Can Gravity Be Understood as a Gauge Theory Through Rovelli's LQG Approach?

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SUMMARY

This discussion confirms that gravity can be understood as a gauge theory through the lens of Rovelli's Loop Quantum Gravity (LQG) approach. The Einstein Lagrangian can be expressed using the gauge fields \( A_{\mu}^{I}(x) \) and their associated field strength \( F_{ab}^{I} \). The formulation introduces an additional independent field, the tetrad, which corresponds to the metric tensor, leading to two sets of equations of motion: the Einstein equations and a relationship between the connection \( A \) and the metric derivatives. This framework also accommodates the Einstein-Cartan theory of gravity, which incorporates geometry with torsion in the presence of matter with spin.

PREREQUISITES
  • Understanding of Gauge Theories
  • Familiarity with Loop Quantum Gravity (LQG)
  • Knowledge of the Einstein Lagrangian and Field Equations
  • Concept of Tetrads and their role in General Relativity
NEXT STEPS
  • Study the mathematical formulation of Gauge Theories in detail
  • Explore Rovelli's works on Loop Quantum Gravity for deeper insights
  • Investigate the implications of the Einstein-Cartan theory of gravity
  • Learn about the relationship between geometry and torsion in gravitational theories
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Physicists, researchers in theoretical physics, and students of general relativity who are interested in advanced concepts of gravity and gauge theories.

Klaus_Hoffmann
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GR as a Gauge theory ??

don't know if this is true or not, but i have been reading books by ROvelli (LQG) or 'Gauge theories' the question is could we study Gravity as the set of functions A_{\mu}^{I}(x)

Then we write the Einstein Lagrangian (or similar) as:

\mathcal L = F_{ab}^{I}F^{I}_{ab} (sum over I=0,1,2,3)

F_{ab}= \partial _{a}A^{I}_{b}-\partial _{b}A^{I}_{a}-\Gamma_{jk}^{i}A_{j}^{I}(x) A_{k}^{I}(x)

I think Rovellli in his LQG theory used this representation... then (\partial_{0}A_{\mu}^{I} is the Kinetic part of Lagrangian and

dA_{\mu}^{I} (d- exterior derivative) represents the potential.

then how would it read the Einstein Field equation and the Riemann or similar tensors ??
 
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Yes, you can formulate gravity in that way. However, then the Lagrangian is not quadratic in F, but linear in F. In addition, you have one additional independent field - the tetrad (corresponding to the metric tensor itself), which does not have an analog in Yang-Mills theories. Having two independent fields, you obtain two set of equations of motion. One is the Einstein equation, while the other is a relation between the connection A and the metric derivatives. In the absence of matter, this relation is the same as in GR. In the case of matter with spin, the connection gets additional terms, describing geometry with torsion. This is the so-called Einstein-Cartan theory of gravity.
 

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