Meaning of Spacetime Foliations

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Discussion Overview

The discussion revolves around the concept of spacetime foliations, particularly in the context of Lorentzian and Newtonian frameworks, and their implications for theories like Bohmian mechanics. Participants explore the differences between traditional spacetime foliations in relativity and the additional structures proposed by Tim Maudlin in his article on non-local correlations in quantum theory.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant notes that Lorentz spacetime represents a new foundation compared to Galilean spacetime, emphasizing the role of the speed of light as a limit.
  • Another participant questions whether Maudlin's reference to spacetime foliations implies the introduction of a preferred frame in special relativity (SR) for defining absolute simultaneity.
  • A different participant expresses confusion regarding the statement that no positive part of the relativistic account is rejected, suggesting that absolute time complicates the construction of a total metric.
  • Some participants discuss the relationship between preferred frames and aether, questioning if all preferred frames in SR can be considered aether frames.
  • There is a debate about whether characteristics of aether apply to all inertial frames and the implications for Bohmian mechanics, particularly regarding its non-locality.
  • One participant asserts that the wave function in Bohmian mechanics is sensitive to configuration changes throughout the universe, raising questions about how this non-locality can be modeled within the framework of special relativity.
  • Another participant challenges the idea that light propagates at the speed of light (c) in the aether frame, suggesting that Bohmian mechanics implies instantaneous propagation instead.

Areas of Agreement / Disagreement

Participants express various viewpoints on the nature of spacetime foliations and their implications for non-locality in quantum mechanics. There is no consensus on whether Maudlin's ideas align with traditional interpretations of spacetime or if they introduce fundamentally new concepts. The discussion remains unresolved regarding the relationship between preferred frames, aether, and the implications for Bohmian mechanics.

Contextual Notes

Participants highlight the complexity of integrating non-local theories with relativistic frameworks, noting that assumptions about simultaneity and spacetime structure are critical to the discussion. The implications of these assumptions on the interpretation of Bohmian mechanics and its compatibility with relativity are not fully explored.

  • #91
The following are important exchanges between Demystifier (Nikolic) and Physicforums only challenger (Maaneli). The contents are important because what is at stake is the soul of physics and the great debate about non-locality.

Selected vital quotes from the thread "Re: Pilot wave theory, fundamental forces":

Maaneli: the relativity of simultaneity is nevertheless a consequence of the metrical structure of Minkowski spacetime

Demystifier: No, this is not true. What is true is that the metrical structure of Minkowski spacetime implies relativity of simultaneity IF THERE IS NO ANY OTHER STRUCTURE. But in the case we are considering there is another structure. And this additional structure is not the parameter s (as you might naively think), but the non-local wave function. (Or the scalar potential in the classical setting discussed in http://xxx.lanl.gov/abs/1006.1986.)

And yet, you can see that this nonlocal wave function (or the scalar potential) is compatible with the metrical structure of Minkowski spacetime and does not introduce a foliation-like structure.

So, does it mean that you agree that WITH example of my theory there IS a known dynamical structure that is consistent with the metrical structure of Minkowski spacetime, and yet violates the relativity of simultaneity?

By the way, one can introduce such a structure even in classical local relativistic mechanics. Consider two twins who initially have the same velocity and same position, and their clocks show the same time. After that, they split apart, and each has a different trajectory, independent of each other. Yet, one can consider pairs of points on two trajectories which have THE SAME VALUE OF PROPER TIME (showed by a local clock on each trajectory). Such a structure (defined at least mathematically, if not experimentally) also can be said to violate relativity of simultaneity, in a way very similar to that of my theory. Of course, there is a difference, but the similarity may be illuminating too.

Demystifier: Or let me use an analogy with nonrelativistic BM. A point is space is denoted as r=(x,y,z). Consider two particles with space positions {\bf r}_1 and {\bf r}_2 at a given time t. There is a Cartesian frame (given by a rotation of the original Cartesian frame) in which {\bf r}_1 and {\bf r}_2 have the same value of z. In this frame, we say that the interaction between these two particles is z-taneous. Does it lead to any paradoxes? Does it mean there is a preferred z-coordinate? Does it mean there is a preferred foliation of space into 2-surfaces? Whatever your answer is, the same answer applies to analogous questions in relativistic-covariant BM. And if you still don't get it, then look at the equations of relativistic-covariant BM again.


Maaneli: ... by virtue of the fact that you have to synchronize the initial (spacetime) positions of the particles at a common time s,

Demystifier: The parameter s is not time.

Maaneli: But as a "joint parameter", it plays precisely the role of a universal time parameter for the evolution of the particle spacetime coordinates. Yes, I realize that the wavefunction on configuration spacetime doesn't depend on s, but that doesn't mean that s cannot also be interpreted as a time parameter (even if it is a fictitious one).

Demystifier: You are right. The parameter s can be interpreted as a sort of time. However, this is more like Newton absolute time, note like Einstein relativistic time [which I already implied by saying it is a UNIVERSAL time parameter]. OK, that's clear enough. And you are right, nonlocal signaling violates the relativity of simultaneity. Yet, in the next post I explain why it is NOT in contradiction with metrical structure of Minkowski spacetime.

(Maaneli in other message mentioned Nikolic theory has foliation like structure)

Demystifer: No, there is no foliation-like structure. The synchronization parameter is NOT something additional to the SR metrical structure, just as time in nonrelativistic BM is NOT something additional to the 3-space rotational-symmetry structure.

My point is that relativistic-covariant BM in 4-dimensional spacetime is ANALOGOUS to nonrelativistic BM in 3-dimensional space. I am just trying to make you understand this ANALOGY, because when you do, you will suddenly say: "Oh, THAT is what you meant. Now I get it. In fact, it is trivial." But it is essential that you see this analogy by yourself, while I can only guide you in the right direction. And at the moment, it seems to me that you don't have a clue what I am talking about, because you are not able to see the analogy. And that is probably because you are unable to think of time as just another "space" coordinate.

To help you think in the correct way, let me suggest you a mental trick. For a moment, FORGET that the spacetime metric has the form (+---). Instead , think of metric as just any metric, which can be (++++), (++--), or whatever. In fact, simply don't think about metric at all. Just pretend that you have a 4-dimensional space with some unspecified metric. Or if it is easier for you, just pretend that the metric is (++++). And forget that one of the coordinates is called "time". (Who cares about names, anyway?) And NOW try to understand again what equations of relativistic-covariant BM are actually saying. This trick works for many physicists, so it could work for you as well.

(Note: the last exchange between Demystifer and Maaneli occurred in Jun 22, 2010)

Maaneli: Of course, by covariant, you must mean "fundamentally covariant", because anyone can construct a covariant particle dynamics on a preferred foliation. I think it might be best for us to resume our discussion on the old thread, "Pilot waves, fundamental forces, etc.", regarding whether your proposal of using a synchronization parameter and treating time and space on equal footing is truly fundamentally covariant or not, and whether or not it does have the condition of equivariance. We never got to finish that discussion, mainly because I became too overwhelmed with deadlines and work and kept forgetting to reply to the thread. My apologies about that.

Demystifier: I would like to continue the discussion there. But I will wait for your first step.

(But they never continued. And since June, 2010. There is no other challenger to Demystifier. And he continued to share his papers which are referenced in peer reviewed journals but unfortunately, no one read it much. Therefore let us continue and settle it once and for all whether Demystifier is fundamentally correct. Before I make a new thread out of this. Just want some comment from you PeterDonis on what you think about all this. Thanks)
 
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  • #92
harrylin said:
I'm now far behind with looking at the interesting references of this thread, that's for later. Consequently I can't really comment on your conclusions. My first impression is that those "flashing" foliation theories are pseudo science, and I think that the Copenhagen interpretation is a pseudo interpretation (effectively a physical non-interpretation). :-p Anyway, the subtle thing about "spacetime" is that of course space-time is (and has been from the start) an important part of classical mechanics. Only Minkowskian (as well as post-Minkowskian) Spacetime is a new concept that corresponds to a popular interpretation of relativistic mechanics.

Look at the nice graphic illustration (even in motion) of the flashes in Tumulka's presentation:

http://www.math.rutgers.edu/~tumulka/talks/penn09.pdf

Mulling at them would give a good work out in our final search for Quantum Gravity.
 
  • #93
I've just noticed this thread, in which some of my papers have been discussed a lot.

If someone is still interested, now I can answer any related questions.

In addition, I would like to mention my very recent paper in which I propose a different relativistic-covariant version of Bohmian mechanics, in which a "preferred" foliation exists, but is determined in a covariant way by the relativistic-invariant wave function:
http://xxx.lanl.gov/abs/1205.4102
 

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