Math 202B: Lecture 22

Let \mathbf{Rep}(G) be the category of finite-dimensional unitary representations of a finite group G. As we discussed last week, \mathbf{Rep}(G) is both “bigger” and “smaller” than the category \mathbf{FHil} of finite-dimensional Hilbert spaces. What this means is that the same Hilbert space V may appear in \mathbf{Rep}(G) as two distinct representations (V,\varphi) and (V,\varphi'), but at the same time hom-spaces in \mathbf{Rep}(G) may be smaller because, unlike \mathrm{Hom}(V,W), linear maps in \mathrm{Hom}_G(V,W) must intertwine the actions \varphi and \psi of two unitary representations (V,\varphi) and (W,\psi). In fact, we have already made this “smaller” feature quantitative by deriving the dimension formula

\dim \mathrm{Hom}_G(V,W) = \frac{1}{|G|} \langle \chi^V,\chi^W\rangle.

In this lecture we will compare \mathrm{Hom}(V,W) and \mathrm{Hom}_G(V,W) structurally as opposed to numerically.

One of the simplest things we can say about a linear map T \in \mathrm{Hom}(V,W) is that its kernel and image are subspaces of V and W, respectively. It is therefore natural to hope that a G-equivariant linear map T \in \mathrm{Hom}_G(V,W) would have kernel and image that are “subrepresentations” of V and W, respectively. To make sense of this we first need to define subobjects in \mathbf{Rep}(G).

Definition 22.1. Let (V,\varphi) be a unitary representation of G, and let W be a vector subspace of V. We say that W is G-stable if \varphi(g)w \in W for all g \in G and w \in W.

Problem 22.1. Prove that if T \in \mathrm{Hom}_G(V,W) then \mathrm{Ker}(T) is a G-stable subspace of V and \mathrm{Im}(T) is a G-stable subspace of W.

The only reason that the above is not our definition of “subrepresentation” is that we require representations to be nonzero.

Definition 22.2. A subrepresentation of (V,\varphi) is a nonzero G-stable subspace W \leq V. In particular, (W,\varphi) is a unitary representation of G in its own right provided we restrict each \varphi(g) to W.

Now let us recall the main structure theorem we have for linear maps between finite-dimensional vector spaces, which was the main result of Math 202A.

Theorem (SVD): For any linear map T \in \mathrm{Hom}(V,W) between finite-dimensional Hilbert spaces, there exist distinct positive numbers \sigma_1> \dots > \sigma_r > 0 and nonzero pairwise orthogonal subspaces V_1,\dots,V_r and W_1,\dots,W_r of V and W such that

V = V_1 \oplus \dots \oplus V_r \oplus \mathrm{Ker}(T) \quad\text{and}\quad W=W_1 \oplus \dots \oplus W_r \oplus \mathrm{Im}(T)^\perp

and the restriction of T to V_i has the form T=\sigma_iU_i with U_i \in \mathrm{Hom}(V_i,W_i) an isometric isomorphism.

It is an under-appreciated fact that the SVD holds in \mathbf{Rep}(G) in a very natural way.

Theorem 22.3 (G-equivariant SVD). Let (V,\varphi) and (W,\psi) be unitary representations of G and let T \in \mathrm{Hom}_G(V,W) be a G-equivariant linear map. Then, the left singular spaces V_1,\dots,V_r of T are subrepresentations of V, the right singular spaces W_1,\dots,W_r are subrepresentations of W, and the restriction of T to V_i is an isomorphism in \mathrm{Hom}_G(V_i,W_i). Moreover, the map U_i = \sigma_iT_i|_{V_i} is an isometric isomorphism in \mathrm{Hom}(V_i,W_i).

In \mathbf{FHil}, a space V whose only subspace is V is necessarily one-dimensional. In \mathbf{Rep}(G), the situation is not as simple.

Definition 22.1. A unitary representation (V,\varphi) of G is said to be irreducible if the only subrepresentation it contains is (V,\varphi) itself.

Let \mathbf{Irr}(G) be the full subcategory of \mathbf{Rep}(G) whose objects are irreducible representations. The hom-spaces in this category are highly restricted.

Theorem 22.4 (Schur’s Lemma). If (V,\varphi) and (W,\psi) are irreducible unitary representations of G, then any nonzero map T \in \mathrm{Hom}_G(V,W) is an isomorphism.

Problem 22.2. Prove Schur’s Lemma (it follows directly from the $latex $G-equivariant SVD).$

Another way to state Schur’s Lemma is that if (V,\varphi) and (W,\psi) are irreducible representations which are not isomorphic, then

\mathrm{Hom}_G(V,W) = \{0_{\mathrm{Hom}(V,W)}\}.

Together with our dimension formula for \mathrm{Hom}_G(V,W), this yields the following.

Corollary 22.5. The characters of two non-isomorphic irreducible unitary representations (V,\varphi) and (W,\psi) are orthogonal: we have \langle \chi^V,\chi^W\rangle=0.

Problem 22.3. Prove that the character of any unitary representation (V,\varphi) of G is a class function on G. Prove that the characters of any two isomorphic representations are equal. Combining these facts, deduce an upper bound on the number of isomorphism classes of irreducible unitary representations of G.

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