Gauge formulation of gravitation theories. I. The Poincare, de Sitter, and conformal cases
The gauge formulations of various gravitation theories are discussed. They are based on the approach in which we have the group Diff R/sup 4/ acting on x/sup ..mu../ and in which we attach to every x/sup ..mu../ a tangent space with the group of action H. Group H does not act on x/sup ..mu../ and plays the role of an internal (global) symmetry group in the standard Yang-Mills theory. The matter fields in the theory transform according to representations of H and are assumed to be scalars of Diff R/sup 4/. The full invariance group of the Lagrangian is then of the form H/sup loc/xDiff R/sup 4/. Here H/sup loc/ is a local gauge group obtained from H exactly as in the Yang-Mills theory. The approach has two characteristic features: (i) The group H/sup loc/ must be spontaneously broken in order to exclude redundant gauge fields (the Lorentz connections) from the theory in a way covariant with respect to the gauge transformations. (ii) To different H there correspond different gravitational theories, all invariant under Diff R/sup 4/ but differing in backgrounds. Thus if H is isomorphic to the Poincare group the corresponding gauge theory turns out to be equivalent to the usual Einstein or Einstein-Cartan theory of gravity in the Minkowski space as a background. The other choices for H considered in the paper are the de Sitter groups and the conformal group. They yield the Einstein theory with a negative (or positive) cosmological term in the corresponding de Sitter space and the Weyl or Cartan-Weyl theory (depending on realization of the conformal group), respectively.
- Research Organization:
- Institute of Physics, Czechoslovak Academy of Sciences, Na Slovance 2, CS-180 40 Prague 8, Czechoslovakia
- OSTI ID:
- 5727028
- Journal Information:
- Phys. Rev. D; (United States), Vol. 25:4
- Country of Publication:
- United States
- Language:
- English
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