3.14. Lecture 14

3.14.1. Real forms

Here we will use our understanding of the representation theory of SL2⁡(ℝ)\operatorname{SL}_{2}(\mathbb{R}) and SU⁢(2)\mathrm{SU}(2) to tell us about the representation theory of 𝔰⁢𝔩2,ℂ\mathfrak{sl}_{2,\mathbb{C}}, and this will then be used to prove complete reducibility.

Definition 3.14.1.

A real form of a complex Lie algebra 𝔤\mathfrak{g} is a real Lie algebra 𝔥⊆𝔤\mathfrak{h}\subseteq\mathfrak{g} such that every element ZZ of 𝔤\mathfrak{g} can be written uniquely as X+i⁢YX+iY for X,Y∈𝔥X,Y\in\mathfrak{h}.

For dimension reasons, necessary and sufficient conditions are that 𝔥∩i⁢𝔥=0\mathfrak{h}\cap i\mathfrak{h}=0 and dimℝ𝔥=dimℂ𝔤\dim_{\mathbb{R}}\mathfrak{h}=\dim_{\mathbb{C}}\mathfrak{g}.

Example 3.14.2.

The Lie algebra 𝔰⁢𝔩n,ℝ\mathfrak{sl}_{n,\mathbb{R}} is a real form of 𝔰⁢𝔩n,ℂ\mathfrak{sl}_{n,\mathbb{C}}.

Example 3.14.3.

The Lie algebra 𝔰⁢𝔲n\mathfrak{su}_{n} is a real form of 𝔰⁢𝔩n,ℂ\mathfrak{sl}_{n,\mathbb{C}}. Indeed, dimℝ𝔰⁢𝔲n=n2−1=dimℂ𝔰⁢𝔩n,ℂ\dim_{\mathbb{R}}\mathfrak{su}_{n}=n^{2}-1=\dim_{\mathbb{C}}\mathfrak{sl}_{n,% \mathbb{C}} and if X,i⁢X∈𝔰⁢𝔲nX,iX\in\mathfrak{su}_{n} then

i⁢X=−(i⁢X)∗=i⁢X∗=−i⁢XiX=-(iX)^{*}=iX^{*}=-iX

so X=0X=0.

Explicitly, we may write A∈𝔰⁢𝔩n,ℂA\in\mathfrak{sl}_{n,\mathbb{C}} as X+i⁢YX+iY with

X=12⁢(A−A∗)X=\frac{1}{2}(A-A^{*})

and

Y=−i2⁢(A+A∗)Y=\frac{-i}{2}(A+A^{*})

in 𝔰⁢𝔲n\mathfrak{su}_{n}.

Example 3.14.4.

Recall that

𝔰⁢𝔬n={A∈𝔰⁢𝔩n,ℝ|A+AT=0}.\mathfrak{so}_{n}=\{A\in\mathfrak{sl}_{n,\mathbb{R}}\,|\,A+A^{T}=0\}.

Let

𝔰⁢𝔬n,ℂ={A∈𝔰⁢𝔩n,ℂ|A+AT=0}.\mathfrak{so}_{n,\mathbb{C}}=\{A\in\mathfrak{sl}_{n,\mathbb{C}}\,|\,A+A^{T}=0\}.

Since the defining equation A+AT=0A+A^{T}=0 can be checked separately on the real and imaginary parts of AA,

𝔰⁢𝔬n,ℂ={B+i⁢C|B,C∈𝔰⁢𝔬n}\mathfrak{so}_{n,\mathbb{C}}=\{B+iC\,|\,B,C\in\mathfrak{so}_{n}\}

and so 𝔰⁢𝔬n\mathfrak{so}_{n} is a real form of 𝔰⁢𝔬n,ℂ\mathfrak{so}_{n,\mathbb{C}}.

Proposition 3.14.5.

Let 𝔥\mathfrak{h} be a real form of 𝔤\mathfrak{g}. There is a one-to-one correspondence between representations of 𝔥\mathfrak{h} and complex-linear representations of 𝔤\mathfrak{g} under which irreducible representations correspond to irreducible representations.

Proof.

Given a ℂ\mathbb{C}-linear representation of 𝔤\mathfrak{g}, it is a representation of 𝔥\mathfrak{h} by restriction. Conversely, if (ρ,V)(\rho,V) is a representation of 𝔥\mathfrak{h}, then it extends to a unique ℂ\mathbb{C}-linear representation of 𝔤\mathfrak{g} given by the formula (forced by ℂ\mathbb{C}-linearity)

ρ⁢(X+i⁢Y)⁢𝐯=ρ⁢(X)⁢𝐯+i⁢ρ⁢(Y)⁢𝐯.\rho(X+iY){\bf v}=\rho(X){\bf v}+i\rho(Y){\bf v}.

It is an exercise to check this preserves the Lie bracket. The second statement is left as an exercise (Problem 3.14.3). ∎

As a corollary we immediately obtain

Theorem 3.14.6.

The representation theories of 𝔰⁢𝔩n,ℝ\mathfrak{sl}_{n,\mathbb{R}} and 𝔰⁢𝔲n\mathfrak{su}_{n} are ‘the same’ as the complex-linear representation theory of 𝔰⁢𝔩n,ℂ\mathfrak{sl}_{n,\mathbb{C}}. All finite-dimensional irreducible representations of 𝔰⁢𝔩2,ℝ\mathfrak{sl}_{2,\mathbb{R}}, SL2⁡(ℝ)\operatorname{SL}_{2}(\mathbb{R}), 𝔰⁢𝔲2\mathfrak{su}_{2}, or SU⁢(2)\mathrm{SU}(2) are of the form Symn⁡(ℂ2)\operatorname{Sym}^{n}(\mathbb{C}^{2}).

Proof.

The claims about Lie algebras follow from Proposition 3.14.5. By Theorem 3.13.10, every (finite-dimensional) irreducible representation of 𝔰⁢𝔩2,ℂ\mathfrak{sl}_{2,\mathbb{C}}, and thus 𝔰⁢𝔩2,ℝ\mathfrak{sl}_{2,\mathbb{R}}, is of the form Symn⁡(ℂ2)\operatorname{Sym}^{n}(\mathbb{C}^{2}), and these clearly exponentiate to representations of SL2⁡(ℝ)\operatorname{SL}_{2}(\mathbb{R}), despite this not being a simply connected group! Similarly for SU⁢(2)\mathrm{SU}(2) (which is simply connected). Since SL2⁡(ℝ)\operatorname{SL}_{2}(\mathbb{R}) and SU⁢(2)\mathrm{SU}(2) are connected, every representation of them is determined by its derivative, so we have a complete list of the irreducible representations. ∎

3.14.2. Decomposing representations

Theorem 3.14.7.

Let VV be any finite-dimensional complex-linear representation of 𝔰⁢𝔩n,ℂ\mathfrak{sl}_{n,\mathbb{C}}. Then VV is completely reducible, that is, splits into a direct sum of irreducible representations.

Proof.

Let VV be a finite-dimensional complex-linear representation of 𝔰⁢𝔩n,ℂ\mathfrak{sl}_{n,\mathbb{C}} and let W⊆VW\subseteq V be a subrepresentation. Then WW is an 𝔰⁢𝔲n\mathfrak{su}_{n}-subrepresentation, by Theorem 3.14.6. As SU⁢(n)\mathrm{SU}(n) is simply-connected, VV and WW exponentiate to representations of SU⁢(n)\mathrm{SU}(n). Since SU⁢(n)\mathrm{SU}(n) is compact, by Maschke’s theorem (Theorem 2.11.4(ii)) there is a complementary SU⁢(n)\mathrm{SU}(n)-subrepresentation W′W^{\prime} with

V=W⊕W′.V=W\oplus W^{\prime}.

Then W′W^{\prime} is a 𝔰⁢𝔲n\mathfrak{su}_{n}-subrepresentation, and so a ℂ\mathbb{C}-linear 𝔰⁢𝔩n,ℂ\mathfrak{sl}_{n,\mathbb{C}}-subrepresentation, so that

V=W⊕W′V=W\oplus W^{\prime}

as representations of 𝔰⁢𝔩n,ℂ\mathfrak{sl}_{n,\mathbb{C}}. Complete reducibility follows. ∎

The argument in this theorem is called Weyl’s unitary trick. For a similar application of this idea, see the proof of Proposition 3.12.2.

Corollary 3.14.8.

Two finite-dimensional complex-linear representations of 𝔰⁢𝔩2,ℂ\mathfrak{sl}_{2,\mathbb{C}} are isomorphic if and only if they have the same multiset of weights.

Proof.

Let (π,V)(\pi,V) and (ρ,W)(\rho,W) be finite-dimensional complex-linear representations of 𝔰⁢𝔩2,ℂ\mathfrak{sl}_{2,\mathbb{C}}. We can decompose VV into irreducibles by looking at the weights. Firstly, look at the maximal weight kk of VV. Then there must be a weight vector 𝐯{\bf v} of weight kk, which is necessarily a highest weight vector, and so VV must contain a copy of Symk⁡(ℂ2)\operatorname{Sym}^{k}(\mathbb{C}^{2}) — namely, the subspace ⟨𝐯,Y⁢𝐯,…,Yk⁢𝐯⟩\left\langle{\bf v},Y{\bf v},\ldots,Y^{k}{\bf v}\right\rangle. By Theorem 3.14.7 we have

V≅Symk⁡(ℂ2)⊕V′.V\cong\operatorname{Sym}^{k}(\mathbb{C}^{2})\oplus V^{\prime}.

The weights of V′V^{\prime} are then obtained by removing the weights of Symk⁡(ℂ2)\operatorname{Sym}^{k}(\mathbb{C}^{2}) from the weights of VV, and we repeat the process, noting that it terminates as VV is finite dimensional. If we then do the same for WW we see that they decompose into the same sum of copies of Symk⁡(ℂ2)\operatorname{Sym}^{k}(\mathbb{C}^{2}) if and only if they have the same multiset of weights. ∎

3.14.3. Exercises

.

Problem 35. Show that the real Lie algebras 𝔰⁢𝔩2,ℝ\mathfrak{sl}_{2,\mathbb{R}} and 𝔰⁢𝔲2\mathfrak{su}_{2} are not isomorphic. Hint: consider the adjoint action of an arbitrary element of 𝔰⁢𝔲2\mathfrak{su}_{2}.

Problem 36. Finish the proof of Proposition 3.14.5.

Problem 37. We have that Symn⁡(ℂ2)\operatorname{Sym}^{n}(\mathbb{C}^{2}) is the irreducible representation of SU⁢(2)\mathrm{SU}(2) of dimension n+1n+1. Let χn\chi_{n} be its character. Every conjugacy class of SU⁢(2)\mathrm{SU}(2) contains an element of the form

exp⁡(i⁢t⁢H)=(ei⁢t00e−i⁢t).\exp(itH)=\begin{pmatrix}e^{it}&0\\ 0&e^{-it}\end{pmatrix}.

Show that

χn⁢(exp⁡(i⁢t⁢H))=sin⁡((n+1)⁢t)sin⁡(t).\chi_{n}(\exp(itH))=\frac{\sin((n+1)t)}{\sin(t)}.

Problem 38. Let (ρ,V)(\rho,V) be an irreducible representation of 𝔤⁢𝔩2,ℂ\mathfrak{gl}_{2,\mathbb{C}}, and let Z=(1001)Z=\begin{pmatrix}1&0\\ 0&1\end{pmatrix}.

  1. (a)
    ​

    Show that ρ⁢(Z)\rho(Z) is as a scalar.

  2. (b)
    ​

    Show that the restriction of VV to 𝔰⁢𝔩2,ℂ\mathfrak{sl}_{2,\mathbb{C}} is irreducible.

  3. (c)
    ​

    Show that for every λ∈ℂ\lambda\in\mathbb{C} and integer n≥0n\geq 0, there is a unique irreducible representation of 𝔤⁢𝔩2,ℂ\mathfrak{gl}_{2,\mathbb{C}} of dimension n+1n+1 with ρ⁢(Z)=λ⁢Id\rho(Z)=\lambda\operatorname{Id}.

  4. (d)
    ​

    Which of these are derivatives of representations of GL2⁡(ℂ)\operatorname{GL}_{2}(\mathbb{C})? Hence classify the finite dimensional holomorphic irreducible representations of GL2⁡(ℂ)\operatorname{GL}_{2}(\mathbb{C}).

Problem 39. Let VV be a finite-dimensional representation of 𝔰⁢𝔩2,ℂ\mathfrak{sl}_{2,\mathbb{C}}.

  1. (a)
    ​

    What are the weights of the dual representation V∗V^{*}?

  2. (b)
    ​

    Deduce that V≅V∗V\cong V^{*}.