General covariance vs. locality

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SUMMARY

The discussion centers on the relationship between general covariance and locality in the context of quantum gravity, as presented by S. Carlip in the article arXiv:gr-qc/0108040v1. Carlip asserts that general covariance, or diffeomorphism invariance, is a fundamental symmetry of general relativity, which implies that physical quantities should not depend on coordinate choices. However, the discussion highlights that diffeomorphism-invariant observables are inherently nonlocal, as active coordinate transformations alter point positions and cannot maintain values defined at individual points.

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  • Understanding of general relativity and its principles
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  • Knowledge of diffeomorphism invariance
  • Basic grasp of observables in physics
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This discussion is beneficial for theoretical physicists, researchers in quantum gravity, and students of general relativity seeking to understand the complexities of locality and covariance in physical theories.

sadegh4137
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hi
i read an article by S.carlip about quantum gravity, arXiv:gr-qc/0108040v1 ,
in this article carlip stated:
why we need quantum gravity
what's problems of quantum gravity
and two ways of quantization of GR.

I couldn't realize some clues in section of "the problems of quantum gravity"
one of them is
General covariance vs. locality that Carlip stated:
The fundamental symmetry of general relativity is general covariance (strictly speaking, diffeomorphism invariance), the lack of dependence of physical quantities on the choice of coordinates. Observables in quantum gravity should presumably respect this symmetry . But diffeomorphism-invariant observables in general relativity are necessarily nonlocal , essentially because active coordinate transformations “move points” and cannot preserve a quantity defined, by its value at individual points.


I can't understand this phrase
is it possible to explain it for me.
thanks
 
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sadegh4137 said:
But diffeomorphism-invariant observables in general relativity are necessarily nonlocal, essentially because active coordinate transformations “move points” and cannot preserve a quantity defined, by its value at individual points.
No, I don't understand that remark either. Translations "move points", and so by this reasoning, translation invariance requires a nonlocal theory. :eek:
 

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