Closed Time-Like Curves: Principles & Observations

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Discussion Overview

The discussion centers on closed time-like curves (CTCs), exploring their theoretical implications, potential observational evidence, and the challenges in demonstrating their existence within various spacetime models. Participants engage with concepts from general relativity and topology, considering both abstract models and practical observations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • Some participants propose that demonstrating a CTC would require evidence of recurring events or phenomena, potentially linked to memory or records of past occurrences.
  • Others argue that the existence of a CTC might necessitate observable structures, such as wormholes, to explain the curves' formation.
  • A participant suggests that imposing periodic boundary conditions on a flat Minkowski spacetime could create a model with CTCs, raising questions about how to demonstrate or refute their existence in such a model.
  • It is noted that the CTC version of Minkowski spacetime is not simply connected, contrasting it with ordinary Minkowski spacetime, which is simply connected.
  • Some participants challenge the idea that CTCs are merely artifacts of event labeling, asserting that different topologies indicate different manifolds.
  • There is a discussion about the nature of local versus nonlocal measurements, with participants questioning the observability of CTCs and the implications of periodicity in observed events.

Areas of Agreement / Disagreement

Participants express differing views on the implications of CTCs, the nature of spacetime topology, and the feasibility of observing CTCs. No consensus is reached regarding the methods of demonstrating or refuting CTCs.

Contextual Notes

Limitations include the dependence on specific definitions of topology and the unresolved nature of how to effectively probe global properties of spacetime in relation to CTCs.

Paul Colby
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Hi,

If I understand correctly, closed time like curves (CTC) are world lines that close upon themselves. What would an observer measure to demonstrate a CTC?
 
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Thanks for the reference. Not certain how it relates to potential experiments which might demonstrate a CTC. Seems to me that one would have to demonstrate events which reoccur or a related phenomena that implies such which itself would have to be reoccurring. Wouldn't showing reoccurrence imply memory or records of past events? Maybe this is the point we mumble something obscure about QM and move along.
 
Wouldn't it require something very obvious and easily observable to be causing the curve to exist, like a wormhole?
 
Grinkle said:
Wouldn't it require something very obvious and easily observable to be causing the curve to exist, like a wormhole?

Sure, but I think this side steps the question I really want to ask but find hard to articulate clearly. One may, for example, take a flat Minkowski space-time and impose periodic boundary conditions creating a model with CTC. How would one go about demonstrating or refuting a CTC in such a model when locally it's the same as one without a CTC? In GR events exist as a set and are given labels, coordinates. In practice, an event is only observable when something happens at those coordinates. As this example seems to show, CTC is only an artifact of bad event labeling.
 
Paul Colby said:
One may, for example, take a flat Minkowski space-time and impose periodic boundary conditions creating a model with CTC. How would one go about demonstrating or refuting a CTC in such a model when locally it's the same as one without a CTC?

You would have to find a way of probing the global topology of the spacetime; the CTC version of Minkowski spacetime that you describe is not simply connected, whereas ordinary Minkowski spacetime is simply connected.

Paul Colby said:
As this example seems to show, CTC is only an artifact of bad event labeling.

No, it isn't; the two spacetimes you describe have different topologies and are therefore different manifolds.
 
PeterDonis said:
No, it isn't; the two spacetimes you describe have different topologies and are therefore different manifolds.

They are different manifolds for certain, globally. My use of "locally the same" I believe is correct if I recall my topology classes.

The only observations I can think of that would tell us this would be the non periodic nature of observed events. How would we observe periodic ones if all things are periodic including the experimenter?

PeterDonis said:
You would have to find a way of probing the global topology of the spacetime;

I know of no nonlocal measurements that are not in some way comprised of local ones. So is the answer, no they are not observable?
 
Paul Colby said:
My use of "locally the same" I believe is correct if I recall my topology classes.

Locally you can't tell one topology from another; locally all manifolds look like a small piece of ##R^4## (or ##R## of whatever dimension you are working with).

Paul Colby said:
I know of no nonlocal measurements that are not in some way comprised of local ones.

Comprised of local measurements made at different points in the manifold. Combining the results from such measurements can tell you things that measurements made at just one point in the manifold will not tell you.
 

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