Curvature is tensorial

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This article gives the statement, and possibly proof, that a map constructed in a certain way is tensorial
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Statement

Let ∇ be a connection on a vector bundle E over a differential manifold M. The Riemann curvature tensor of ∇ is given as a map Γ(TM)⊗Γ(TM)⊗Γ(E)→Γ(E) defined by:

R(X,Y)Z=∇X∇YZ−∇Y∇XZ−∇[X,Y]Z

We claim that R is a tensorial map in each of the variables X,Y,Z.

Related facts

Facts used

Fact no. Name Full statement
1 Leibniz rule for derivations For a vector field X and functions f,g, we have: X(fg)=(Xf)(g)+f(Xg)
2 Corollary of Leibniz rule for Lie bracket For a function f and vector fields X,Y:


f[X,Y]=[fX,Y]+(Yf)X
f[X,Y]=[X,fY]−(Xf)Y

3 The Leibniz-like axiom that is part of the definition of a connection For a function f and vector fields A,B, and a connection ∇, we have ∇A(fB)=(Af)(B)+f∇A(B)

Proof

To prove tensoriality in a variable, it suffices to show C∞-linearity in that variable. This is because linearity in C∞-functions guarantees linearity in a function that is 1 at exactly one point, and zero at others.

The proofs for X and Y are analogous, and rely on manipulation of the Lie bracket [fX,Y] and the property of a connection being C∞ in the subscript vector. These proofs do not involve any explicit use of Z. The proof for Z relies simply on repeated application of the product rule, and the fact that XY−YX=[X,Y].

Tensoriality in the first variable

Given: f:M→R is a C∞-function.

To prove: R(fX,Y)=fR(X,Y), or more explicitly, ∇fX∇Y−∇Y∇fX−∇[fX,Y]=f(∇X∇Y−∇Y∇X−∇[X,Y]

We start out with the left side:

∇fX∇Y−∇Y∇fX−∇[fX,Y]

Each step below is obtained from the previous one via some manipulation explained along side.

Step no. Current status of left side Facts/properties used Specific rewrites
1 f∇X∇Y−∇Y(f∇X)−∇[fX,Y] By definition of a connection, ∇ is C∞-linear in its subscript argument. ∇fX→f∇X
2 f∇X∇Y−(Yf)∇X−f∇Y∇X−∇[fX,Y] Fact (3), the Leibniz-like axiom for connection. ∇Y(f∇X)→(Yf)∇X+f∇Y∇X. To understand this more clearly imagine an input Z to the whole expression, so that the rewrite becomes ∇Y(f∇X(Z))→(Yf)∇X(Z)+f∇Y∇X(Z). In the notation of fact (3), A=Y, f=f, and B=∇X(Z).
3 f(∇X∇Y−∇Y∇X)−∇(Yf)X+[fX,Y] ∇ is C∞-linear in its subscript argument <nath>(Yf)\nabla_X \to \nabla_{(Yf)X}</math>
4 f(∇X∇Y−∇Y∇X−∇[X,Y]) Fact (2) [fX,Y]→f[X,Y]−(Yf)X.

Tensoriality in the second variable

Let f:M→R be a scalar function. We will show that:

R(X,fY)=fR(X,Y)

We start out with the left side:

∇X∇fY−∇fY∇X−∇[X,fY]

Applying the Leibniz rule and the property of a connection being C∞ in its subscript variable yields:

(Xf)∇Y+f(∇X∇Y−∇Y∇X)−∇[X,fY]

which simplifies to:

f(∇X∇y−∇Y∇X)−∇[X,fY]−(Xf)Y

We now use the corollary stated above:

f[X,Y]=[X,fY]−(Xf)Y

substituting this gives:

f(∇X∇Y−∇Y∇X−∇[X,Y]

which is fR(X,Y)

Tensoriality in the third variable

Let f:M→R be a scalar function. We will show that:

R(X,Y)(fZ)=fR(X,Y)Z

We start out with the left side:

∇X∇Y(fZ)−∇Y∇X(fZ)−∇[X,Y](fZ)

Now we apply the Leibniz rule for connnections on each term:

∇X((Yf)(Z)+f∇YZ)−∇Y((Xf)Z+f∇XZ)−f∇[X,Y]Z−([X,Y]f)Z

We again apply the Leibniz rule to the first two term groups:

(XYf)(Z)+(Yf)∇XZ+(Xf)∇YZ+f∇X∇YZ−(YXf)Z−(Xf)∇YZ−(Yf)∇XZ−f∇Y∇XZ−f∇[X,Y]Z−([X,Y]f)Z

After cancellations we are left with the following six terms:

f(∇X∇Y−∇Y∇X−∇[X,Y])Z+((XY−YX−[X,Y])f)Z

But since [X,Y]=XY−YX, the last three terms vanish, and we are left with:

fR(X,Y)Z