Lie Algebra Structure of 3-Sphere: Left Invariant Vector Fields

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Discussion Overview

The discussion centers on the Lie Algebra structure of the three-sphere (S^3), particularly in relation to left invariant vector fields and their connection to the Hopf fibration. Participants explore theoretical aspects, mathematical reasoning, and potential applications in physics, such as electron spin in quantum mechanics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant seeks to express the Lie Algebra structure of S^3 in terms of left invariant vector fields, specifically those tangent to or perpendicular to the fibers of the Hopf fibration.
  • Another participant identifies the Lie group structure of S^3 as SU(2) and mentions the 2:1 covering from SU(2) to SO(3) as relevant to the Hopf fibration.
  • A participant expresses confidence that breaking down the structure in terms of the Hopf fibration is feasible and relates it to electron spin in quantum mechanics.
  • One participant questions whether the basis of left invariant vector fields can determine a Riemannian connection on S^3, linking it to the Gauss curvature.
  • A later reply suggests that this inquiry may relate to the Berger metrics on S^3.

Areas of Agreement / Disagreement

Participants generally agree on the relevance of the Lie group structure and the Hopf fibration, but the discussion includes speculative questions and does not reach a consensus on the implications for Riemannian connections or Gauss curvature.

Contextual Notes

The discussion includes assumptions about the relationship between left invariant vector fields and Riemannian connections, as well as the applicability of the Berger metrics, which remain unresolved.

wofsy
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I know I should be able to look this up but am having trouble this morning.

I would like to know the Lie Algebra structure of the three sphere. In particular I'd like to express it in terms of the left invariant vector fields that are either tangent to the fibers of the Hopf fibration or perpendicular to it. By this I mean express the algebra in terms if an ortho-normal left invariant basis one of whose elements is tangent to the fiber circles of the Hopf fibration.
 
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The Lie group structure on S^3 is that of SU(2), so the Lie algebra of S^3 is su(2).

I don't know if this will help you get the explicit construction you're after, but there is a 2:1 covering SU(2) -> SO(3) from which one can obtain the Hopf fibration.
 
thanks that's very helpful

I think it won't be hard to break this out in terms of the Hopf fibration. In fact I think this is what they do when describing electron spin in quantum mechanics.

An aside question that I have is - can such a basis be viewed as determining a Riemannian connection on S3 when viewed as the unit circle bundle of a 2-plane bundle over the 2 sphere? If so, then the Lie algebra structure should tell me the Gauss curvature.

Thanks again.
 
Yes, I believe this would be a special case of the construction of the Berger metrics on S^3.
 

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