How Are Maurer-Cartan Forms Utilized in Physics?

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SUMMARY

Maurer-Cartan one-forms are Lie-algebra valued one-forms that map vectors at a point on a Lie group to the identity in the Lie algebra. They are crucial in constructing metrics for spaces with symmetries described by the Lie group, enabling the definition of global parallelism on the group manifold. This parallelism allows for the comparison of tangent vectors and results in a globally flat affine connection with vanishing curvature but non-vanishing torsion. An example of their application is in the geometry of homogeneous spaces, such as the two-sphere represented by SO(3)/SO(2).

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  • Understanding of Lie groups and Lie algebras
  • Familiarity with differential geometry concepts
  • Knowledge of affine connections and curvature
  • Basic principles of homogeneous spaces in physics
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  • Study the construction of metrics on homogeneous spaces G/H
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  • Investigate the implications of non-vanishing torsion in affine connections
  • Read about the geometry of the two-sphere and its relation to SO(3)/SO(2)
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Physicists, mathematicians, and researchers interested in differential geometry, particularly those focusing on the applications of Lie groups and homogeneous spaces in theoretical physics.

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".
 
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Thanks for that link! I will definitely check it, and if I have more questions I'll come back! :)
 

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