Wikipedia article: No time in General Relativity

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Discussion Overview

The discussion centers around the concept of time in the context of general relativity (GR) and its implications for quantum mechanics, particularly focusing on the so-called "problem of time." Participants explore the relationship between time and spacetime in GR, the challenges of quantizing gravity, and interpretations of the Wheeler-DeWitt equation.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants suggest that the problem of time in quantum gravity arises from the notion that there is no time in general relativity, as the Hamiltonian is a constraint that must vanish.
  • Others argue that certain solutions, like the FLRW model, do have a globally well-defined time, challenging the assertion that time does not exist in GR.
  • It is noted that in FLRW spacetimes, "time" is a geometric property, but this does not equate to time evolution in the quantum mechanical sense.
  • Participants discuss the necessity of a well-defined global notion of energy to have a Hamiltonian operator that generates time evolution, which is absent in general spacetimes in GR.
  • One participant expresses skepticism about the Wheeler-DeWitt equation, stating that it implies there is no time at all, while another clarifies that it indicates the wave function of the universe does not change.

Areas of Agreement / Disagreement

Participants express differing views on the existence and nature of time in general relativity and its implications for quantum mechanics. There is no consensus on the interpretations of the problem of time or the implications of the Wheeler-DeWitt equation.

Contextual Notes

Limitations include the dependence on specific models like FLRW and the unresolved nature of how to quantize gravity while maintaining a coherent notion of time.

Nick666
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"In quantum gravity, the problem of time is a conceptual conflict between general relativity and quantum mechanics. Roughly speaking, the problem of time is that there is none in general relativity. This is because in general relativity, the Hamiltonian is a constraint that must vanish. However, in theories of quantum mechanics, the Hamiltonian generates the time evolution of quantum states. Therefore we arrive at the conclusion that "nothing moves" ("there is no time") in general relativity. Since "there is no time", the usual interpretation of quantum mechanics measurements at given moments of time breaks down. This problem of time is the broad banner for all interpretational problems of the formalism."

http://en.wikipedia.org/wiki/Problem_of_time

Could you shed some light on this for me ? Is this another way of saying there's no time, only spacetime in GR ?
 
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I think the summary statements in this article are just wrong. Some of the more detailed explanations are ok, but still tend to overstate the case. Solutions considered physically plausible (e.g. FLRW) have a globally well defined time. I have usually seen this discussed more in terms of:

- you want to quantize gravity
- but gravity = curvature = the relation of space and time
- so you suddenly need to have time itself subject to non-determinism

and nobody knows how to do this yet.
 
PAllen said:
Solutions considered physically plausible (e.g. FLRW) have a globally well defined time.

The "time" in these spacetimes is a geometric property of the solution (in FRW solutions, for example, it's the "time" defined by the set of "comoving" worldlines and the spacelike hypersurfaces orthogonal to them). But this property in itself does not give you "time evolution" in the sense of QM.

Another way of stating the problem is that, in order to have a Hamiltonian operator that can generate time evolution in the sense of QM, you need a well-defined global notion of energy. But there isn't one in a general spacetime in GR. The best you can do in the general case is to construct an expression that looks like a "Hamiltonian", but vanishes identically (this is the "Hamiltonian constraint"), so it can't act as a generator of anything.
 
Well, the Wheeler-DeWitt equation does say ##\hat{H} \vert \psi \gt = 0##, which basically amounts to "the wave function of the universe doesn't change". At least, to the extent you can express what it's saying in a short sentence of ordinary language.
 

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