Is hyperbolic space consistent with homogeneity?

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Discussion Overview

The discussion revolves around the consistency of hyperbolic space with homogeneity, particularly in the context of the Friedmann-Robertson-Walker (FRW) metric. Participants explore the implications of different metrics on the perception of homogeneity in cosmological distances and the nature of spatial measurements in a universe described by hyperbolic geometry.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant notes that the FRW metric can be expressed with different curvature parameters (k=-1, 0, +1) and discusses the implications of these on homogeneity, particularly highlighting the special nature of points in the k=-1 case when embedded in Euclidean space.
  • Another participant argues that the distance measured in cosmology is not Euclidean but rather based on the intrinsic metric of a spacelike slice, suggesting that k=-1 hyperbolic space can still be homogeneous.
  • A later reply agrees that the spatial distance measure is not Euclidean but Minkowskian, asserting that distances in the universe are perceived through the Euclidean measure, which may lead to a non-homogeneous appearance in galaxy distribution.
  • Further contributions emphasize that while the space may be homogeneous with respect to the intrinsic metric, the perception of homogeneity may be affected by the metrics used for measurement.
  • Participants question the validity of using the Euclidean distance measure, with one expressing confusion over the intrinsic metric being used in cosmological observations.

Areas of Agreement / Disagreement

Participants generally agree that the intrinsic metric of hyperbolic space can be homogeneous, but there is contention regarding the implications of this for how distances are perceived in the universe. Multiple competing views remain on whether the perceived distribution of galaxies reflects true homogeneity.

Contextual Notes

Participants highlight the dependence on the choice of metric for measuring distances and the implications this has for the perception of homogeneity. There are unresolved questions about the nature of the metrics being used in cosmological observations and how they relate to the intrinsic properties of hyperbolic space.

center o bass
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The FRW metric is usually expressed as
$$ds^2 = -dt^2 + a(t)^2 ( \frac{dr^2}{1-kr} + r^2 d\Omega^2))$$
where ##k=-1,0,+1## respectively for a hyperbolic, flat or spherical space. The spatial part of this metric can be derived by considering a 3-sphere embedded in a four-dimensional flat space -- any sphere obviously being homogeneous.

Similarly, the k=-1 case can be derived by considering a hyperboloid embedded in a flat four dimensional space. Now, the hyperboloid is only a homogeneous space when embedded in a flat minkowskian space -- in Euclidean space the point at the tip of the hyperboloid (corresponding to r=0) is certainly special.

Since it is the euclidean distance we measure when measuring distances to other galaxies, it seems like the k=-1 case is not consistent with homogeneity. Is this correct, or is my thinking wrong?
 
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center o bass said:
Since it is the euclidean distance we measure when measuring distances to other galaxies, it seems like the k=-1 case is not consistent with homogeneity.

The distance we measure is not the Euclidean distance; it's the distance in a spacelike slice of constant cosmological time (i.e., ##dt = 0## in the metric you wrote down), given the metric of the spacelike slice. (Note that we don't directly "measure" this distance either; we calculate it based on other "distance" observations.) None of this has anything to do with how, or whether, you can embed that spacelike slice in a higher-dimensional Euclidean or Minkowskian space. The only requirement for homogeneity is that no point is "special" with reference to the intrinsic metric of the spacelike slice. The ##k = -1## hyperbolic space satisfies that requirement.
 
PeterDonis said:
The distance we measure is not the Euclidean distance; it's the distance in a spacelike slice of constant cosmological time (i.e., ##dt = 0## in the metric you wrote down), given the metric of the spacelike slice. (Note that we don't directly "measure" this distance either; we calculate it based on other "distance" observations.) None of this has anything to do with how, or whether, you can embed that spacelike slice in a higher-dimensional Euclidean or Minkowskian space. The only requirement for homogeneity is that no point is "special" with reference to the intrinsic metric of the spacelike slice. The ##k = -1## hyperbolic space satisfies that requirement.

I agree that the spatial distance measure is not euclidean; its Minkowskian (see Weinberg Gravitation p. 391) -- so the space is homogeneous only with respect to this metric. However, I would argue that we measure distances in the universe by the Euclidean distance measure, and thus, to us, I would not think that it appears homogeneous regarding the distribution of galaxies etc.
 
So I agree that the space is homogeneous with regards to the intrinsic metric. However, as we do not use this metric (which has signature -1), my argument is that we do not __see it__ as being homogeneous?
 
center o bass said:
I would argue that we measure distances in the universe by the Euclidean distance measure,

Why do you think that? The "Euclidean distance measure" is a measure in a higher-dimensional embedding space that doesn't even exist (it's just a mathematical fiction used by some people for modeling).

center o bass said:
However, as we do not use this metric (which has signature -1)

I'm confused. What "intrinsic" metric do you think we are not using? (If you think we are using the Euclidean metric, see above.)
 

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