Torsion is tensorial: Difference between revisions
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==Facts used== | ==Facts used== | ||
<math>\ | {| class="sortable" border="1" | ||
! Fact no. !! Name !! Statement with symbols | |||
|- | |||
| 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>: | |||
<br><math>\! f[X,Y] = [fX,Y] + (Yf)X</math><br><math>\! f[X,Y] = [X,fY] - (Xf)Y</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 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
| Fact no. | Name | Statement with symbols |
|---|---|---|
| 1 | Any connection is -linear in its subscript argument | for any -function and vector field . |
| 2 | The Leibniz-like axiom that is part of the definition of a connection | For a function and vector fields , and a connection , we have |
| 3 | Corollary of Leibniz rule for Lie bracket (in turn follows from Leibniz rule for derivations | For a function and vector fields :
|
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.