6 SL2

6.4 Real forms and complete decomposability

We use our understanding of the representation theory of 𝔰𝔩2, into an understanding of the representation theory of SL2() and SU(2), and prove complete reducibility.

Definition 6.23.

A real form of a complex Lie algebra 𝔤 is a real Lie algebra 𝔥𝔤 such that every element Z of 𝔤 can be written uniquely as X+iY for X,Y𝔥.

Remark 6.24.

In lectures, we didn’t give this definition, just doing the special case of 𝔰𝔲n𝔰𝔩n,.

For dimension reasons, necessary and sufficient conditions are that 𝔥i𝔥=0 and dim𝔥=dim𝔤.

Example 6.25.

The Lie algebra 𝔰𝔩n, is a real form of 𝔰𝔩n,.

Example 6.26.

The Lie algebra 𝔰𝔲n is a real form of 𝔰𝔩n,. Indeed, dim𝔰𝔲n=n2-1=dim𝔰𝔩n, and if X,iX𝔰𝔲n then

iX=-(iX)=iX=-iX

so X=0.

Explicitly, we may write A𝔰𝔩n, as X+iY with

X=12(A-A)

and

Y=-i2(A+A)

in 𝔰𝔲n.

Example 6.27.

Recall that

𝔰𝔬n={A:n,A+AT=0}.

Let

𝔰𝔬n,={A:n,A+AT=0}.

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

𝔰𝔬n,={B+iC:B,C𝔰𝔬n}

and so 𝔰𝔬n is a real form of 𝔰𝔬n,.

Proposition 6.28.

Let 𝔥 be a real form of 𝔤.

There is a one-to-one correspondence between representations of 𝔥 and complex-linear representations of 𝔤 under which irreducible representations correspond to irreducible representations.

Proof.

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

ρ(X+iY)v=ρ(X)v+iρ(Y)v.

It is easy to see that this preserves the Lie bracket. The proposition follows (the final statement is left as an exercise). ∎

As a corollary we immediately obtain

Theorem 6.29.

The representation theories of 𝔰𝔩n, and 𝔰𝔲n are ‘the same’ as the complex-linear representation theory of 𝔰𝔩n,. All finite-dimensional irreducible representations of 𝔰𝔩2,R, SL2(), 𝔰𝔲2, or SU(2) are of the form Symn(2).

Proof.

The claims about Lie algebras follow from the above discussion. Every (finite-dimensional) irreducible representation of 𝔰𝔩2, is of the form Symn(2), and these clearly exponentiate to representations of SL2(), despite this not being a simply connected group! Similarly for SU(2) (which is simply connected). Since SL2() and SU(2) are connected, every representation of them is determined by its derivative, so we have a complete list of the irreducible representations. ∎

Theorem 6.30.

Every finite-dimensional complex-linear representation of 𝔰𝔩n, is completely reducible.

Proof.

Let V be a finite-dimensional complex-linear representation of 𝔰𝔩n, and let WV be a subrepresentation. Then W is an 𝔰𝔲n-subrepresentation. As SU(n) is simply-connected, V and W exponentiate to representations of SU(n). Since SU(n) is compact, by Maschke’s theorem there is a complementary SU(n)-subrepresentation W with

V=WW.

Then W is a 𝔰𝔲n-subrepresentation, and so a -linear 𝔰𝔩n,-subrepresentation, so that

V=WW

as representations of 𝔰𝔩n,. 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 6.2.