad\rho(s) = \begin{pmatrix}1 & 0\\ 0 & -1\end{pmatrix}.

For n≥3n\ge3 it is irreducible: an invariant line would be an eigenline of ρ(r)\rho(r), whose eigenvectors (1,∓i)(1, \mp i) are swapped by ρ(s)\rho(s).

D2nD_{2n} on the plane: rotation by 2πn\frac{2\pi}n and a reflection; irreducible for n≥3n\ge3.

Lemma 1.4G-homomorphisms

A GG-homomorphism ϕ:V→W\phi : V\to W is a linear map with ϕρV(g)=ρW(g)ϕ\phi\rho_V(g) = \rho_W(g)\phi for all gg. Its kernel is a subrepresentation of VV and its image a subrepresentation of WW; an invertible GG-homomorphism is exactly an equivalence. Hom⁡G(V,W)\operatorname{Hom}_G(V, W) is a vector space.

Equivariant maps have invariant kernels and images; invertible ones are equivalences.

Proof