Yang Mills Theory of Gravity

Abstract

The canonical formulation of general relativity is based on decomposition space--time manifold $M$ into $R\times \Sigma$, this decomposition has to preserve the invariance of general relativity, invariance under general coordinates, and local Lorentz transformations. These symmetries associate with conserved currents that are coupled to gravity. In this paper, we try to solve the equations of motion of general relativity in self-dual formalism using only the spin currents(Lorentz currents), in static case, and without needing using the Einstein's equation, that makes the general relativity similar to Yang-Mills theory of gauge fields. We give an example, matter located at a point, so we have spherical symmetric system. Then we add Yang--Mills Lagrangian to general relativity Lagrangian. Finally we use the decomposition of the space--time manifold $M=R\times \Sigma$ to find that ${\Sigma }_i^{0a}$ is a conjugate momentum of $A_a^i$ and ${\Sigma }_i^{ab}{F}_{ab}^i$ is energy density.

v2 includes some corrections to the published paper

References in corpus (6)

• The five-loop beta function of Yang-Mills theory with fermions
• Loop expansion and the bosonic representation of loop quantum gravity
• Reformulation of the symmetries of first-order general relativity
• One-Loop Renormalization of Non-Abelian Gauge Theory and βFunction Based on Loop Regularization Method
• Consistent matter couplings for Plebanski gravity
• Loop Representation of Wigner's Little Groups