Emergent Space/Time: AdS/CFT and dS/CFT

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    Emergent space/time
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SUMMARY

The discussion centers on the complexities of the AdS/CFT and dS/CFT correspondences, particularly the emergence of time in pseudo-Riemannian geometries. It highlights that while AdS space is often considered emergent, the understanding of time's emergence remains ambiguous. The conversation emphasizes the need for a non-unitary conformal field theory (CFT) with unitary renormalization group (RG) flow, suggesting that the boundary theory's properties may not dictate the bulk geometry's signature. Key references include arXiv papers on the subject, indicating ongoing research and speculation in this area.

PREREQUISITES
  • Understanding of AdS/CFT and dS/CFT correspondences
  • Familiarity with conformal field theories (CFTs)
  • Knowledge of renormalization group (RG) flow concepts
  • Basic principles of pseudo-Riemannian geometry
NEXT STEPS
  • Research the implications of non-unitary CFTs in quantum gravity
  • Study the role of RG flow in conformal field theories
  • Examine the differences between Euclidean and Lorentzian signatures in AdS and dS spaces
  • Explore the analytical continuation techniques between AdS and dS results
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The discussion is beneficial for theoretical physicists, particularly those specializing in quantum gravity, string theory, and the study of conformal field theories. It also serves as a resource for researchers exploring the implications of spacetime geometry in high-energy physics.

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https://www.physicsforums.com/showpost.php?p=3263502&postcount=94
mitchell porter said:
At the moment, it only works properly for an emergent AdS space, but if the dS/CFT correspondence can be understood, then this will be true for spaces of positive curvature as well. (In dS/CFT the boundary is purely spacelike and lies in the infinite past and future, rather than being timelike as in AdS/CFT, so it's as if the timelike direction in the Lorentzian gravitational space is emerging from Euclidean field theory on a sphere in the infinite past.)

Actually, thinking even about AdS/CFT which is commonly said to be emergent space, but not emergent time, if the bulk geometry is pseudo-Riemannian, which has multiple timelike directions at each point, shouldn't time emerge too?
 
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I think one wants a non-unitary CFT that has a unitary renormalization group flow. Whatever that means.
 
What, what, what? :smile: Can a layman get an explication?
 
See http://arxiv.org/abs/hep-th/0106113" . "In general the dual CFT may be non-unitary". But we want, or we think we want, the bulk theory to be unitary, and since it is defined by RG flow in the "RG space" of the boundary CFT, PM wants "unitary RG flow" in that space. Ultimately it may not be the right way to put it, but I know what he's saying.
 
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mitchell porter said:
See http://arxiv.org/abs/hep-th/0106113" . "In general the dual CFT may be non-unitary". But we want, or we think we want, the bulk theory to be unitary, and since it is defined by RG flow in the "RG space" of the boundary CFT, PM wants "unitary RG flow" in that space. Ultimately it may not be the right way to put it, but I know what he's saying.

A CFT sits a a fixed point(its scale invariant) by definition so presumably once one flows from the fixed point the theory is no-longer a CFT but some perturbation of it in a relevant direction??
 
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That thought was bothering me even as I wrote. I guess that for both conformal and nonconformal boundary theories, the AdS radial dimension encodes behavior at different scales, but for the conformal case, one shouldn't speak of "flow".
 
Of course it is true that a CFT doesn't itself flow, but it does have a spectrum of operators and controls the flow in its vicinity. In any event, my statement was colloquial and meant for pure amusement.

Unitarity in the RG flow is a strange thing. I would expect it to be connected to operators with imaginary dimension \Delta, something not unfamiliar from non-unitary CFTs and other exotica. This way when you flow for an "RG time" T you find expressions like e^{\Delta T} which now look more like unitary evolution if \Delta = i |\Delta |. Hence RG time becomes real physical time!

I think this is well known wild speculation, but it is not much more than that right now.
 
Thanks guys! Actually, I was thinking of something presumably simpler. Lorentzian spacetimes have "time" or "times" that Riemannian spacetimes don't. In AdS/CFT, what in the boundary theory determines the signature of the bulk geometry?

Papers like http://arxiv.org/abs/0804.3972 and http://arxiv.org/abs/0804.4053 seem to have Galilean boundary theories with Lorentzian bulk, so I presume it isn't the signature of the boundary that determines the bulk signature? (Or is this some weird thing that condensed matter folks do that "real" string theorists wouldn't contemplate?)
 
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  • #10
Just speaking classically, de Sitter space has a spacelike conformal boundary, anti de Sitter has a timelike conformal boundary, and Minkowski space has a lightlike conformal boundary. (When I say the AdS boundary is timelike, I mean it has a timelike direction - it has spacelike directions too.) Also, of course, the bulk theories all have Lorentzian signature, classically.

I read somewhere that results in AdS can sometimes be analytically continued to results in dS by way of working in Euclidean signature in the AdS boundary theory, but the dS "results" had problems as usual - maybe they were purely formal expressions; I forget the details.
 

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