Torsion is tensorial: Difference between revisions

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(New page: ==Statement== ===Symbolic statement=== Let <math>M</math> be a differential manifold and <math>\nabla</math> be a linear connection on <math>M</math> (viz., <math>\nabla</math> i...)
 
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given by:
given by:


<math>\tau(\nabla)(X,Y) = \nabla_X Y - \nabla_Y X - [X,Y]</math>
<math>\tau(\nabla)(X,Y) = \nabla_Y X - \nabla_X Y - [X,Y]</math>


Then, <math>\tau(\nabla)</math> is a [[tensorial map]] in both coordinates.
Then, <math>\tau(\nabla)</math> is a [[tensorial map]] in both coordinates.
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''Proof'': We prove this by expanding everything out:
''Proof'': We prove this by expanding everything out:


<math>\tau(\nabla)(fX,Y) = \nabla_{fX}(Y) - \nabla_Y(fX) - [fX,Y] = f \nabla_XY - f \nabla_Y X - (Xf)(Y) - [fX,Y]</math>
<math>\tau(\nabla)(fX,Y) = \nabla_Y(fX) - \nabla_{fX}(Y) - [fX,Y] = f \nabla_YX  - f \nabla_Y X - (Yf)(X) - [fX,Y]</math>


To prove the equality with <math>f \tau(\nabla)(X,Y)</math>, we need to show:
To prove the equality with <math>f \tau(\nabla)(X,Y)</math>, we need to show:


<math>(Xf)(Y) = f[X,Y] - [fX,Y]</math>
<math>(Yf)(X) = f[X,Y] - [fX,Y]</math>


To prove this, we need to show that both sides evaluate to the same expression for any function <math>g</math>. Plugging a function <math>g</math>, we see that the right side becomes:
To prove this, we need to show that both sides evaluate to the same expression for any function <math>g</math>. Plugging a function <math>g</math>, we see that the right side becomes:


<math>f(X(Yg) - Y(Xg)) - f(X(Yg)) + Y((fX)g) = Y((fX)g) - f(Y(Xg)) </math>
<math>f(X(Yg) - Y(Xg)) - f(X(Yg)) + Y((fX)g) = Y(f(Xg)) - f(Y(Xg)) </math>


The left hand side is:
Applying the Leibniz rule for <math>Y</math> on the product of functions <math>f</math> and <math>Xg</math>, this simplifies to:


<math>(Xf)(Yg) = (Yg)(Xf) = Y(g(Xf))
<math>(Yf)(Xg) + Y(Xg)(f) - f(Y(Xg)) = (Yf)(Xg)</math>
 
which is precisely equal to the left side.
 
===Tensoriality in the second coordinate===
 
The proof is analogous to that for the first coordinate.
 
{{fillin}}

Revision as of 00:36, 5 April 2008

Statement

Symbolic statement

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

Consider the torsion of , namely:

given by:

Then, is a tensorial map in both coordinates.

Proof

Tensoriality in the first coordinate

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

To prove:

Proof: We prove this by expanding everything out:

To prove the equality with , we need to show:

To prove this, we need to show that both sides evaluate to the same expression for any function . Plugging a function , we see that the right side becomes:

Applying the Leibniz rule for on the product of functions and , this simplifies to:

which is precisely equal to the left side.

Tensoriality in the second coordinate

The proof is analogous to that for the first coordinate.

Fill this in later