Torsion is tensorial: Difference between revisions

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* [[Leibniz rule for derivations]]: This states that for a vector field <math>X</math> and functions <math>f,g</math>, we have:
* [[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>
<math>\! X(fg) = (Xf)(g) + f(Xg)</math>


* [[Corollary of Leibniz rule for Lie bracket]]: This states that for a function <math>f</math> and vector fields <math>X,Y</math>:
* [[Corollary of Leibniz rule for Lie bracket]]: This states that for a function <math>f</math> and vector fields <math>X,Y</math>:


<math>f[X,Y] = [fX,Y] + (Yf)X</math>
<math>\! f[X,Y] = [fX,Y] + (Yf)X</math>


<math>f[X,Y] = [X,fY] - (Xf)Y</math>
<math>\! f[X,Y] = [X,fY] - (Xf)Y</math>


* The Leibniz rule axiom that's part of the definition of a [[connection]], namely:
* The Leibniz rule axiom that's part of the definition of a [[connection]], namely:


<math>\nabla_X(fZ) = (Xf)(Z) + f\nabla_X(Z)</math>
<math>\! \nabla_X(fZ) = (Xf)(Z) + f\nabla_X(Z)</math>


==Proof==
==Proof==

Revision as of 01:18, 24 July 2009

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

X(fg)=(Xf)(g)+f(Xg)

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

f[X,Y]=[X,fY](Xf)Y

  • The Leibniz rule axiom that's part of the definition of a connection, namely:

X(fZ)=(Xf)(Z)+fX(Z)

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.