Schwinger-Dyson equations for Quantum Gravity

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SUMMARY

The discussion centers on the application of Schwinger-Dyson equations to Quantum Gravity (QG), specifically addressing the functional expression for Z[J] and its implications for Einstein's equations. The equations presented, particularly R_{a,b}( -i \frac{ \delta Z (J)}{\delta J}) + J(x)Z(J) = 0, highlight the complexity of solving these equations numerically, especially in the context of non-renormalizability. Participants express skepticism about the viability of this approach due to issues with fluctuating metrics and the potential for uncontrolled blow-ups in calculations. The conversation also touches on the mapping of functional derivative expansions to Feynman diagrams.

PREREQUISITES
  • Understanding of Schwinger-Dyson equations
  • Familiarity with functional derivatives in quantum field theory
  • Knowledge of Einstein's equations in general relativity
  • Concept of non-renormalizability in quantum gravity
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  • Research numerical methods for solving Schwinger-Dyson equations
  • Explore perturbative and non-perturbative expansions in quantum field theory
  • Study the implications of fluctuating metrics in quantum gravity
  • Investigate the relationship between functional derivatives and Feynman diagrams
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Physicists, quantum field theorists, and researchers focused on the intersection of quantum mechanics and general relativity, particularly those exploring solutions to quantum gravity challenges.

mhill
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using the Schwinger Dyson equations that gives us a differential expression for the functional Z[J] so Z[0] is just the path integral over 4-dimensional spaces .then for Einstein equation (no matter) they read (system of 10 functional equations)

R _{a,b}( -i \frac{ \delta Z (J)}{\delta J})+ J(x)Z(J)=0

then let's suppose we had a super-powerfull computer so we could solve these S-D equations Numerically could it be a solution to the problem of QG ?? , in fact could someone say me what methods are used to solve these kind of equations with functional derivatives ?? .. if possible in the perturbative and Non-perturbative expansions, thanks
 
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Well the functional derivative expansion maps directly into an expansion onto Feynman diagrams. But the expression you have written will probably blow up due in an uncontrollable way due to non-renormalizability. Also, R_{ab} is a function of position on that manifold, but position is only meaningful for a particular metric. If the metric itself is fluctuating, what exactly is the meaning of your equation then? I don't think this is the way to go about quantum gravity. What is Z[0]?
 

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