Fiber Bundle Basics: An Overview of Penrose's Twisted Bundles

Click For Summary

Discussion Overview

The discussion centers on the concept of fiber bundles as introduced by Roger Penrose, particularly focusing on the differences between trivial bundles and twisted bundles, such as the Möbius strip. Participants explore the implications of these structures in terms of orientation, cross-sections, and the topology of the bundles.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants clarify the notation used for fiber bundles, defining B as the base space, F as the fiber, and E as the total space.
  • One participant expresses confusion about the concept of "twisted" in the context of fiber bundles, particularly how it relates to the Möbius strip.
  • Another participant introduces the idea of a connection in fiber bundles, explaining its role in defining parallel transport and the orientation of fibers.
  • Some participants discuss the notion of global versus local orientation in fiber bundles, noting that a Möbius strip cannot support a global orientation due to its topology.
  • There is a mention of bundle isomorphism and how it relates to the distinction between trivial and twisted bundles.
  • Participants explore the concept of cross-sections in both trivial and twisted bundles, questioning how continuity is maintained in the twisted case.
  • One participant emphasizes that fibers are "glued together" by the topology of the total space, which imposes a notion of nearness among them.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the implications of twisted bundles, with some agreeing on the definitions and concepts while others remain uncertain about specific aspects, such as orientation and continuity in twisted cases. The discussion does not reach a consensus on these points.

Contextual Notes

Participants note that the definitions and properties of fiber bundles depend on the topology imposed on the total space, and that local trivializations play a crucial role in understanding continuity and orientation. The discussion highlights the complexity of these concepts without resolving the underlying uncertainties.

  • #31
quasar987 said:
I'm trying to read another meaning into what you wrote, but it really looks like you're saying that every rank 1 vector bundle is trivial, which is of course false.

What are you saying here?

I have to think about it. Quite possible I was wrong. E\otimes E is then trivial.
 

Attachments

  • deiudonne83.jpg
    deiudonne83.jpg
    17.6 KB · Views: 497
Last edited:
Physics news on Phys.org
  • #32
Rasalhague said:
(By the way, Penrose is talking about a slightly different pair of shapes, where F is the R1 vector space, rather than just a finite interval of it.)
I haven't followed the thread so I don't know if it's relevant, but topologically R1 and a finite (open) interval are homeomorphic spaces.
 
  • #33
@quasar987
Thanks. Now I remember: the story was that in real vector bundles there is always a global cross section, but not that it is nowhere vanishing. Next time I will check better before posting anything.
 
  • #34
arkajad said:
I have to think about it. Quite possible I was wrong. E\otimes E is then trivial.

Well, the topic of the thread is the Mobius bundle, which is a nontrivial rank 1 vector bundle over the circle. Also, the tautological line bundle over RP^n is another example of a nontrivial rank 1 bundle over RP^n that has also been mentioned by lavinia earlier.

I do not see the relevance of the lemma you quote. It talks about the possibility of extending globally a locally extendable section defined on a closed set. But it does not say that the extension will be nonvanishing outside of the closed set S...so I don't see why it is relevant.
 
  • #35
arkajad said:
@quasar987
Thanks. Now I remember: the story was that in real vector bundles there is always a global cross section, but not that it is nowhere vanishing. Next time I will check better before posting anything.

No problem! I am too often guilty of that myself. :-p
 
  • #36
If I understand this characteristic class stuff, then it also seems that the tangent bundle of the 2 sphere can not have a 1 dimensional subbundle. For if so the tangent bundle would decompose into a Whitney sum of two line bundles and each would have zero Euler class because the sphere is simply connected. The Whitney sum formula for the Euler class would then imply that the Euler class of the 2 sphere is also zero which can not be because its Euler characteristic is 2.

More generally from the same kind of reasoning, it would seem that the tangent bundle of an even dimensional sphere does not have any proper subbundle.

I think that Arkajad was thinking that the Whitney sum of the Mobius line bundle over the circle is trivial. In this bundle, parallel translation around the circle brings a vector back to its negative. So one can not get a section through parallel translation, I guess. However, if one allows the vector to rotate 180 degrees as one moves around the circle once, you get a section. What does this mean about the bundle?
 

Similar threads

  • · Replies 10 ·
Replies
10
Views
4K
  • · Replies 15 ·
Replies
15
Views
5K
  • · Replies 7 ·
Replies
7
Views
4K
  • · Replies 15 ·
Replies
15
Views
4K
  • · Replies 26 ·
Replies
26
Views
1K
  • · Replies 11 ·
Replies
11
Views
4K
  • · Replies 6 ·
Replies
6
Views
3K
  • · Replies 16 ·
Replies
16
Views
5K
  • · Replies 3 ·
Replies
3
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K