Torsion is tensorial: Difference between revisions

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==Facts used==
==Facts used==
* [[Leibniz rule for derivations]]: This states that for a vector field <math>X</math> and functions <math>f,g</math>, we have:


<math>\! X(fg) = (Xf)(g) + f(Xg)</math>
{| class="sortable" border="1"
 
! Fact no. !! Name !! Statement with symbols
* [[Corollary of Leibniz rule for Lie bracket]]: This states that for a function <math>f</math> and vector fields <math>X,Y</math>:
|-
 
| 1 || Any connection is <math>C^\infty</math>-linear in its subscript argument || <math>\nabla_{fA} = f\nabla_A</math> for any <math>C^\infty</math>-function <math>f</math> and vector field <math>A</math>.
<math>\! f[X,Y] = [fX,Y] + (Yf)X</math>
|-
 
| 2 || The Leibniz-like axiom that is part of the definition of a connection || For a function <math>f</math> and vector fields <math>A,B</math>, and a connection <math>\nabla</math>, we have <math>\nabla_A(fB) = (Af)(B) + f\nabla_A(B)</math>
<math>\! f[X,Y] = [X,fY] - (Xf)Y</math>
|-
 
| 3 || [[uses::Corollary of Leibniz rule for Lie bracket]] (in turn follows from [[uses::Leibniz rule for derivations]]|| For a function <math>f</math> and vector fields <math>X,Y</math>:
* The Leibniz rule axiom that's part of the definition of a [[connection]], namely:
<br><math>\! f[X,Y] = [fX,Y] + (Yf)X</math><br><math>\! f[X,Y] = [X,fY] - (Xf)Y</math>
 
|}
<math>\! \nabla_X(fZ) = (Xf)(Z) + f\nabla_X(Z)</math>


==Proof==
==Proof==

Revision as of 17:36, 6 January 2012

This article gives the statement, and possibly proof, that a map constructed in a certain way is tensorial
View other such statements

Statement

Symbolic statement

Let M be a differential manifold and be a linear connection on M (viz., is a connection on the tangent bundle TM of M).

Consider the torsion of , namely:

τ():Γ(TM)×Γ(TM)Γ(TM)

given by:

τ()(X,Y)=XYYX[X,Y]

Then, τ() is a tensorial map in both coordinates.

Facts used

Fact no. Name Statement with symbols
1 Any connection is C-linear in its subscript argument fA=fA for any C-function f and vector field A.
2 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)+fA(B)
3 Corollary of Leibniz rule for Lie bracket (in turn follows from Leibniz rule for derivations For a function f and vector fields X,Y:


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

Proof

Tensoriality in the first coordinate

We'll use the fact that tensoriality is equivalent to C-linearity.

To prove: τ()(fX,Y)=fτ()(X,Y)

Proof: We prove this by expanding everything out on the left side:

τ()(fX,Y)=fX(Y)Y(fX)[fX,Y]=fXYfYX(Yf)(X)[fX,Y]

To prove the equality with fτ()(X,Y), we observe that it reduces to showing:

(Yf)(X)=f[X,Y][fX,Y]

which is exactly what the corollary of Leibniz rule above states.

Tensoriality in the second coordinate

The proof is analogous to that for the first coordinate.

To prove τ()(X,fY)=fτ()(X,Y)

Proof: We prove this by expanding everything out on the left side:

τ()(X,fY)=X(fY)=fY(X)[X,fY]=(Xf)(Y)+fXYfYXf[X,Y](Xf)Y

(the last step uses the corollary of Leibniz rule).

Canceling terms, yields the required result.