Transition Functions and Lie Groups

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SUMMARY

The discussion focuses on the role of transition functions in the context of Lie groups and fiber bundles, emphasizing that these functions are essential for gluing local coordinate charts together on Riemannian manifolds. It clarifies that Jacobian matrices, derived from coordinate transformations, are not the same as the transformations themselves. The conversation highlights the necessity of local coordinate charts even in flat manifolds and the additional structures provided by Lie groups that facilitate this process.

PREREQUISITES
  • Understanding of Riemannian manifolds
  • Familiarity with Jacobian matrices and their role in coordinate transformations
  • Basic knowledge of Lie groups
  • Concept of fiber bundles in differential geometry
NEXT STEPS
  • Research the properties of Lie groups and their applications in geometry
  • Study the concept of fiber bundles and their significance in topology
  • Explore the relationship between Jacobian matrices and coordinate transformations in detail
  • Learn about local coordinate charts and their role in manifold theory
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Mathematicians, physicists, and students of differential geometry who are interested in the interplay between transition functions, Lie groups, and fiber bundles.

knowwhatyoudontknow
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I understand that on Riemannian manifolds, the transition functions that glue charts together are coordinate transformations (Jacobian matrices).

However, I am not quite sure how transition functions work in the context of Lie groups and Fiber bundles. Do we consider the manifolds to be flat and glue the charts together with elements of the Lie group whose actions represent coordinate translations?

On the other hand, if the manifold is flat, why do we need to consider more than a single chart?
 
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knowwhatyoudontknow said:
I understand that on Riemannian manifolds, the transition functions that glue charts together are coordinate transformations (Jacobian matrices).
Just to be clear, a Jacobian matrix is not a coordinate transformation. It is built from the first derivatives of a coordinate transformation.

knowwhatyoudontknow said:
However, I am not quite sure how transition functions work in the context of Lie groups and Fiber bundles.
The same as any other manifold. You need to introduce local coordinate charts and glue them together. The particular thing with those is that they have some additional structure that may help you do that.
 
Yes, I realize my error regarding the Jacobian matrices. I confused coordinate transformations with how functions change under a change of coordinates. This makes better sense now. Thanks.
 

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