The previous few lectures have prepared us for the following definitions.
Definition (Lie Group). A Lie group is a group that is also a smooth manifold (i.e. looks like Rn locally).
Example. All of the following are Lie groups: {GLn(R),GLn(C),SOn,Un,SUn}. However, GLn(Q) is not a Lie group—it has too many “holes” in it.
Definition (One-Parameter Subgroup). Given a Lie group G, a one-parameter subgroupH⊆G is a subgroup that is the image of a differentiable homomorphism φ:R→G.
Example. The longitudinal subgroups from last lecture are one-parameter subgroups of SU2.
Theorem. (Determinant and Trace) For any A∈Cn×n, we have deteA=etr(A).
Proof: This holds when A is diagonalizable. By continuity, it holds for all A. ■
The point of all this setup is the following observation:
Observation. For any A∈Cn×n, the map φA:R→GLn(C) via φA(s)=esA yields a one-parameter subgroup of GLn(C).
In particular, the derivative is dsdφA(s)=AφA(s).
Remark. (Reading Comprehension) Why is φA(s)=esA∈GLn(C) always true for any A∈Cn×n?
And here's an even stronger observation.
Theorem. (One-Parameter General Subgroups) Suppose φ:R→GLn(C) yields a one-parameter subgroup of GLn(C). Then φ looks like φ:s↦eAs for some A∈Cn×n.
Proof: This is effectively a functional equation, with constraints:
(1)φ(0)=In(2)φ(s+t)=φ(s)φ(t)
Differentiating (2) and taking s=0 yields φ′(t)=φ′(0)φ(t). Say A=φ′(0). The point is that φ′(t)=Aφ(t) is a linear first-order ODE, so it has a unique solution satisfying (1), and φ:t↦etA is such a solution. ■
Remark. Recall the only solution to Cauchy's FE—provided f is continuous!—is the linear equation.
One can think of every one-parameter subgroup of GLn(C) as being parametrized by its “tangent vector” φ′(0). Once the “initial conditions” φ(0)=In and φ′(0)=A are set, the rest of the path is fixed!
§ One-Parameter Subgroups of SLn(C) and On(R)
More generally, for any subgroup G⊆GLn(C), the one-parameter subgroups of G are precisely the images of maps φ:R→G via φ:s↦eAs for some A∈Cn×n. The only constraint on A is that eAs∈G for all s∈R.
Let's investigate this constraint for various G⊆GLn(C).
Theorem. (One-Parameter Special Subgroups) The one-parameter subgroups of SLn(C) are precisely the images of φ:s↦esA for some A∈Cn×n satisfying tr(A)=0.
Proof: We just need esA∈SLn(C) for all s∈R, or:
detesA=1⟹1=detesA=etr(sA)=es⋅tr(A).
And the above could only hold for all s if tr(A)=0. ■
Similarly, we can talk about one-parameter subgroups of On(R).
Theorem. (One-Parameter Orthogonal Subgroups) The one-parameter subgroups of On(R) are precisely the images of φ:s↦esA for some A∈Rn×n satisfying A⊤=−A (i.e. skew-symmetric matrices).
Proof: We just need esA∈On(R) for all s∈R, or:
In=esA(esA)⊤=esAesA⊤.
Differentiating at s=0 forces A+A⊤=0, so A⊤=−A. ■
The one-parameter subgroups of On(R) actually tell us about its dimension!
Theorem. (Dimension of Orthogonal Subgroups) We have dimOn(R)=(2n).
Proof: It's equivalent to know the dimension of the set of one-parameter subgroups of On(R). But these biject with the set of skew-symmetric matrices, which is of dimension (2n). ■
Remark. This is pretty hard to show without inspecting the one-parameter subgroups!
Note that if φ:s↦esA describes a one-parameter subgroup of G, we need not have A∈G. For example, A=[100−1] generates a one-parameter subgroup of SL2(C), but [100−1] is not in SL2(C). We only need A∈Cn×n.
Remark. (Reading Comprehension) Show that the one-parameter subgroups of SU2 are precisely the images of φ:s↦esA for some A∈Cn×n satisfying A†=−A and tr(A)=0. For example, A=[i6−6−i] works.
If A∈Cn×n does not satisfy this, then the path φ(s):=esA will “fly off” the surface S3.
§ Lie Algebras and Lie Brackets
Definition (Lie Algebra). If G is a Lie group, then its Lie algebraLie(G) is the tangent space at its identity—in other words, the set of all possible φ′(0) for one-parameter subgroups φ:R→G.
Definition (Lie Bracket). Every Lie algebra of matrices is equipped with the Lie bracket[A,B]:=AB−BA.
Example. The Lie algebra of SLn(C) is {A∈Cn×n:tr(A)=0}, and that of On(R) is {A∈Rn×n:A⊤=−A}. Meanwhile, the Lie algebra of GLn(C) is just all of Cn×n.
In the specific case of matrix groups, we have the following alternative definition:
Definition (Lie Algebra). If G⊆GLn(C) is a Lie group, then its Lie algebra is:
Lie(G):={A∈Cn×n∣esA∈G for all s∈R}.
Let's check some closure properties of Lie algebras and the Lie bracket.
Theorem. (Closure of Addition) For any A,B∈Lie(G), we have A+B∈Lie(G).
Proof: The fact that A,B∈Lie(G) is equivalent to the fact that esA and esB are in G for all s∈R. Therefore, their product esAesB=In+(A+B)s+O(s2) is in G for all s∈R, so A+B is a valid direction in the tangent space at the identity, meaning A+B∈Lie(G). ■
Theorem. (Closure of Lie Bracket) For any A,B∈Lie(G), we have [A,B]∈Lie(G).
Proof: The idea is to consider the following expression:
eAseBse−Ase−Bs==(1+As+2A2s2+O(s3))(1+Bs+2B2s2+O(s3))(…e−As…)(…e−Bs…)1+(AB−BA)s2+O(s3) after much simplification.
The above is in G for all s∈R. Thus, sending s→0, we see es2(AB−BA) is in G. Therefore, “locally” speaking, AB−BA is a valid direction in the tangent space at the identity, so AB−BA=[A,B] is in Lie(G). ■
Remark. It is not the case that A,B∈Lie(G) implies AB∈Lie(G). (Try to find a counterexample!)
The Lie Bracket also has a bunch of identities, which one can check if they really want to.
Theorem. (Lie Bracket Identities) The following identities are true for any A,B,C∈Lie(G) and c∈R.
Remark. Identity (4) is known as the Jacobi Identity, equivalent to [A,[B,C]]=[[A,B],C]+[B,[A,C]].
There's a neat analogy to the product rule dtd[f(t)g(t)]=[dtdf(t)]g(t)+f(t)[dtdg(t)].
Every Lie group has a corresponding Lie algebra, found via “differentiation”. However, just as “integration” always has a +C term, not every Lie algebra has a unique Lie group; uniqueness is only guaranteed up to coverings.
Example. Both R and S1 have isomorphic Lie algebras, and R/Z≅S1 indicates their mutual covering group.
We care about Lie algebras because they turn geometry and physics problems (i.e. Lie groups) into linear algebra problems (i.e. Lie algebras).