Undergrad GR: Attractors & Liouville's Theorem

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Liouville's theorem states that the volume of phase space is preserved in classical Hamiltonian mechanics, implying that attractors do not exist in this framework. In general relativity (GR), while the Raychaudhuri equation suggests shrinking volumes, it does not directly address phase space dynamics. GR adheres to Liouville's theorem, but the phase space in field theories is infinite-dimensional, complicating the relationship between 3-dimensional volume and phase space volume. The discussion also touches on the implications of time reversal invariance in GR, with expanding solutions like white holes often dismissed due to unrealistic initial conditions. Overall, the connection between Liouville's theorem and GR remains complex and not fully rigorous due to the infinite degrees of freedom in field theories.
atyy
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TL;DR
Does GR have attractors?
In classical Hamiltonian mechanics, because of Liouville's theorem about the volume of phase space being preserved by time evolution, there are no attractors.

Naively, I think of the Raychaudhuri equation in GR as showing a shrinking volume. However, I guess Raychaudhri's equation does not deal with the phase space of GR.

Does GR have attractors?
Is there something like the Liouville theorem in GR, especially since GR has a Hamiltonian formulation?
 
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Just a guess, but given that very little is known about the global properties of solutions to the initial value problem, I would say that it is a very hard question.
 
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atyy said:
Is there something like the Liouville theorem in GR, especially since GR has a Hamiltonian formulation?
Every Hamiltonian system obeys the Liouville theorem. GR is not an exception. Note, however, that the phase space in field theories is infinite dimensional. In particular, the 3-dimensional volume of a lump of matter (which may shrink due to gravitational collapse) has nothing to do with the infinite-dimensional phase-space volume.
 
atyy said:
Naively, I think of the Raychaudhuri equation in GR as showing a shrinking volume.
GR is invariant under the time reversal. Raychaudhuri equation can describe also the expansion. In the black-hole context, such an expanding solution is called a white hole. Such solutions are usually discarded because they require unrealistic initial conditions, or equivalently, because for such solutions entropy decreases with time.
 
Demystifier said:
Every Hamiltonian system obeys the Liouville theorem. GR is not an exception. Note, however, that the phase space in field theories is infinite dimensional. In particular, the 3-dimensional volume of a lump of matter (which may shrink due to gravitational collapse) has nothing to do with the infinite-dimensional phase-space volume.
Are you sure the theorem holds in field theories?
 
martinbn said:
Are you sure the theorem holds in field theories?
Formally yes, but I guess it's not fully rigorous due to the infinite number of degrees of freedom.
 
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