Is General Relativity Really About Physics on Curved Spacetimes?

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Discussion Overview

The discussion revolves around the interpretation of General Relativity (GR) in relation to the concept of background spacetime, particularly in light of Carlo Rovelli's remarks on Loop Quantum Gravity (LQG). Participants explore the implications of GR being described as background independent and the challenges this poses to traditional understandings of spacetime in physics.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Technical explanation

Main Points Raised

  • Some participants reference Rovelli's assertion that GR is not about physics on curved spacetimes and argue that this contradicts the standard view of GR, which involves a curved spacetime background influenced by mass and energy.
  • Others suggest that the Minkowski metric is merely a particular solution within GR and not a fundamental background, indicating that all metrics in GR hold equal status.
  • There is a contention regarding the interpretation of "no background" in GR, with some arguing that Rovelli's perspective implies a complete absence of spacetime, while others clarify that it refers to the absence of a fixed background spacetime.
  • One participant expresses confusion over the terminology used in the discussion, noting that "background" seems to have different meanings for different contributors.
  • Some argue that the notion of spacetime as a fixed background is misleading and that GR should be understood as a theory where the geometry of spacetime is dynamic and evolves.
  • References to Lee Smolin's work are made, emphasizing the distinction between background-dependent theories, such as string theory, and background-independent theories like GR.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the implications of Rovelli's statements regarding background spacetime. There are multiple competing views on the interpretation of GR and its relationship to background independence, leading to an unresolved discussion.

Contextual Notes

Participants highlight the potential confusion arising from the term "background" and its implications in different theoretical frameworks. The discussion reflects varying interpretations of foundational concepts in GR and LQG, with no clear resolution on the definitions or implications of these terms.

  • #31
waterfall said:
So Hobba was right in the other thread we were discussing when he said ""Up to about the plank scale the assumption it is flat is fine, with gravitons making it behave like it had curvature or actually giving it curvature (we can't determine which) works quite well."

Yes, I think Hobba was right.
 
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  • #32
atyy said:
Yes, I think Hobba was right.

Ok. But there was something you said later in the thread that perplexed me. You said:

"BTW, although massless spin 2 can be equivalent to Einstein gravity in spacetimes that can be covered by harmonic coordinates (or similar), I don't think the reverse is true that the existence of a spin 2 field is sufficient to produce Einstein gravity.

Zhang and Hu, A Four Dimensional Generalization of the Quantum Hall Effect
Elvang and Polchinski, The Quantum Hall Effect on R^4

Bekaert et al, How higher-spin gravity surpasses the spin two barrier"

How could that be. You said massless spin 2 in harmonic coordintes can produce Einstein gravity, then you followed it immediately with the conflicting passage " I don't think the reverse is true that the existence of a spin 2 field is sufficient to produce Einstein gravity." But you just mentioned in the first sentence that it can! This has been perflexing me for a week so hope you can explain the context of what mean in your conflicting paragraph. Thanks.
 
  • #33
waterfall said:
Ok. But there was something you said later in the thread that perplexed me. You said:

"BTW, although massless spin 2 can be equivalent to Einstein gravity in spacetimes that can be covered by harmonic coordinates (or similar), I don't think the reverse is true that the existence of a spin 2 field is sufficient to produce Einstein gravity.

Zhang and Hu, A Four Dimensional Generalization of the Quantum Hall Effect
Elvang and Polchinski, The Quantum Hall Effect on R^4

Bekaert et al, How higher-spin gravity surpasses the spin two barrier"

How could that be. You said massless spin 2 in harmonic coordintes can produce Einstein gravity, then you followed it immediately with the conflicting passage " I don't think the reverse is true that the existence of a spin 2 field is sufficient to produce Einstein gravity." But you just mentioned in the first sentence that it can! This has been perflexing me for a week so hope you can explain the context of what mean in your conflicting paragraph. Thanks.

A chair can be made of wood, but not everything made of wood is a chair.
 
  • #34
atyy said:
A chair can be made of wood, but not everything made of wood is a chair.

Ok. So you mean full GR includes black holes dynamics *near* singularity which spin-2 field over flat spacetime doesn't cover. Good. Thanks for the clarification.
 
  • #35
waterfall said:
Ok. So you mean full GR includes black holes dynamics *near* singularity which spin-2 field over flat spacetime doesn't cover. Good. Thanks for the clarification.

Yes, that's true, but not what I meant. I meant that there may be spin 2 fields that produce "gravity" that is different from that of GR, even below the Planck scale.

http://arxiv.org/abs/1007.0435
 
  • #36
atyy said:
Yes, that's true, but not what I meant. I meant that there may be spin 2 fields that produce "gravity" that is different from that of GR, even below the Planck scale.

http://arxiv.org/abs/1007.0435

I actually read the paper above. It's talking about higher spin (more than 2) that produce "gravity" that is different from that of GR. It's not talking about spin 2.. so maybe you are mistaken above?

Also your analogy "A chair can be made of wood, but not everything made of wood is a chair." is not related to the above paper but as an answer to my other question, isn't it?
 
  • #37
atyy said:
Yes, that's true, but not what I meant. I meant that there may be spin 2 fields that produce "gravity" that is different from that of GR, even below the Planck scale.

http://arxiv.org/abs/1007.0435

I think what you meant was that since spin-3 or spin-4 describe GR. Then spin-2 describe "gravity" that is not 100% GR. This is very important to distinguish because it means spin-2 over flat spacetime is not equivalent to GR even those describe by harmonic coodinates.

The meaning of equivalent is "=". So when something is not matched 100%. They are not equal. So when you said before it is equivalent and later said spin-2 is not sufficient to produce GR. Then your statements conflict. Try to be consistent in descriptions especially when dealing with such complicated subject. Thanks.
 

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