Connectedness
A matrix Lie group G is said to be path-connected (in topology) if given any two matrices A and B in G, there exists a continuous path A(t), a ≤ t ≤ b, lying in G with A(a) = A and A(b) = B. A matrix Lie group is connected if and only if it is path-connected.A matrix Lie group G which is not connected can be decomposed (uniquely) as a union of several pieces, called components, such that two elements of the same component can be joined by a continuous path, but two elements of different components cannot.
Group Connected Components
GL(n;C) yes 1
SL(n;C) yes 1
GL(n;R) no 2
SL(n;R) yes 1
O(n) no 2
SO(n) yes 1
U(n) yes 1
SU(n) yes 1
O(n;1) no 4
SO(n;1) no 2
Heisenberg yes 1
E(n) no 2
P(n;1) no 4
Simple Connectedness
A matrix Lie group G is said to be simply connected if it is connected and, in addition, every loop in G can be shrunk continuously to a point in G. More precisely, assume that G is connected. Then, G is simply connected if given any continuous path A(t), 0 ≤ t ≤ 1, lying in G with A(0) = A(1), there exists a continuous function A(s,t), 0 ≤ s,t ≤ 1, taking values in G and having the following properties:
(2) A(0,t) = A(t), when s=0 the loop is the specified loop A(t);
(3) A(1,t) = A(1,0) for all t, when s=1 the loop is a point.
Group versus Lie Algebra Homomorphisms
(A) Lie algebra homomorphism
Every Lie group homomorphism give rise to a Lie algebra homomorphism. Let G and H be matrix Lie groups, with Lie algebras g and h, respectively. Suppose that Φ : G --> H is a Lie group homomorphism. Then, there exists a unique real linear map ϕ : g --> h such that for all X ∈ g. The map ϕ has the following additional properties:(1) ϕ (AXA-1) = Φ(A) ϕ(X) Φ(A)-1, for all X ∈ g, A ∈ G.
(2) ϕ([X,Y]) = [ ϕ(X), ϕ(Y)], for all X, Y ∈ g (Lie algebra homomorphism)
(3) ϕ(X) = d/dt Φ(etX) |t=0, for all X ∈ g
(B) Lie group homomorphism
Let G and H be matrix Lie groups with Lie algebras g and h. Let ϕ : g --> h be a Lie algebra homomorphism. If G is simply connected , then there exists a unique Lie group homomorphism Φ : G --> H such that Φ(eX) = eϕ(X) for all X ∈ g. However, if G is not simply connected, this will not be true. We should look for Ğ that has the same Lie algebra as G but such that Ğ is simply connected.
Baker-Campbell-Hausdorff formula says that if X and Y are sufficiently small, then
log(eXeY) = X + Y + 1/2[X,Y] + 1/12[X,[X,Y]] - 1/12[Y,[X,Y]] + ...
Because ϕ is a Lie algebra homomorphism,ϕ(log(eXeY)) = ϕ(X) + ϕ(Y) + 1/2[ϕ(X),ϕ(Y)] + 1/12[ϕ(X),[ϕ(X),ϕ(Y)]] - 1/12[ϕ(Y),[ϕ(X),ϕ(Y)]] + ... = log(eϕ(X)eϕ(Y))
For group homomorphism, Φ(eXeY) = exp(ϕ(eXeY) = exp(ϕ(exp(log(eXeY) ))). From above, Φ(eXeY) = exp(log(eϕ(X)eϕ(Y))) = eϕ(X)eϕ(Y) = Φ(eX)Φ(eY). Therefore, by Baker-Campbell-Hausdorff formula, if X is small, Φ is a group homomorphism.Covering Groups
Let G be a connected Lie group. Then, a universal covering group (or universal cover) of G is a simply-connected Lie group H together with with a Lie group homomorphism Φ : H --> G such that the associated Lie algebra homomorphism ϕ : h --> g is a Lie algebra homomorphism. The homomorphism Φ is called the covering homomorphism (or projection map).
For any connected Lie group, a universal cover exists. If G is a connected Lie group and (H1, Φ1) and (H2, Φ2) are universal covers of G, then there exists a Lie group isomorphism Ψ : H1 --> H2 such that Φ2 o Ψ = Φ1.
The universal cover of a matrix Lie group may not be a matrix Lie group.
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