1.3. Lecture 3

One of the main goals of representation theory is to classify all the irreducible representations of a group GG (or more correctly, the isomorphism classes of irreducible representations). This entails producing a list of representations of GG and showing that

  1. (i)

    any irreducible representation of GG is isomorphic to some entry of the list, and

  2. (ii)

    there are no redundancies in the list, i.e all entries are non-isomorphic.

1.3.1. Example: dihedral groups

We list the elements of the dihedral group DnD_{n} as

{rk,srk|k=0,,n1}.\{r^{k},sr^{k}\,|\,k=0,\ldots,n-1\}.

We aim to show that Table 1.1 gives the complete list of irreducible representations of DnD_{n}, for nn odd. We leave the case of nn even as an exercise (there are two more 1-dimensional representations in this case).

Table 1.1. Representations of DnD_{n}.
Dimension ρ(r)\rho(r) ρ(s)\rho(s)
(Id,)(\mathrm{Id},{\mathbb{C}}) 11 11 11
(ϵ,)(\epsilon,{\mathbb{C}}) 11 11 1-1
ρk1k<n/2\underset{1\leq k<n/2}{\rho_{k}} 22 (e2πikn00e2πikn)\left(\begin{smallmatrix}e^{\frac{2\pi ik}{n}}&0\\ 0&e^{\frac{-2\pi ik}{n}}\end{smallmatrix}\right) (0110)\left(\begin{smallmatrix}0&1\\ 1&0\end{smallmatrix}\right)

We start by noting the following:

Proposition 1.3.1.

Let (π,V)(\pi,V) be an irreducible representation of a finite group GG. Then dimπ|G|\operatorname{dim}\pi\leq|G|; in particular, VV is finite-dimensional.

Proof.

Let 𝐯V{\bf v}\in V be a non-zero vector. Consider the subspace U=span{π(g)𝐯|gG}VU=\mathrm{span}\{\pi(g){\bf v}\,|\,g\in G\}\subseteq V. Since UU is spanned by the vectors π(g)𝐯\pi(g){\bf v} as gg runs over all elements of GG, we have 1dimU|G|1\leq\operatorname{dim}U\leq|G|. We claim that (π,U)(\pi,U) is a subrepresentation of (π,V)(\pi,V). Given 𝐮U{\bf u}\in U, we may write it as a linear combination of the spanning elements, i.e.

𝐮=hGzhπ(h)𝐯,{\bf u}=\sum_{h\in G}z_{h}\pi(h){\bf v},

where each zhz_{h}\in{\mathbb{C}}. Given any gGg\in G, we then have

π(g)𝐮=π(g)(hGzhπ(h)𝐯)=hGzhπ(g)π(h)𝐯=hGzhπ(gh)𝐯=hGzg1hπ(h)𝐯.\pi(g){\bf u}=\pi(g)\left(\sum_{h\in G}z_{h}\pi(h){\bf v}\right)=\sum_{h\in G}% z_{h}\pi(g)\pi(h){\bf v}=\sum_{h\in G}z_{h}\pi(gh){\bf v}=\sum_{h\in G}z_{g^{-% 1}h}\pi(h){\bf v}.

The vector hGzg1hπ(h)𝐯\sum_{h\in G}z_{g^{-1}h}\pi(h){\bf v} is a linear combination of vectors in UU, and so is also in UU. The subspace UU is therefore GG-invariant, and hence a subrepresentation. Since (π,V)(\pi,V) is irreducible and U0U\neq 0, V=UV=U. ∎

Theorem 1.3.2.

Let nn be odd. Then Table 1.1 is a complete list of non-isomorphic irreducible representations of DnD_{n}.

Proof.

Firstly, we observe that the matrices in the table satisfy the group relations for DnD_{n}, and so do in fact define representations of DnD_{n}.

Now let (π,V)(\pi,V) to be an irreducible (complex) representation of DnD_{n}. Since VV is finite-dimensional, by Proposition 1.3.1, π(r)\pi(r) has an eigenvector 𝐯V{\bf v}\in V with eigenvalue λ\lambda. Note that 𝐯=π(e)𝐯=π(rn)𝐯=π(r)n𝐯=λn𝐯{\bf v}=\pi(e){\bf v}=\pi(r^{n}){\bf v}=\pi(r)^{n}{\bf v}=\lambda^{n}{\bf v}; λ\lambda is therefore an nn-th root of unity.

Consider the vector 𝐰=π(s)𝐯{\bf w}=\pi(s){\bf v}. The key calculation is:

π(r)𝐰=π(r)π(s)𝐯=π(rs)𝐯=π(sr1)𝐯=π(s)π(r)1𝐯=π(s)(λ1𝐯)=λ1𝐰.\pi(r){\bf w}=\pi(r)\pi(s){\bf v}\\ =\pi(rs){\bf v}=\pi(sr^{-1}){\bf v}=\pi(s)\pi(r)^{-1}{\bf v}=\pi(s)(\lambda^{-% 1}{\bf v})=\lambda^{-1}{\bf w}.

We also have π(s)𝐰=π(s)2𝐯=𝐯\pi(s){\bf w}=\pi(s)^{2}{\bf v}={\bf v} and so span{𝐯,𝐰}\mathrm{span}\{{\bf v},{\bf w}\} is a subrepresentation of VV. As VV is irreducible, we see that V=span{𝐯,𝐰}V=\mathrm{span}\{{\bf v},{\bf w}\}.

  • Case 1:

    Suppose that λλ1\lambda\neq\lambda^{-1}. Then 𝐯{\bf v} and 𝐰{\bf w} are eigenvectors of π(r)\pi(r) with distinct eigenvalues, and so are linearly independent. Thus dimV=2\operatorname{dim}V=2. In the basis 𝐯,𝐰{\bf v},{\bf w}, the representation is

    π(r)\displaystyle\pi(r) =(λ00λ1)\displaystyle=\left(\begin{matrix}\lambda&0\\ 0&\lambda^{-1}\end{matrix}\right)
    π(s)\displaystyle\pi(s) =(0110).\displaystyle=\left(\begin{matrix}0&1\\ 1&0\end{matrix}\right).

    If λ=e2πik/n\lambda=e^{2\pi ik/n} for some 1k<n/21\leq k<n/2, then we get the representation ρk\rho_{k}. Otherwise, λ=e2πik/n\lambda=e^{-2\pi ik/n} for some 1k<n/21\leq k<n/2 and we instead take the basis 𝐰,𝐯{\bf w},{\bf v} to get ρk\rho_{k} again.

  • Case 2:

    Suppose that λ=λ1\lambda=\lambda^{-1}. Then λ=1\lambda=1 as nn is odd. Since

    π(r)(𝐯+𝐰)=π(s)(𝐯+𝐰)=𝐯+𝐰,\pi(r)({\bf v}+{\bf w})=\pi(s)({\bf v}+{\bf w})={\bf v}+{\bf w},

    we see that 𝐯+𝐰{\bf v}+{\bf w} spans a subrepresentation of VV. If 𝐯+𝐰0{\bf v}+{\bf w}\neq 0, then V=(𝐯+𝐰)V={\mathbb{C}}({\bf v}+{\bf w}) is the trivial representation. Otherwise, π(s)𝐯=𝐰=𝐯\pi(s){\bf v}={\bf w}=-{\bf v}, and we get the representation ϵ\epsilon.

    It remains to show that the representations in the table are non-isomorphic; this is left as Exercise 1.3.2 below.

1.3.2. Exercises

..

Problem 25.

  1. (a)

    Show that if (π,V)(\pi,V) and (ρ,W)(\rho,W) are two isomorphic finite-dimensional representations of a group GG, then π(g)\pi(g) and ρ(g)\rho(g) have the same eigenvalues for all gGg\in G.

  2. (b)

    Complete the proof of Theorem 1.3.2.

Problem 26. Find all the irreducible representations of DnD_{n} for nn even.

Problem 27. Show that the irreducible representations of S3S_{3} consist of (a) The 1-dimensional trivial representation (b) the sign representation (sgn,)(\mathrm{sgn},{\mathbb{C}}), where sgn(σ){±1}\mathrm{sgn}(\sigma)\in\{\pm 1\} is the sign of the permutation σ\sigma, and (c) the representation (π,W0)(\pi,W_{0}), where π\pi is the usual permutation representation of S3S_{3} on 3{\mathbb{C}}^{3}, and W0={(z1,z2,z3)3|z1+z2+z3=0}W_{0}=\{(z_{1},z_{2},z_{3})\in{\mathbb{C}}^{3}\,|\,z_{1}+z_{2}+z_{3}=0\}. Hint: use the fact that we have a complete classification of the irreducible representations of DnD_{n}.

Problem 28. Classify the irreducible representations of Q8Q_{8}. Hint: adapt the strategy we used for DnD_{n}.