Torsion is tensorial: Difference between revisions

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


<math>\tau(nabla)(X,fY) = \nabla_X(fY) = \nabla_{fY}(X) - [X,fY] = (Xf)(Y) + f \nabla_XY - f\nabla_YX - f[X,Y] - (Xf)Y</math>
<math>\tau(\nabla)(X,fY) = \nabla_X(fY) = \nabla_{fY}(X) - [X,fY] = (Xf)(Y) + f \nabla_XY - f\nabla_YX - f[X,Y] - (Xf)Y</math>


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


Canceling terms, yields the required result.
Canceling terms, yields the required result.

Revision as of 14:34, 10 April 2008

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.