Does the Topology of AdS4 Affect Global Hyperbolicity?

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Discussion Overview

The discussion revolves around the global hyperbolicity of AdS4 spacetime, specifically examining the implications of its topology and the relationship between different metric representations. Participants explore the mathematical structure and coordinate systems used to describe AdS4, as well as the nature of the associated geometries.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant questions whether the coordinate system described leads to a topology of ##\mathbb{R} \times S^3## or if it is actually ##\mathbb{R}^2 \times S^2##, expressing uncertainty about the dimensionality of the angles involved.
  • Another participant proposes that the term ##l^2(d\chi^2 + \sin^2 \chi d\Omega^2)## represents the round metric on a 3-sphere of radius ##l##, noting that the range of ##\chi## suggests it covers only half of the 3-sphere.
  • A clarification is sought regarding the definition of ##S^3##, with a participant confirming it refers to a surface in ##\mathbb{R}^4## and its relation to groups like ##\mathrm{SO}(3)## and ##\mathrm{SU}(2)##.
  • Another participant acknowledges a misunderstanding regarding the notation ##d\Omega^2##, which represents the solid angle over ##S^2##, and expresses regret for any confusion caused.

Areas of Agreement / Disagreement

Participants express differing views on the topology associated with the coordinate system and the implications for global hyperbolicity. There is no consensus reached on these points, and the discussion remains unresolved.

Contextual Notes

Some assumptions about the nature of the metrics and their implications for global hyperbolicity are not fully explored, and the discussion reflects varying interpretations of the mathematical representations involved.

ergospherical
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Is ##\mathrm{AdS_4}## globally hyperbolic?$$g = -\left(1+ \dfrac{r^2}{l^2} \right)dt^2 + \dfrac{dr^2}{1+ \dfrac{r^2}{l^2}}+ r^2d\Omega^2$$Letting ##r = l \tan \chi## then defining ##\tilde{g} = g \cos^2 \chi##\begin{align*}
g &= \sec^2 \chi (-dt^2 + l^2 d\chi^2) + l^2 \tan^2 \chi d\Omega^2 \\ \\

\tilde{g} &= -dt^2 + l^2 (d\chi^2 + \sin^2 \chi d\Omega^2) \\
\tilde{g} &= -dt^2 + l^2 d\omega^2\end{align*}the topology is ##\mathbb{R} \times S^3##. Does global hyperbolicity of ##\tilde{g}## ##\iff## global hyperbolicity of ##g##?
 
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I don't know anything about string theory, but isn't that coordinate system a mapping to ##\mathbb{R^2} \times S^2## not ##\mathbb{R^1} \times S^3##? It looks like only two angles and a radius to me (plus time). Am I missing something?

If I'm missing something obvious, ignore me. I just chimed in because the thread went unanswered.
 
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My thinking was that ##l^2(d\chi^2 + \sin^2 \chi d\Omega^2)## is the round metric on a ##3##-sphere of radius ##l## (or in fact since ##\chi \in \bigg{[} 0, \dfrac{\pi}{2} \bigg{)}## it'll only be half of the 3-sphere...)
 
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Just to make sure we're talking about the same thing, when you say ##S^3##, you mean a surface embedded in ##\mathbb{R}^4## given by ##x^2 + y^2 + z^2 + w^2 = 1##, right? As in, the sphere that is diffeomorphic to the special orthogonal group ##\mathrm{SO}(3)## and the special unitary group ##\mathrm{SU}(2)##, right?
 
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Yeah, and ##(\chi, \theta, \varphi)## would be the hyperspherical coordinates on the 3-sphere of radius ##l##.
 
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I'm a dope and I only just caught that ##d\Omega^2## was a total solid angle over ##S^2##. Now I'm on board with your claim about the topology. Sorry for derailing ya
 

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