2020-04-03, Friday
Parallel Transport.
Let γ:[0,1]→M be an embedded smooth curve. (If you worry about the boundary, think of an embedded curve (−ϵ,1+ϵ)→M.) Let E→M be a vector bundle, ∇ be a connection. Our goal is to define the isomorphism
Pγ:Eγ(0)→Eγ(1).
Suppose u0∈Eγ(0), we want to find a section ut∈Eγ(t), such that
∇γ˙(t)ut=0.
Namely, we should have a 'constant' (or flat) section t↦ut, living over the image of γ.
The above statement is correct morally, however, ∇γ˙(t)ut notation is problematic since ut is only a section living on a line, not on an open set of M. There are two ways to make this rigorous.
One is to go to a coordinate patch. Say image of
γ is contained in a trivializing patch
U of
E, and we have
{eα} a frame of
E, and
x1,⋯,xn are base coordinate, then we may express a section using the coefficients
ut=α∑uα(t)eα(γ(t))∈Eγ(t). The collection of coefficients
uα(t) should satisfy a system of ODE
dtduα(t)+Γiβα(γ(t))γ˙i(t)uβ(t)=0.
The second way, is to define the pullback bundle
γ∗E and the pull-back connection
γ∗∇. In fact, this can be defined more generally. Let
(M,E,∇) be a bundle with connection, and
F:N→M be a smooth map. We can define
F∗E the pull-back bundle on
N, by setting
(F∗E)p=EF(p) for any
p∈N, and we can define the connection on
F∗E by setting
(F∗∇)Xp(F∗s)=(∇F∗(Xp)s)∣p where
s is a section of
E defined near
F(p), and
Xp is a tangent vector in
TpN. see
this mathoverflow discussion for why this defines the pullback connection.
Curvature
Prop 3.3.8 [Ni] We may extend ∇:Ω0(M,E)→Ω1(M,E) to ∇:Ωk(M,E)→Ωk+1(M,E), such that it satisfies the Leibniz rule. If ω∈Ωr(M) and u∈Ωs(M,E), then
d∇(ω∧u)=d(ω)∧u+(−1)∣ω∣ω∧∇(u).
([Ni] uses d∇ for this extension, where I still use ∇.)
Prop For any smooth function f∈C∞(M) and ω∈Ωr(M,E), we have
(∇2)(fω)=f∇2(ω)
Proof: This is a calculation worth doing,
∇(dfω+f∇(ω))=dd(f)ω−df∇(ω)+df∇(ω)+f∇2(ω)=f∇2(ω).
Recall that, if a map a:Ωk(M,E)→Ωk+s(M,E) is a C∞(M)-linear map, then
the action of a is point-wise (no derivative of section of E is neede). In other word, we may view a∈Ωs(M, End(E)).
Curvature We define the curvature F∇=∇2∈Ω2(M, End(E))
Suppose we have a local trivialization {eα} over U⊂M. Then, we have an induced trivial connection dU on E∣U, and we may write
∇∣U=dU+A, for some A∈Ω1(U, End(E)). We then have
F∇∣U=(∇∣U)2=(dU+A)2=dUA+A∧A
where we define ∧:Ωr(M, End(E))×Ωs(M, End(E))→Ωr+s(M, End(E)) by ∧ on the form factor, and compose on the associative algebra factor End(E)
(η⊗a)∧(ξ⊗b)=(η∧ξ)⊗(ab),η,ξ∈Ω∗(M),a,b∈Ω0( End(E)).
In the following, ω denote k-form, u denote section of E. X,Y,Z are vector fields. We have
∇X(ω⊗u)=LX(ω)⊗u+ω⊗∇X(u)
iX∇+∇iX=∇X
iXiY+iYiX=0
∇XiY−iY∇X=i[X,Y]
For example, we test the last formula on Ω1(M,E), η∈Ω1(M), u a section of E,
(∇XiY−iY∇X)(η⊗u)=∇X(η(Y)⊗u)−iY(LX(η)⊗u+η∇Xu)
=LX(η(Y))⊗u+η(Y)⊗∇X(u)−[Y(η(X))+dη(X,Y)]⊗u−η(Y)⊗∇X(u)
=ι[X,Y](η)⊗u
Some formula about curvature
F(X,Y)=[∇X,∇Y]−∇[X,Y]
In local coordinates xi on U, we have
Fij=−Fji=[∇i,∇j]
where ∇i=∇∂i.