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
View other such statements
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.
Facts used
- Leibniz rule for derivations: This states that for a vector field and functions , we have:
- Corollary of Leibniz rule for Lie bracket: This states that for a function and vector fields :
- The Leibniz rule axiom that's part of the definition of a connection, namely:
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 on the left side:
To prove the equality with , we observe that it reduces to showing:
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
Proof: We prove this by expanding everything out on the left side:
(the last step uses the corollary of Leibniz rule).
Canceling terms, yields the required result.