Horizon in AdS/CFT: CFT in Black Hole Spacetime

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Discussion Overview

The discussion revolves around the relationship between black hole spacetimes and conformal field theories (CFTs), particularly focusing on the location of the horizon in the CFT and the implications of a thermal CFT in the context of black holes. Participants explore theoretical frameworks, assumptions about thermal equilibrium, and the nature of states in quantum mechanics.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants question where the horizon is located in the CFT when considering a black hole spacetime.
  • There is a proposal that if a black hole corresponds to a thermal CFT, it implies the CFT exists in a box with an external universe providing temperature, although this is contested.
  • One viewpoint suggests that the black hole must be coupled to a heat bath to maintain a constant temperature, implying thermal equilibrium.
  • Another participant argues that the CFT is finite and unbounded, thus it does not require a heat bath, and posits that the entire CFT could be considered the horizon.
  • Concerns are raised about the implications of the CFT representing the whole universe being in a mixed state, questioning the consistency with quantum mechanics, which typically allows only pure states for the entire universe.
  • It is noted that in the context of eternal black holes, there are two copies of the CFT, and the black hole geometry may represent an entangled state of these CFTs, which appear thermal to each individually.

Areas of Agreement / Disagreement

Participants express differing views on the nature of the CFT in relation to black holes, particularly regarding the need for a heat bath and the implications of mixed versus pure states. The discussion remains unresolved with multiple competing perspectives presented.

Contextual Notes

Assumptions about thermal equilibrium and the nature of the universe's state are not fully explored, leaving open questions about the implications of these assumptions on the discussion.

atyy
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In a spacetime with a black hole, where is the horizon in the CFT?

Also, if a black hole spacetime corresponds to a thermal CFT, doesn't that mean the CFT is in a box where there is still a universe outside to provide a temperature?
 
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Hmm, here there are two copies of the CFT and one of them is averaged over.
http://arxiv.org/abs/hep-th/0106112
Eternal Black Holes in AdS
Juan M. Maldacena

I wonder if this has held up?

http://arxiv.org/abs/hep-th/9903237
AdS/CFT and the Information Paradox
D.A. Lowe, L. Thorlacius

http://arxiv.org/abs/0811.0263
Black Holes as Effective Geometries
Vijay Balasubramanian, Jan de Boer, Sheer El-Showk, Ilies Messamah

http://arxiv.org/abs/0909.1038
The information paradox: A pedagogical introduction
Samir D. Mathur
 
Last edited:
atyy said:
In a spacetime with a black hole, where is the horizon in the CFT?

Also, if a black hole spacetime corresponds to a thermal CFT, doesn't that mean the CFT is in a box where there is still a universe outside to provide a temperature?

You have to assume that the black hole is coupled to a heat bath such that the temperature remains constant and it's in thermal equilibrium. Then the black hole will remain at some temperature forever.


The CFT is finite and unbounded as is the horizon of the black hole. So the CFT isn't in a box since a box has bounds. Therefore the CFT doesn't need a heat bath because there is no where for the heat to flow from/to. So the whole CFT is the horizon.
 
Finbar said:
You have to assume that the black hole is coupled to a heat bath such that the temperature remains constant and it's in thermal equilibrium. Then the black hole will remain at some temperature forever.


The CFT is finite and unbounded as is the horizon of the black hole. So the CFT isn't in a box since a box has bounds. Therefore the CFT doesn't need a heat bath because there is no where for the heat to flow from/to. So the whole CFT is the horizon.

So if the CFT is the whole universe, then the universe will be in a mixed state - but how can that be - quantum mechanically, shouldn't there be only pure states when it comes to the whole universe?
 
atyy said:
So if the CFT is the whole universe, then the universe will be in a mixed state - but how can that be - quantum mechanically, shouldn't there be only pure states when it comes to the whole universe?

In the case of the eternal black hole discussed by Maldecena in your first link, there are actually two copies of the CFT. The black hole geometry is an approximate description of an entangled state of the two CFTs. This entangled state has the property that it looks exactly thermal to each CFT individually. Additionally, the CFTs are unable to communicate due to the black hole horizons.
 

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