Hamiltonian Formulation of GR for Elliptic Spacetime?

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Discussion Overview

The discussion revolves around the limitations of the ADM formulation of General Relativity (GR) when applied to elliptic spacetimes. Participants explore the implications of the ADM method's reliance on globally hyperbolic manifolds and its inability to accommodate closed timelike curves, raising questions about the broader applicability of Hamiltonian formulations in GR.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Conceptual clarification

Main Points Raised

  • One participant notes that the ADM formulation requires a foliation of spacetime into 3+1 dimensions, which may not be possible in elliptic spacetimes due to geodesics crossing each other.
  • Another participant mentions that the ADM formulation assumes a globally hyperbolic manifold, suggesting that non-hyperbolic solutions would require different methods.
  • A reference to Wald indicates that the Hamiltonian formulation necessitates Cauchy surfaces, reinforcing the need for global hyperbolicity.
  • One participant expresses concern that this limitation poses challenges for theories of Quantum Gravity based on the ADM formulation.
  • Another participant argues that the restriction may not be as significant, as many physicists expect Quantum Gravity to inherently prohibit closed timelike curves and other problematic causal structures.
  • Comments from a linked paper suggest that Hamiltonian formulations could apply to a broader class of models than the initial value formulation, which is limited to globally hyperbolic spacetimes.
  • There is confusion regarding the implications of topology in Hamiltonian formulations, with participants questioning how solutions with different topologies might be accommodated.
  • One participant clarifies that the global hyperbolic restriction does not exclude spatially bounded solutions, indicating that Cauchy surfaces can have various topologies.

Areas of Agreement / Disagreement

Participants express differing views on the significance of the ADM formulation's limitations, with some emphasizing the constraints it imposes on Quantum Gravity theories, while others argue that these limitations may not be as critical. The discussion remains unresolved regarding the broader applicability of Hamiltonian formulations in GR.

Contextual Notes

Participants note that the ADM formulation's reliance on globally hyperbolic manifolds and Cauchy surfaces may limit the exploration of certain spacetime geometries, particularly those with closed timelike curves. The implications of topology in Hamiltonian formulations are also highlighted as a point of contention.

korialstasz
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This has bothered me for some time. In the ADM formulation, we foliate spacetime into 3+1 dimensions by creating 3 dimensional hypersurfaces via ##T = constant## along the worldline of some observer whose proper time is ##T##. This allows us to write dynamical equations for the evolution of some initial 3D spacelike hypersurface ##\Sigma##.

However, this only works for a general flat or hyperbolic manifold, because geodesics which are initially normal to ##\Sigma## will never cross. For an elliptic spacetime, those geodesics would eventually cross each other, such that the map ##\Sigma_T \rightarrow \Sigma_{T'}## would fail to be one-to-one. This means that solutions to Einstein's Equations found via the ADM formulation cannot have closed timelike curves, since every geodesic can only intersect each hypersurface once.

Therefore, what limitations does the ADM formulation of GR impose on the full set of solutions of Einstein's Equations? If we can't foliate an elliptic manifold, then doesn't that mean that we won't find any elliptic spacetime geometries using the ADM method?
 
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So far as I know (and I'm not an expert in ADM), it assumes a-priori that the manifold is globally hyperbolic to achieve the required foliation. Then it could not be used to find non-hyperbolic manifold as a solution. Some other method would be required to find such a solution.
 
According to Wald (sec E.2 p. 459), in the Hamiltonian formulation of GR the space-like hypersurfaces in the one-parameter family foliating the space-time are taken to be Cauchy so the space-time would have to be globally hyperbolic (as PAllen noted). Hopefully this helps! Cheers.
 
Thanks a bunch, that's what I've read as well. I'm writing my undergrad thesis on the ADM formulation of GR and using it as a basis of a theory of Quantum Gravity, and this seems to be a major limitation for any QG theory built from the Hamiltonian formulation. I'll take it up with my advisor
 
korialstasz said:
Thanks a bunch, that's what I've read as well. I'm writing my undergrad thesis on the ADM formulation of GR and using it as a basis of a theory of Quantum Gravity, and this seems to be a major limitation for any QG theory built from the Hamiltonian formulation. I'll take it up with my advisor

Why major? All it prevents are closed time like curves and some other dubious causal structures (e.g. intersection of a past light cone of e1 and future light cone of e2 that is not compact). Many physicists would say they expect QG to prohibit such things anyway.
 
korialstasz said:
Thanks a bunch, that's what I've read as well. I'm writing my undergrad thesis on the ADM formulation of GR and using it as a basis of a theory of Quantum Gravity, and this seems to be a major limitation for any QG theory built from the Hamiltonian formulation. I'll take it up with my advisor

There were comments on this in http://philosophyfaculty.ucsd.edu/faculty/wuthrich/pub/WuthrichChristianPhD2006Final.pdf

"Thus, Hamiltonian formulations might apply to a larger class of models in GTR than does the initial value formulation, which only deals with globally hyperbolic spacetimes. There is a natural connection between these two formulations, but they need not coincide."

"The restriction to generally relativistic models with manifolds of topology R × Ʃ is far from innocent, for at least two reasons."

"In this sense, a Hamiltonian formulation of GTR does not a priori rule out the existence of closed timelike curves. It should be noted, however, in both known Hamiltonian formulations of GTR, spacetime is foliated using a global time function."
 
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atyy said:
There were comments on this in http://philosophyfaculty.ucsd.edu/faculty/wuthrich/pub/WuthrichChristianPhD2006Final.pdf

"Thus, Hamiltonian formulations might apply to a larger class of models in GTR than does the initial value formulation, which only deals with globally hyperbolic spacetimes. There is a natural connection between these two formulations, but they need not coincide."

"The restriction to generally relativistic models with manifolds of topology R × Ʃ is far from innocent, for at least two reasons."

"In this sense, a Hamiltonian formulation of GTR does not a priori rule out the existence of closed timelike curves. It should be noted, however, in both known Hamiltonian formulations of GTR, spacetime is foliated using a global time function."

ADM, being one of the [best] "known Hamiltonian formulations".
 
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PAllen said:
ADM, being one of the [best] "known Hamiltonian formulations".

Actually, I don't quite get why Wuthrich says in principle any solution of GR which has topology R X Ʃ has a Hamiltonian formulation, even though the known cases have (I think) Ʃ = time.
 
atyy said:
Actually, I don't quite get why he says in principle any solution of GR which has topology R X Ʃ has a Hamiltonian formulation, even though the known cases have (I think) Ʃ = time.

Hmm, I thought the R was time. A quick read of the section in your link suggests considering allowing initial conditions that are causally connected to support a slicing where R is not time. The author admits it is not clear how this would work.

In case the OP isn't aware, global hyperbolic restriction does not prevent spatially bounded solutions - each cauchy surface could be topologically a 3-sphere, for example.
 
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  • #10
PAllen said:
Hmm, I thought the R was time. A quick read of the section in your link suggests considering allowing initial conditions that causally connected to support a slicing where R is not time. The author admits it is not clear how this would work.

In case the OP isn't aware, global hyperbolic restriction does not prevent spatially bounded solutions - each cauchy surface could be topologically a 3-sphere.

Yes, R was time, got fooled by thinking Ʃ was closer to T.
 

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