Spacetime topology of the Universe

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Discussion Overview

The discussion centers on the topology of the Universe as spacetime, exploring various speculations and models related to its structure. Participants examine the implications of different topological properties and their relationship to geometry, particularly in the context of Friedmann-Robertson-Walker (FRW) models.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • Some participants suggest that the topology of spacelike hypersurfaces of constant cosmological time might be nearly flat on a large scale.
  • Others argue that flatness is a geometric property rather than a topological one, stating that spacetime should be homeomorphic to a product of a spatial topology and time.
  • There is a contention regarding the interpretation of homeomorphism, with some asserting that it does not convey information about geometry.
  • Participants discuss the implications of standard FRW models, noting that the topology of spacetime could be either ##\mathbb{R}^4## for spatially infinite universes or ##\mathbb{S}^3 \times \mathbb{R}## for spatially finite ones.
  • Questions arise about the relationship between the expanding universe and the proper distance between galaxies, with some participants noting that this may not pertain directly to topology.
  • One participant introduces the concept of Closed Timelike Curves (CTC) in relation to FRW models, suggesting that while topological manifolds may allow for CTC, the actual existence depends on the metric structure.
  • Another participant challenges the notion of CTC as a topological concept, emphasizing the necessity of a metric for such discussions.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between topology and geometry, as well as the implications of FRW models. The discussion remains unresolved, with differing opinions on the nature of spacetime topology and its properties.

Contextual Notes

Some statements reflect a misunderstanding of the distinction between topological and geometric properties, and there are unresolved questions regarding the implications of various models and concepts introduced in the discussion.

cianfa72
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TL;DR
Speculations about the topology of the Universe as spacetime
The question might be a bit weird: which are the current "speculations" about the topology of the Universe as spacetime ?

I'm aware of, from the point of view of spacelike hypersurfaces of constant cosmological time, the topology of such "spaces" might be nearly flat on large scale.

What about the topology of spacetime itself? Thanks.
 
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I wouldn't say that flatness is a topological property. It requires more structure. If the space slices are homeomerphic to ##X##, the the space time is homeomorphic to ##X\times \mathbb R##.
 
martinbn said:
I wouldn't say that flatness is a topological property. It requires more structure.
Ah yes, I should say spacelike hypersurfaces of constant cosmological time homeomorphic to a "flat" 3D space.

martinbn said:
If the space slices are homeomerphic to ##X##, the the space time is homeomorphic to ##X\times \mathbb R##.
Why ? According to you the spacetime as whole should have the topology of a sort of "sheet" or "cylinder".
 
cianfa72 said:
the topology of such "spaces" might be nearly flat on large scale.
That's not topology, that's geometry. In standard FRW models of the universe, the topology of spacetime is ##\mathbb{R}^4## if the universe is spatially infinite, or ##\mathbb{S}^3 \times \mathbb{R}## if it is spatially finite (closed).
 
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cianfa72 said:
spacelike hypersurfaces of constant cosmological time homeomorphic to a "flat" 3D space.
That's no better than your previous statement; "homeomorphic" says nothing whatever about geometry, "flat" or otherwise. If it's homeomorphic to ##\mathbb{R}^3##, it's homeomorphic to any space with topology ##\mathbb{R}^3##, whether it's flat or not.
 
PeterDonis said:
In standard FRW models of the universe, the topology of spacetime is ##\mathbb{R}^4## if the universe is spatially infinite, or ##\mathbb{S}^3 \times \mathbb{R}## if it is spatially finite (closed).
In standard FRW models, the timelike congruence of comoving observers is hypersurface orthogonal (let's say it is "irrotational", i.e. it has zero vorticity), yet in general it isn't stationary (spacelike hypersurfaces of constant cosmological time don't have the same geometry).

Does "expanding universe" mean that the "proper distance" between galaxies, evaluated as the length along geodesic curves connecting them in any of such spacelike hupersurfaces (geodesic curves when restricted to any of such hypersurfaces), increases with cosmological time ?
 
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cianfa72 said:
In standard FRW models, the timelike congruence of comoving observers is hypersurface orthogonal (let's say it is "irrotational", i.e. it has zero vorticity), yet in general it isn't stationary (spacelike hypersurfaces of constant cosmological time don't have the same geometry).
None of these things have anything to do with topology. This thread is about topology, isn't it? What do you want to talk about?

cianfa72 said:
Does "expanding universe" mean that the "proper distance" between galaxies, evaluated as the length along geodesic curves connecting them in any of such spacelike hupersurfaces (geodesic curves when restricted to any of such hypersurfaces), increases with cosmological time ?
None of this has anything to do with topology either. What is the topic of this thread supposed to be?
 
PeterDonis said:
None of this has anything to do with topology either. What is the topic of this thread supposed to be?
You are right, it was a bit OT. It was just to better understand the meaning of "expanding universe".

Coming back to spacetime topology, FRW models (or better FLRW ?) with topologies ##\mathbb R^4## or ##\mathbb{S}^3 \times \mathbb{R}## allow in principle Closed Timelike Curves (CTC) as topological manifolds. However the relevant structure for their actual existence is the metric (metric tensor ##g_{ab}##) i.e. let me say the actual "distribution" of light cones through spacetime.

Do exist examples of FWR models that have CTC ?
 
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cianfa72 said:
It was just to better understand the meaning of "expanding universe".
Then start a separate thread on that question.
 
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cianfa72 said:
FRW models (or better FLRW ?) with topologies ##\mathbb R^4## or ##\mathbb{S}^3 \times \mathbb{R}## allow in principle Closed Timelike Curves (CTC) as topological manifolds.
This is nonsense. There is no such thing as a CTC as a topological manifold; "timelike" requires a metric, which is not a topological concept.

I am closing this thread because you can't even pose a question that is on the topic you yourself chose for the thread.
 

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