The classical limit of AdS/CFT

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SUMMARY

The discussion centers on the classical limit of the AdS/CFT correspondence, specifically the relationship between classical theories in this framework. It is established that bulk gravity remains classical only in an extreme limit where the radius of curvature is large in Planck units, corresponding to a large N limit in the gauge theory. The gauge theory coupling is directly related to the string coupling, with specific relationships outlined as $$N \sim (M_P R)^4$$ and $$g^2 N \sim g_s N \sim (M_s R)^4$$. The conversation highlights the complexity of classical limits and the importance of stringy corrections, emphasizing that classical behavior in the bulk occurs when both $$N$$ and $$g^2 N$$ are large.

PREREQUISITES
  • Understanding of AdS/CFT correspondence
  • Familiarity with gauge theories and their parameters
  • Knowledge of string theory concepts, including string coupling
  • Basic grasp of Planck units and their significance in theoretical physics
NEXT STEPS
  • Research the implications of large N limits in gauge theories
  • Study the relationship between string coupling and gauge theory coupling
  • Explore the role of Planck units in quantum gravity theories
  • Investigate classical gauge theories and their properties in the context of AdS/CFT
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The discussion is beneficial for theoretical physicists, particularly those specializing in quantum field theory, string theory, and the AdS/CFT correspondence, as well as researchers exploring the classical limits of these frameworks.

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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.
 
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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