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Ashtekar Connection
Linked via "Yang-Mills theories"
The Ashtekar connection (Ashtekar-Barbero connection), also formally known as the Ashtekar-Barbero connection in its most common formulation, is a crucial component in the canonical quantization program for general relativity (GR). Introduced by Abhay Ashtekar in the early 1980s, this mathematical structure reformulates general relativity in terms of variables conceptually analogous to those used in Yang-Mills theories, facilitating …
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Ashtekar Formulation
Linked via "Yang-Mills theory"
This variable is an $\mathbb{R}^3$-valued vector density, representing the spatial geometry analogously to the electric field in electromagnetism.
This transformation converts the complex, non-polynomial Hamiltonian of GR into a structure strongly resembling Yang-Mills theory, characterized by constraints that behave like Gauss's law and the conservation of momentum/energy in a gauge theory.
Constraint Equations in the Ashtekar Formalism -
Diffeomorphism Invariance
Linked via "Yang-Mills theory"
Constraints in Ashtekar Variables
When using the Ashtekar variables (the Ashtekar connection $A^ai$ and the triad) $E^ai$), the structure of the constraints simplifies significantly, resembling Yang-Mills theory constraints, although the physical meaning remains rooted in spacetime geometry:
| Constraint | Canonical Variables $(A^ai, E^ai)$ | Physical Interpretation | -
Gauge Structure
Linked via "Yang-Mills quantization techniques"
Gauge Structure in Gravity
While the Standard Model is built upon non-Abelian gauge theories, General Relativity (GR) is fundamentally built upon diffeomorphism invariance—a general coordinate transformation symmetry. While often treated separately, attempts to formulate quantum gravity using gauge theory principles often involve treating the metric field or related … -
Gauss Constraint
Linked via "Yang-Mills theory"
Physical Interpretation and Role
The Gauss constraint dictates that the connection $\mathcal{A}$ must be compatible with the triad $E$ under local gauge rotations in the internal $\mathfrak{su}(2)$ space. If the system were viewed purely as a Yang-Mills theory, the Gauss constraint would enforce that the "charge density" associated with the Ashtekar connection vanishes everywhere.
A key aspect of the [Gauss constraint](/entries/gauss-co…