Conservation of energy-momentum of matter as the basis for the gauge theory of gravitation
Friedrich W. Hehl, Yuri N. Obukhov

TL;DR
This paper explores the gauge theory of gravity based on energy-momentum conservation, extending from translation invariance to the full Poincaré group, and reviews the Einstein-Cartan theory and its potential developments.
Contribution
It extends the gauge approach to gravity by incorporating the full Poincaré group, including angular momentum, building on the Einstein-Cartan framework.
Findings
The theory is equivalent to general relativity with torsion.
Gauging the full Poincaré group leads to a richer gravitational theory.
Potential for further theoretical developments in gravitational gauge theories.
Abstract
According to Yang \& Mills (1954), a {\it conserved} current and a related rigid (`global') symmetry lie at the foundations of gauge theory. When the rigid symmetry is extended to a {\it local} one, a so-called gauge symmetry, a new interaction emerges as gauge potential ; its field strength is . In gravity, the conservation of the energy-momentum current of matter and the rigid translation symmetry in the Minkowski space of special relativity lie at the foundations of a gravitational gauge theory. If the translation invariance is made local, a gravitational potential arises together with its field strength . Thereby the Minkowski space deforms into a Weitzenb\"ock space with nonvanishing torsion but vanishing curvature. The corresponding theory is reviewed and its equivalence to general relativity pointed out. Since…
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