Second-Order Graviton Propagator in Rovelli-Smolin's Loop Quantum Gravity

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Discussion Overview

The discussion revolves around the second-order graviton propagator in the context of Rovelli and Smolin's work on Loop Quantum Gravity (LQG). Participants explore the implications of this propagator, its relation to perturbative quantum gravity, and the role of the parameter lambda in the Barret-Crane model.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant suggests that the second-order in the lambda constant in the Barret-Crane model may be analogous to second-order perturbation theory in linear quantum gravity, raising questions about renormalization.
  • Another participant recommends a non-technical paper by Smolin that summarizes current developments in the field, indicating its accessibility for those with limited time.
  • A different participant points to a blog post by Lubos Motl, implying that it may provide additional insights or critiques regarding the topic.
  • One participant argues that if one approaches LQG through the lens of perturbative quantum field theory on classical backgrounds, it may not be a coherent framework.
  • The role of the lambda parameter in the group field method is mentioned, with uncertainty expressed about its meaning and how it relates to the detail of the expansion.

Areas of Agreement / Disagreement

Participants express differing views on the interpretation of the second-order graviton propagator and the implications of the lambda parameter, indicating that multiple competing perspectives remain without consensus.

Contextual Notes

Some participants note limitations in their understanding due to time constraints and the complexity of the subject matter, which may affect the depth of their contributions.

Sauron
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I have finished a quick first reading of the rovelli at all paper ingraviton propagator http://arxiv.org/gr-qc/0604044

I couldn´t dive too much into the details because spin foams was a prerequisite and i only could do an equally fast reading of the alejandro perez review of the subjecto (i am tourning into the math exams now and i have less time for LQG).

But still with these porr knowledge i guess an aspecto is not trated as deep as it deserves in these articles.

I men,they get second order in a [tex]\lamdba[\tex] constant which appears in the Barret-Crane model, that is, it multiplies te "interaction" term. I didn´t see it firmly stablished but i guess that is somewhat equivalent to a second order in a series in the usual gravity G constant.That is, second order of perturbation theory in linear perturbative quantum gravity.<br /> <br /> If these is true these would mean that they second order graviton propagator would correspond to the renormalized (loosely speaking) second order graviton propagator of the "naive" linear quantum gravity, isn´t it?<br /> <br /> That would be a mayor succes because, as it is well known, linear quantum gravity isn´t renormalizable. So LQG would be, among other things, a way of ding renormalization in linear quantum gravity (i can´t brief it because it also would be LQG <img src="https://cdn.jsdelivr.net/joypixels/assets/8.0/png/unicode/64/1f644.png" class="smilie smilie--emoji" loading="lazy" width="64" height="64" alt=":rolleyes:" title="Roll Eyes :rolleyes:" data-smilie="11"data-shortname=":rolleyes:" />).<br /> <br /> Of course one of the mayor claims of loop QG is that you don´t need renormalization because it provides a natural cut´.off and et, etc. <br /> <br /> As i said these doubt come from an inadequate fast rading. Hope not too disturb people if i made a too stupid question.[/tex]
 
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Sauron said:
(i am tourning into the math exams now and i have less time for LQG)...

good luck with the math exams, Sauron!

since you have little time for reading right now, I will suggest a paper by Smolin that gives a brief non-technical description of Rovelli's graviton work.

http://arxiv.org/hep-th/0605052

I am finding this Smolin paper gives a helpful survey of current developments that is easy to read, and picks out the most important developments, and is intuitive without many equations.

Look on page 12, for a paragraph about Rovelli's graviton work
and also a paragraph about Loll triangulations.
It can be interesting to see these things through Smolin's eyes, as he looks at research of other people in the field of Loop-and-allied gravity and tries to understand the significance.

when will your exams be finished?
 
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I apologize in advance, but you might want to check Lubos' blog

http://motls.blogspot.com/2006/04/carlo-rovelli-and-graviton-propagator.html"
 
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Motl demonstrates one thing clearly: If you think in terms of perturbative QFT on around classical backgrounds LQG doesn't make sense.

As for lambda, this parameter arises in the group field method to generate spinfoam state sums. The order in lambda should correspond to the amount of detail you are resolving in your expansion. Last I heard (but I'm definitely not up to speed on this) the meaning of this parameter was not clear.
 

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