Metric of n-sheeted AdS_3: Constructing BTZ

In summary, the AdS_3 metric is a three-dimensional space with a specific mathematical formula. The n-sheeted space of this metric is defined as a manifold M_n that is n times folded cover of a boundary M_1. The bulk solution of this n-sheeted space is the n-sheeted BTZ, which can be constructed from the AdS_3 metric by making n identifications. The definition of an n-sheeted space is not precisely known, but it involves taking n copies of a boundary, cutting them apart, and gluing them in a cyclic order. The BTZ solution can also be expressed in a mathematical formula, and the n-sheeted BTZ can be written as a modified version of it.
  • #1
craigthone
59
1
suppose the AdS_3 metric is given by
$$ds^2 =d\rho^2+cosh^2\rho d\psi^2 +sinh^2 \rho d\phi^2$$
what is the n-sheeted space of it? Can the n-sheeted BTZ be constructed from it by identifications as n=1 case?

Thanks in advance.
 
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  • #2
Maybe you should give the definition of an n-sheeted space here to get more responses.
 
  • #3
About n-sheeted space, I do not know the precise defination. I will give some introductions.
consider a 3-dimensional space B_1 whose boundary is M_1. Then the manifold M_n is defined as n-folded cover of M_1: taking n copies of M_1, cutting each of them apart at a region A, and gluing them in cyclic order. Then the bulk solution B_n whose boundary is M_n is the n-sheeted space of B_1.

For example:
BTZ solution can be wriiten as :
$$ ds^2=r^2 d\tau^2 +(r^2+1)^{-1} dr^2 + (r^2+1) d\phi^2$$
n-sheeted BTZ is given by:
$$ ds^2= r^2 d\tau^2 +(n^2r^2+1)^{-1} n^{2}dr^2 + (n^2r^2+1) n^{-2} d\phi^2$$
 

1. What is the significance of the "n-sheeted" metric in AdS3?

The "n-sheeted" metric in AdS3 refers to the construction of a geometry with multiple copies of the AdS3 space stacked on top of each other. This creates a "covering space" that allows for the existence of closed timelike curves, which are necessary for the construction of the BTZ black hole.

2. How is the BTZ black hole constructed using the "n-sheeted" metric?

The BTZ black hole is constructed by identifying points on the "n-sheeted" AdS3 space that are related by a discrete group of isometries. This group, known as the modular group, acts on the "n-sheeted" space and creates a quotient space that is isomorphic to the BTZ black hole.

3. What are the physical implications of the "n-sheeted" AdS3 metric?

The "n-sheeted" AdS3 metric has important implications for the study of quantum gravity and black holes. It allows for the construction of the BTZ black hole, which is a solution to the equations of general relativity in 2+1 dimensions. This provides a valuable model for understanding the properties of black holes in higher dimensions.

4. How does the "n-sheeted" AdS3 metric relate to holography?

The "n-sheeted" AdS3 metric is closely related to the holographic principle, which states that information about a region of space can be encoded on its boundary. In the case of AdS3, the boundary is a 2-dimensional conformal field theory, and the "n-sheeted" metric describes the bulk geometry from which the boundary theory emerges.

5. Are there other applications of the "n-sheeted" AdS3 metric?

Yes, the "n-sheeted" AdS3 metric has been used in various areas of theoretical physics, including string theory, quantum gravity, and holography. It has also been studied in the context of topological black holes and cosmological models. Additionally, it has been used as a tool for understanding the properties of other black holes in different dimensions.

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