Why do we need a theory of quantum gravity

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SUMMARY

A theory of quantum gravity is essential for reconciling general relativity with quantum mechanics, particularly in understanding phenomena such as black holes and the early universe. The discussion highlights the need for a quantum description of the stress-energy tensor, ##T_{\mu\nu}##, which currently relies on classical formulations. The challenge lies in transforming Einstein's equations, R_{\mu\nu}-\frac{1}{2}g_{\mu\nu} R = 8\pi T_{\mu\nu}, into a quantum framework where both sides of the equation are operators. Current approaches, such as quantum field theory on curved spacetimes, represent a step towards this goal but are not comprehensive.

PREREQUISITES
  • Understanding of Einstein's field equations in general relativity
  • Familiarity with quantum mechanics and the standard model of particle physics
  • Knowledge of quantum field theory and its applications
  • Concept of operators in quantum mechanics
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  • Research the implications of black hole thermodynamics in quantum gravity
  • Study the concept of quantum field theory on curved spacetimes
  • Explore the role of the stress-energy tensor in quantum gravity theories
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Physicists, cosmologists, and researchers interested in theoretical physics, particularly those focused on the intersection of quantum mechanics and general relativity.

MathJakob
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I've been wondering, why does the world need a theory of quantum gravity? What questions would be solved if such a theory was discovered?

What does a theory of quantum gravity mean for black holes, if anything?

Try to be quite indepth about the questions rather than something like "It will tell us what happened at t = 0" :P
 
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As you might know, Einsteins equations are
R_{\mu\nu}-\frac{1}{2}g_{\mu\nu} R = 8\pi T_{\mu\nu} \,\text{.}
##T_{\mu\nu}## is the stress-energy tensor of the matter content of the theory (electrons, quarks, gauge fields, ...). The problem is that the matter is described by a quantum theory (the standard model) and thus ##T_{\mu\nu}## should really be an operator ##\hat T_{\mu\nu}##. But if the right hand side is an operator, the left hand side should be an operator as well for the equation to make sense. Thus we try to find a quantum theory that describes the gravity part of the eqation.

You might ask: "Why don't we use ##\left<\hat T_{\mu\nu}\right>## for the right hand side?" People actually do this and it's called quantum field theory on curved spacetimes. It is expected to be a limiting case of the a full quantum theory.
 
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