Does quantizing metric fields mean quantum gravity?

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Discussion Overview

The discussion revolves around the relationship between quantizing metric fields and the concept of quantum gravity. Participants explore various theories of quantum gravity, including String Theory and Loop Quantum Gravity (LQG), and examine the implications of canonical quantization in the context of gravitational fields.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants question whether the canonical quantization methods discussed in certain papers correspond to quantum gravity, suggesting that the metric field is not quantized.
  • Others argue that the introduction of creation and annihilation operators for gravitational perturbations indicates a quantum gravity framework.
  • A participant notes that the papers may be considering an effective field theory in a low-energy limit, raising questions about the non-renormalizable issues faced by different quantum gravity theories.
  • There is a discussion about whether different quantum gravity theories coincide in the low-energy limit, with some expressing uncertainty about the ability to derive such limits from existing theories.
  • One participant asserts that the belief in a massless spin-2 field as the low-energy limit of any valid quantum gravity theory is based on intuition rather than derivation.
  • Another participant clarifies that string theory does not exhibit ultraviolet divergences, contrasting it with the field theory of gravity, which is noted to be non-renormalizable due to such divergences.

Areas of Agreement / Disagreement

Participants express differing views on whether the discussed quantization methods relate to quantum gravity, with some asserting it does and others disagreeing. There is also uncertainty regarding the implications of low-energy limits across different quantum gravity theories, indicating a lack of consensus.

Contextual Notes

Limitations in understanding the low-energy limits of quantum gravity theories and the implications of non-renormalizability are noted, as well as the dependence on definitions of terms like "quantum gravity" and "effective field theory."

Haorong Wu
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TL;DR
In some papers, the gravitational field is canonically quantized. Does this lead to quantum gravity?
(I am not sure which forum this post belongs to. Hope someone kindly helps me move it to a proper forum.)

In papers, for example, here, here, and here, the authors start from the Lagrangian for matters and gravitational fields, then Dirac's constrained canonical quantization is used. They achieve annihilation and creation operators for gravitational perturbation.

I am not familiar with quantum gravity theories. I know there are several competing candidates, including String theory and LQG. These theories face different problems. Does this kind of canonical quantization belong to some of them, or it does not correspond to quantum gravity?

Thanks.
 
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This is not quantum gravity, in those papers metric field is not quantized. This is decoherence of quantum matter caused by classical gravitational interaction.
 
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@Demystifier. As in the first paper, Eqs. (23) and (24) introduce creation and annihilation operators ##b## and ##b^\dagger##. Well, I will copy from the paper

We express the quantized TT perturbations in terms of creation and annihilation operators $$\hat h_{ij}(x)=\sqrt {\frac 2 \kappa} \sum_r \int \frac {d^3k}{(2\pi)^3 \sqrt{2 \omega_k}} L^r_{ij}(k)(\hat b_r(k)e^{ikx}+\hat b^\dagger_r(k)e^{-ikx} )$$
I am confused because I only see creation and annihilation operators in quantum theory. And here, ##b## and ##b^\dagger## are operators for the gravitational field. The corresponding operators for the matter field are labeled by ##a## and ##a^\dagger##.

So these operators can be used on classical fields?
 
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You are actually right, in this paper it is quantum gravity. Sorry!
 
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Thanks, @Demystifier. No need to apologize.

I have gone through the papers again. It seems they are mainly considering an effective field theory in a low-energy limit. If I am correct, the non-renormalizable problem in String theory happens because of the ultraviolet divergence. I am not sure what problems are faced by the LQG theory. Some say that this theory will face a non-renormalizable problem as well when it takes classical limits.

Therefore, is this true that different quantum gravity theories coincide in the low-energy limit, and we can study quantum gravity in an effective field theory?
 
Haorong Wu said:
is this true that different quantum gravity theories coincide in the low-energy limit, and we can study quantum gravity in an effective field theory?
I'm not sure we even know what the low energy limit is of any quantum gravity theory, in the sense of actually being able to derive it. Most physicists appear to believe that any valid quantum gravity theory will have as its low energy limit the known quantum field theory of a massless spin-2 field, which was studied in the 1960s and 1970s and whose classical limit is known to be General Relativity. (This theory is also known to be non-renormalizable, but that is not an issue if we view it, as most physicists do, as an effective field theory that describes the low energy degrees of freedom.) However, I think that belief is based on physical intuition rather than any actual derivation from a quantum gravity theory such as string theory or LQG.
 
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Haorong Wu said:
If I am correct, the non-renormalizable problem in String theory happens because of the ultraviolet divergence.
No, in string theory there is no ultraviolet divergence. The non-renormalizability due to ultraviolet divergences is a feature of the field theory of gravity.
 
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Demystifier said:
No, in string theory there is no ultraviolet divergence. The non-renormalizability due to ultraviolet divergences is a feature of the field theory of gravity.
Oh, sorry. I must misunderstand an introductory talk about quantum gravity given by Hermann Nicolai.
 

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