How Are Maurer-Cartan Forms Utilized in Physics?

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Discussion Overview

The discussion centers on the application of Maurer-Cartan one-forms in physics, particularly in the context of Lie groups and their associated geometries. Participants explore how these forms relate to constructing metrics for spaces with symmetries described by Lie groups and their implications in physical theories.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant seeks to understand the role of Maurer-Cartan one-forms, suggesting they may help construct metrics for symmetric spaces.
  • Another participant emphasizes the importance of parallelism on the group manifold as fundamental to the discussion.
  • A later reply clarifies that the Maurer-Cartan form can be used to create vector fields on the group, establishing global parallelism and defining a globally flat affine connection with specific properties.
  • There is a mention of the complexity of the geometry of homogeneous spaces G/H compared to the group itself, with an example provided of the two-sphere as a case study.
  • A reference is shared for further reading on the use of Maurer-Cartan forms in the context of homogeneous spaces.

Areas of Agreement / Disagreement

Participants express various viewpoints on the utility of Maurer-Cartan forms, with some focusing on their role in parallelism and vector fields, while others highlight the complexities involved in applying these concepts to homogeneous spaces. No consensus is reached on a singular application or interpretation.

Contextual Notes

The discussion reflects uncertainties regarding the implications of Maurer-Cartan forms in physical applications, particularly in relation to the geometry of homogeneous spaces and the conditions under which these forms are utilized.

haushofer
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Hi,

I'm trying to understand the use of Maurer-Cartan one-forms in physics. As far as I understand it's a Lie-algebra valued one-form which sends vectors at an arbitrary point g on the Lie-group to the identity e (the Lie algebra). But my question is: what is the use of these things in physics? I have the feeling that somehow they let you construct metrics for spaces with symmetries described by the Lie-group in question, but can someone elaborate on this or give some references where people explain this?
 
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More fundamental than the invariant metric is the parallelism of the group manifold.
 
Could you be a bit more specific? :)
 
Call the Maurer-Cartan form \omega. Take a given vector \xi in the Lie algebra of the group. At each point g of the group there is a unique tangent vector \xi_p with the property that \omega(\xi_p)=\xi.. This way you create vector fields on the group - one vector field for each element of the Lie algebra. This defines global parallelism. You can compare tangent vectors at a distance by requiring that \omega has the same value on both vectors. It defines globally flat affine connection on the group manifold - it has vanishing curvature, but non-vanishing torsion.
 
Ok, that's clear. And how does this manifest itself in physics? "Given a Lie algebra, one can construct the corresponding space with that isometry" or something?
 
In physics we are usually dealing with homogeneous spaces G/H. Their geometry is more complicated than that of the group itself, though geometry of G plays a role there too. The first nice example to look at is the two-sphere, the homogeneous space SO(3)/SO(2). It has an invariant metric, but it is not parallelizable.
For a use of Maurer-Cartan forms within the framework of homogeneous space you may like to check http://books.google.fr/books?id=zGp...&q="cartan-maurer" homogeneous space&f=false".
 
Last edited by a moderator:
Thanks for that link! I will definitely check it, and if I have more questions I'll come back! :)
 

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