marcus said:
Well a world-famous GR expert named Ted Jacobson has something called Einstein-Aether which has a timelike unit-vector field. And Petr Horava at UC Berkeley (pronounced Ho-zha-va) has proposed GR replacement that I believe somebody has gotten a preferred foliation out of. I don't keep track of all the proposed GR replacements. You know about CDT, i guess. Ambjorn and Loll's Causal Dynamical Triangulation. That is built on a preferred foliation. That is slicing spacetime into space like slices so you get layers---essentially a preferred time.
And of course there is Tomita Time that some Loop people have been working on.
And as I told you you get a preferred time in Cosmology as soon as you fill the early universe with hot gas and look at the CMB. Or even if you just have ordinary Friedman model expansion.
How many percentage of physicists think of this preferred time? Lee Smolin based it on the Big Bang and CMB. For weeks I still can't decide what to make of this. Do you guys treat a global preferred time as a global preferred frame? is it the same? For those who knows arguments where the big bang and CMB are Lorentz invariant and there can't be preferred time, please share it now... the following is the logic behind Lee Smolin belief in it (anyone has counterarguments?) from his book "Time Reborn" (shared for sake of discussion).
"Before discussing how theory might resolve this contradiction, let’s look at what experiment
has to say. A preferred global notion of time implies a preferred observer, whose clock
measures that preferred time. This contradicts the relativity of inertial frames, according to
which there is no experimental or observational way to distinguish an observer supposedly
at rest from those moving with a constant but arbitrary velocity.
The first thing to note is that the universe is arranged in a way that does indeed pick out
a preferred state of rest. We know this because when we look around with our telescopes
we see the great majority of galaxies moving away from us at roughly the same speed in
every direction. But this can only be true of one observer, because someone moving rapidly
away from us and into space would see those galaxies ahead of her, which she is catching
up with, moving slower than those behind her. Moreover, we have good evidence that the
galaxies are uniformly distributed in space, at least when their positions are averaged over
a sufficiently large scale—that is, the universe seems to be the same when looked at in any
direction. From these facts, we can deduce that at each point in space there will be one
special observer who sees the galaxies moving away from her at the same speed in every
direction.3 So the motions of the galaxies pick out a preferred observer, and hence a preferred
state of rest, at each point in space.
Another way to fix a preferred family of observers is to use the cosmic microwave background.
These preferred observers see the CMB coming at them at the same temperature
from all directions in the sky.4
Happily, the two families of preferred observers coincide. The galaxies appear, on average,
to be at rest in the same reference system in which the CMB comes at us at the same
temperature from all directions. So the universe is organized in a way that picks out a preferred
state of rest. But this fact need not contradict the principle of the relativity of motion.
A theory can have a symmetry that is not respected by its solutions. To the contrary:
Solutions of theories often break the theories’ symmetries. The fact that there is fundamentally
no preferred direction in space does not prevent the wind from blowing from the north
today. Our universe represents just one solution to the equations of general relativity. That
one solution can be asymmetric—that is, it can include a preferred state of rest—without
contradicting the principle that the theory has a symmetry. The universe might have started
off in a way that broke the symmetry."