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

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    Emergent space/time
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Discussion Overview

The discussion revolves around the concepts of emergent space and time in the context of AdS/CFT and dS/CFT correspondences. Participants explore the implications of these theories for understanding the nature of spacetime, particularly focusing on the differences between Lorentzian and Euclidean signatures, the role of conformal field theories (CFTs), and the potential for non-unitary theories.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Conceptual clarification

Main Points Raised

  • Some participants propose that while AdS/CFT is often described as emergent space, the emergence of time is also a possibility if the bulk geometry is pseudo-Riemannian, which has multiple timelike directions.
  • There is a suggestion that a non-unitary CFT could have a unitary renormalization group (RG) flow, although the meaning of this is not fully clarified.
  • One participant questions the implications of RG flow for CFTs, noting that once a theory flows from a fixed point, it may no longer be a CFT but a perturbation of it.
  • Another participant discusses the idea that the AdS radial dimension encodes behavior at different scales, but cautions against using the term "flow" in the context of conformal theories.
  • Speculation arises regarding the connection between unitarity in RG flow and operators with imaginary dimensions, suggesting that this could lead to a reinterpretation of RG time as real physical time.
  • A participant raises a question about what in the boundary theory determines the signature of the bulk geometry, noting the existence of Galilean boundary theories with Lorentzian bulk.
  • There is a mention of the classical distinctions between the conformal boundaries of de Sitter, anti-de Sitter, and Minkowski spaces, highlighting their different signatures.
  • Concerns are expressed about the validity of results in dS being derived from AdS through analytic continuation, with some participants noting that these results may be formal and problematic.

Areas of Agreement / Disagreement

Participants express a range of views on the nature of emergent space and time, the implications of RG flow, and the relationships between boundary and bulk theories. No consensus is reached, and multiple competing perspectives remain throughout the discussion.

Contextual Notes

Limitations include the unclear definitions of terms like "unitary RG flow," the unresolved implications of RG flow on CFTs, and the speculative nature of some claims regarding imaginary dimensions and their connection to physical time.

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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 [tex]\Delta[/tex], something not unfamiliar from non-unitary CFTs and other exotica. This way when you flow for an "RG time" T you find expressions like [tex]e^{\Delta T}[/tex] which now look more like unitary evolution if [tex]\Delta = i |\Delta |[/tex]. 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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