Parallel transport around a loop

Click For Summary
SUMMARY

The discussion focuses on the concept of parallel transport in the context of the Riemann curvature tensor, specifically examining the behavior of commuting vector fields X and Y. It establishes that the parallel transport of a vector Z around a quadrilateral formed by these fields is represented by the expression τ_{sX}^{-1}τ_{tY}^{-1}τ_{sX}τ_{tY}Z, which quantifies the failure of Z to return to its original position in the tangent space Tx0M. The discussion highlights that the closure of the quadrilateral is guaranteed when X and Y commute, and introduces the torsion tensor T(X,Y) to measure deviations from this closure in the presence of torsion.

PREREQUISITES
  • Understanding of Riemann curvature tensor
  • Familiarity with vector fields and diffeomorphisms
  • Knowledge of parallel transport concepts
  • Basic grasp of torsion in differential geometry
NEXT STEPS
  • Study the properties of the Riemann curvature tensor in detail
  • Explore the mathematical implications of torsion in differential geometry
  • Learn about the proof of closure for commuting vector fields
  • Investigate applications of parallel transport in general relativity
USEFUL FOR

Mathematicians, physicists, and students of differential geometry who are interested in the intricacies of parallel transport, curvature, and torsion in the context of Riemannian manifolds.

dEdt
Messages
286
Reaction score
2
From the Wikipedia article on the Riemann curvature tensor:
Suppose that X and Y are a pair of commuting vector fields. Each of these fields generates a pair of one-parameter groups of diffeomorphisms in a neighborhood of x0. Denote by τtX and τtY, respectively, the parallel transports along the flows of X and Y for time t. Parallel transport of a vector Z ∈ Tx0M around the quadrilateral with sides tY, sX, −tY, −sX is given by
\tau_{sX}^{-1}\tau_{tY}^{-1}\tau_{sX}\tau_{tY}Z.
This measures the failure of parallel transport to return Z to its original position in the tangent space Tx0M.

The last sentence assumes that ##\tau_{sX}^{-1}\tau_{tY}^{-1}\tau_{sX}\tau_{tY}## returns Z back to x0. It isn't obvious to me that this should be true. My guess is that this is true because X and Y commute, but I can't think of a proof for this claim.
 
Physics news on Phys.org
X and Y being commuting fields is equivalent to the quadrilateral being closed (provided there is no torsion).

In the presence of torsion, quadrilaterals of commuting vectors fail to close, and the torsion tensor measures the amount by which they fail to close:

T(X,Y) \equiv \nabla_X Y - \nabla_Y X - [X,Y]
Here ##Z = T(X,Y)## is the vector that closes the gap left after taking into account the possibility that X and Y fail to commute.
 
X and Y being commuting fields is equivalent to the quadrilateral being closed (provided there is no torsion).

That's what I suspected. Do you have a proof for this?
 

Similar threads

  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 2 ·
Replies
2
Views
3K
Replies
1
Views
2K
  • · Replies 8 ·
Replies
8
Views
2K
  • · Replies 19 ·
Replies
19
Views
1K
  • · Replies 10 ·
Replies
10
Views
4K
  • · Replies 24 ·
Replies
24
Views
3K
  • · Replies 1 ·
Replies
1
Views
5K
  • · Replies 22 ·
Replies
22
Views
6K
  • · Replies 44 ·
2
Replies
44
Views
25K