The classical limit of AdS/CFT

In summary, the classical limit of the two quantum theories is different. There is a correspondence between the corresponding classical theories, but it is not a perfect match.
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The AdS/CFT correspondence is a correspondence of one quantum theory to another quantum theory. But what about the classical limit of these two theories? Is there a correspondence between the corresponding classical theories? If there is, what a precise form this classical-to-classical correspondence takes?
 
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fzero commented on this in https://www.physicsforums.com/threa...-form-ways-it-could-fail.706159/#post-4479075. I don't understand it much, but here is his comment.

fzero said:
The bulk gravity is only ever classical in an extreme limit, but even so, the limit in which the rest of the theory is classical is actually different. Let's recall how parameters are related in the case of IIB on AdS5. The gauge theory ##N## is the 5-form flux and is related to the volume of the 5-sphere (which is in turn related to the AdS radius ##R##), so

$$N \sim ( M_P R)^4.$$

The limit in which gravity is classical is one in which the radius of curvature is large in Planck units, so this is the limit of large ##N## in the gauge theory.

The gauge theory coupling on the other hand is directly related to the string coupling

$$ g^2 N \sim g_s N \sim ( M_s R)^4,$$

where the last expression uses the relationship between the string scale, string coupling, and Planck scale. Stringy corrections, which include bulk scalar and gauge interactions, involve the string scale, rather than the Planck scale. So there is a range of values for the string coupling, where gravity is classical, but quantum string interactions are important.

In the limit where both $$N, g^2 N$$ are large, everything in the bulk is classical.
 
  • #3
Thanks atty, but I don't find in satisfying. For instance, one can certainly consider a classical gauge theory with small N (classical electrodynamics is an example), so I cannot accept the claim that classical limit is the large N limit. Indeed, the classical limit should be related to the Planck constant going to zero (in a suitable way), while the discussion above does not even mention the Planck constant.
 
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Related to The classical limit of AdS/CFT

1. What is the classical limit of AdS/CFT?

The classical limit of AdS/CFT refers to the regime in which the AdS/CFT correspondence between a conformal field theory (CFT) and anti-de Sitter space (AdS) becomes most accurate. This occurs when the curvature of AdS is large and the coupling constant of the CFT is small, resulting in a weakly coupled gravity theory.

2. What is the significance of the classical limit in AdS/CFT?

The classical limit is important because it allows for a simplified and more accurate understanding of the AdS/CFT correspondence. In this limit, the CFT can be described by a classical gravity theory in AdS, making it easier to make calculations and predictions.

3. How is the classical limit of AdS/CFT related to holography?

The classical limit of AdS/CFT is closely related to the holographic principle, which states that a higher dimensional theory can be described by a lower dimensional one. In this case, the classical limit allows for the CFT to be described by a classical gravity theory in a lower dimensional space, leading to the holographic description of the theory.

4. Can the classical limit of AdS/CFT be applied to other theories?

Yes, the classical limit of AdS/CFT can be applied to other theories that have a holographic dual description. This includes theories with different dimensions and symmetries, as long as they can be mapped onto AdS and have a classical limit.

5. Is the classical limit of AdS/CFT experimentally validated?

Currently, there is no direct experimental evidence for the classical limit of AdS/CFT. However, the correspondence has been extensively studied and shown to hold in many cases, providing strong theoretical support for its validity.

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