Unveiling the Connection: Rotation Groups & Hyperspheres

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SUMMARY

The discussion centers on the isomorphism between the group of orthonormal rotations in n-dimensional space, denoted as SO(n), and the group of geodesic translations in a positively curved hypersphere of n(n-1)/2 dimensions. Tyger asserts that this relationship is intuitive yet underrepresented in existing literature. A specific example is provided for n=3, where SO(3) corresponds to geodesic translations on a sphere, highlighting the need for clarification regarding the definition of "geodesic translations" in this context.

PREREQUISITES
  • Understanding of rotation groups, specifically SO(n)
  • Familiarity with geodesic translations in differential geometry
  • Knowledge of hyperspheres and their dimensional properties
  • Basic concepts of isomorphism in mathematical groups
NEXT STEPS
  • Research the properties of SO(n) and its applications in physics
  • Explore the concept of geodesics in Riemannian geometry
  • Study the implications of isomorphism in mathematical structures
  • Investigate the role of hyperspheres in higher-dimensional geometry
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Mathematicians, physicists, and students of geometry interested in the relationships between rotation groups and geodesic translations in higher-dimensional spaces.

Tyger
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My first post, about rotation groups..

A result about rotation groups.

To me this seems clear, simple and very intuitive, but in all the papers and books I've read on the subject I have never seen it presented. Maybe some of you have seen it, or maybe it is new. It is very simple to state:

The group of orthonormal rotations in a space of n dimensions, SO(n) is isomorphic to the group of geodesic translations in a positively curved space (hypersphere) of n(n-1)/2 dimensions.
 
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Originally posted by Tyger
A result about rotation groups.

To me this seems clear, simple and very intuitive, but in all the papers and books I've read on the subject I have never seen it presented. Maybe some of you have seen it, or maybe it is new. It is very simple to state:

The group of orthonormal rotations in a space of n dimensions, SO(n) is isomorphic to the group of geodesic translations in a positively curved space (hypersphere) of n(n-1)/2 dimensions.

this is a nice thought. It may require a special clarification of what is meant by "group of geodesic translations" in order to make sense-----or this could be my private confusion and it is immediately understandable to everyone but me!

I think of the case n=3 where your theorem says
SO(3) is isomorphic to the geodesic translations of a sphere in 3 dimensions.
This seems right except that rotation around an axis is only a "geodesic translation" for points on the equator. So that one may have to extend the definition in some fashion.

Sorry about the vagueness, I just this moment saw your message and am replying directly.
 
Maybe I better clarify my statement

Choose any two points in a sphere of n(n-1)/2 dimensions, draw a geodesic from one point to the other. Every such geodesic can be mapped to a rotation in a space of n dimensions.
 

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