That does not follow. It is sufficient for the separate measurements to be space-like separated, not simultaneous.
For creating a problem for relativity, this is, of course, sufficient. Because after this the only choice is (a) to become mystical, by rejecting realism and causality (b) to accept hidden FTL causal influences.
Rendering your preferred frame a superfluous bit of metaphysics not needed for predicting observable physical behaviors.
Superfluous only if you reject realism and causality and are satisfied by unexplained correlations.
And, of course, adding metaphysical elements is nothing wrong. The greatest discovery of physics - the atomic structure of matter - was for a long time only a metaphysical element.
They are stupid appeals to intuition, because they are alternatives to parsimonious prediction of observable physical behaviors from the physical theory.
If you think that scientists have to restrict themself to parsimonious prediction of observable physical behaviors, I simply disagree. Such predictions are useful in technological applications, and allow to falsify wrong theories in science itself, thus, are an extremely important part of science, but certainly not all.
As you admit in the next paragraph, there are physically plausible, consistent-with-observation solutions to GR which seem to inform our view of phenomena in our galaxy. Since our galaxy does not admit a global time coordinate, it follows that a purported interpretation which contains a global time coordinate cannot apply to our galaxy and is not consistent with GR.
Not quite correct. The phenomena in our galaxy allow for a global time coordinate. The only natural candidate for an equation for a preferred time coordinate is harmonic time, the harmonic equation is an evolution equation, thus, harmonic time will be defined by the initial conditions. In case of a black hole, the initial time will be more or less Minkowski time before the collapse. The interesting point of this is that the part after horizon formation is not covered by this harmonic coordinate. But, once this part is also not observable from outside, all what we know about the galaxy up to now allows for a global time coordinate.
That's not an "interpretation" -- that's a new physical theory. Until you explain what is wrong with the 1916 Schwarzschild solution, you have said nothing except the GR that you preach is not actually GR.
There is nothing wrong with the Schwarzschild solution, harmonic coordinates are known for it and simple. How you name it is nothing I have to care much, I would suggest to name it the Lorentz ether. Its equation is the Einstein equation of GR and the harmonic equation to identify the preferred coordinates.
Only if you demonstrate your departure from parsimony is anything other than a wild-eyed-guess predicated on slovenly catering to your personal prejudices.
I don't have to demonstrate that name-calling against this interpretation or theory is impossible. I can freely acknowledge that name-calling is possible and ignore it.
A physics theory is a mathematical model of the behavior of a wide class of related phenomena. When you add your universal time to GR, you better have worked out how your gravity theory works differently than the 100-year-old one and the evidence for the addition.
Once in this interpretation of GR the equation of GR - the Einstein equations - remains unchanged, all what has to be modified is that one has to add an equation for the preferred coordinates - which I have, the harmonic equation - and to specify that one of the coordinates is a global time, thus, mathematically has to be time-like.
Locally this is always possible. But it leads to some additional global restrictions.
What is evidence for the addition? First, a large number of solutions - all those with nontrivial topology - are simply excluded as unphysical. Observing them would falsify this interpretation. Have you observed it?
Then, there is Goedel's rotating universe. It does not allow for a global time coordinate, thus, would falsify the interpretation. The global rotation of the universe is observable, and the observation gives zero.
A little bit more subtle is what happens with models of a homogeneous universe, the FLRW ansatz. Here, only the flat ansatz would describe a universe which is really homogeneous, even in the preferred coordinates. This gives not really an additional prediction - a universe with nonzero curvature allows for harmonic coordinates - but it would no longer be a homogeneous universe. But if we add the hypothesis that the universe is, in the large and approximately, homogeneous, we obtain an additional prediction with a very clear number - 0 for the global spatial curvature. Which nicely corresponds to reality.
It's not enough to claim Einstein, Schwarzschild and every GR researcher for the past 100 years was wrong -- you have to do their job better or you aren't doing physics; you aren't doing science-as-an-human-endeavor, you aren't contributing to science-as-a-store-of-knowledge.
It would be, of course, not enough - but I'm not doing this, so that this is irrelevant.
de Broglie-Bohm mechanics is about particles and whimsical trajectories. Quantum Field Theory is about fields (also antimatter, how particles get mass, why gold isn't silver-colored, etc.)
It is, unfortunately, usually presented in this way. There is no necessity for this. I prefer to present it for general configuration spaces. There is some restriction, the game works only for Hamiltonians of the form $$H = p^2 + V(q)$$. This restriction may seem serious, but for relativistic field theories it is not problematic at all. The general form is of type $$L = \dot{\phi}^2 - F(\phi, \partial_i\phi)$$, thus, gives quadratic momentum dependence. So, a relativistic field theory is in itself not a problem for dBB theory. It requires a hidden preferred frame, that's all. The case of a complely scalar field is completely unproblematic, gauge fields become problematic only if one wants to get rid of gauge degrees of freedom, a gauge field where gauge-equivalent field configurations are considered as different field states can be covered without any problem in the same way. Fermions are more problematic, but there are ways to handle them. Of course, I prefer the way suggested in
http://arxiv.org/abs/0908.0591 without mentioning dBB theory, where a pair of Dirac fermions (interpreted as an electroweak pair) is constructed out of a scalar field with symmetry breaking. Given that scalar fields are unproblematic, the consequence is that pairs of Dirac fermions are unproblematic too. But there are also other proposals for fermions in dBB-like field theories.
I'm sorry, I though you were talking about adaptions of dBB that actually were relevant, not some antique dinosaur.
Name-calling based on the date then a theory has been presented is irrelevant.
http://arxiv.org/abs/quant-ph/0601095 rejects causality, thus, is IMHO not even worth to be read.
http://arxiv.org/abs/1402.7256 is a nice article, I have not found anything serious to object during a short overview.
http://plato.stanford.edu/entries/qm-bohm/#li is also a nice overview article, but also seems unaware of standard dBB field theory. "Bohmian mechanics does not account for phenomena such as particle creation and annihilation characteristic of quantum field theory." is clearly false, this is handled in a straightforward way in dBB scalar field theory.
The article
http://philsci-archive.pitt.edu/4567/1/philsci-gr-needs-no-interp.pdf is quite interesting, may be I will add some further comment about it.