Hi Carlo,
I am also going to break in here, because I believe George Ellis made a crucial remark.
George explained his understanding of your claim that there is no preferred time variable in GR (George Ellis, Dec. 12, 2008 @ 20:27 GMT):
"This is correct as regards spacelike surfaces that can represent constant time. But proper time along world lines is indeed a preferred time variable in GR. The fundamental difference from Newtonian theory is that the preferred time is defined along world lines, instead of by spacelike surfaces. Proper times along timelike worldlines is what is measured by clocks ticking (p.3). So you focus on problems with surfaces of constant time, I focus on the meaningful nature of proper time along world lines."
On the other hand, in your arXiv:gr-qc/0604045v2, p. 4, you explained your understanding of 'no preferred time variable in GR' in the following fashion:
"In general relativity, when we describe the dynamics of the gravitational field (not to be confused with the dynamics of matter in a given gravitational field), there is no external time variable that can play the role of observable independent evolution variable. The field equations are written in terms of an evolution parameter, which is the time coordinate x^0, but this coordinate, does not correspond to anything directly observable. The proper time [tau] along spacetime trajectories cannot be used as an
independent variable either, as [tau] is a complicated non-local function of the gravitational field itself.
Therefore, properly speaking, GR does not admit a description as a system evolving in terms of an observable time variable.
...
"This weakening of the notion of time in classical GR is rarely emphasized: After all, in classical GR we may disregard the full dynamical structure of the theory and consider only individual solutions of its equations of motion. A single solution of the GR equations of motion determines "a spacetime", where a notion of proper time is associated to each timelike worldline (notice the remark by George above - D.C.).
"But in the quantum context a single solution of the dynamical equation is like a single "trajectory" of a quantum particle: in quantum theory there are no physical individual trajectories: there are only transition probabilities between observable eigenvalues. Therefore in quantum gravity it is likely to be impossible to describe the world in terms of a spacetime, in the same sense in which the motion of a quantum electron cannot be described in terms of a single trajectory."
It seems to me that you and George are discussing 'apples and oranges': you are discussing the problem of time in classical GR, while he was (tacitly?) implying some yet-to-be discovered quantum gravity in which the "meaningful nature of proper time along world lines" (George Ellis, Dec. 12, 2008 @ 20:27 GMT) would be akin to "a single trajectory" (arXiv:gr-qc/0604045v2, p. 4).
May I ask you to sort out this issue with 'scrupulous intellectual honesty' (C. Rovelli, arXiv:gr-qc/0109034v2, p. 9).
Please also notice my criticism of your Essay, posted earlier ( Dec. 12, 2008 @ 03:58 GMT and Dec. 12, 2008 @ 16:21 GMT): the Heraclitian Time, which corresponds to the very *generation of 3-D space*, is absent in GR.
Again, if you really believe, with scrupulous intellectual honesty, that we should "forget" time, you have to demonstrate the emergence of 3-D space from some primitive (Borel?) set of abstract mathematical points, and then prove that this *emergence* is indeed timeless.
Please act promptly: the Heraclitean Time you have by the contest ending (January 1, 2009) is running out.
Dimi