The aim of developing this ether theory was not at all to obtain some modification of the equation to modify some solutions. It was the problem of quantization. I have started with a simple thought experiment of quantum gravity, the gravity variant of the double slit experiment where a test particle possible measures the position. If the interaction was strong enough, then the position of the test particle will be different for different paths of the particle - and the superposition is destroyed by the measurement. Else not.
Now do this with gravity. Then you have to compare the positions of the test particle. For the two cases, that means, for two different gravitational fields. And now remember GR, diffeomorphism invariance, and the hole argument. And you will see that there is no such thing in GR as "the same position" for different metrics.
But the experiment will be the same, it will have a result. Or the test particle is at the same place, then the interaction was not strong enough and the position was not measured, or it was measured, and the superposition destroyed. So, quantum theory gives an observable which does not exist in classical theory.
So, an additional equation, which allows to define the notion "the same position" for different solutions of GR is simply necessary to compute a prediction for this thought experiment. There was a nice candidate for this - the harmonic condition. And, of course, one wants to have a Lagrange formalism for the resulting theory, that's all. It is the simplest solution for a problem which GR cannot solve but quantum gravity has to solve, to be able to compute the results of this simple thought experiment.
The parameter choice \Upsilon>0 leads to nice in principle observable differences, namely stable gravastars and a big bounce instead of a big bang, thus, getting rid of the two most important singularities of GR. And of course this would be visible if the values of \Upsilon would be large enough. Then, the spatially flat universe is the only homogeneous one, thus, clearly preferred for symmetry reasons - a curved one would have to have a center. So, the "in principle observable" is not a problem at all.
PeterDonis said:
No, it means it's speculative. Just as the Standard Model itself was speculative until experiments confirmed its predictions. Work on speculative theories is part of science; however, past history shows that, without experimental input, it's very hard to make progress.
Fine. But I disagree about the role of experiments in the progress. Remember on the greatest success stories of physics at all - atomic theory. How long was it "speculative", in the sense that there was no experimental proof of the existence of atoms? Quite long. Was there no progress in atomic theory over all this time? No, there was a lot of progress. But this progress was mainly explanatory. The things which were already well-known have been interpreted in terms of atomic theory. Instead of simply describing them in terms of unspecified "fields".
If we take the example of atomic theory as a pattern, we should expect that new theories have to start with interpretation and explanation of what has been already reached.
strangerep said:
@Ilja: you claim (iiuc) to have the SM with 3 generations, but I when I searched your paper (0908.0591) for mention of the CKM matrix I found none. Do you derive it somewhere else?
No, the masses themselve are not derived.
strangerep said:
Also, I did not find any discussion about masslessness of neutrinos. (?)
Or, if not massless, a derivation of the PMNS matrix?
There are no reasons to expect they are massless. What the model predicts is that there are right-handed neutrinos, and that they have to be inert. (This also with the additional possibility of exchanging left with right.)
What is predicted are the fermions, the gauge fields, and the charges.
In
http://arxiv.org/abs/0912.3892 I give some qualitative considerations which show that the masses of the neutrinos have to be much smaller than those of the other fermions. And, given that the leptons are more closely associated with the neutrinos, one can for similar reasons expect that their masses are lower than quark masses.
The other qualitative prediction is that the massless part - that with exact gauge symmetry on the fundamental level - is U(3).
I suspect one can make some prediction about the smallness of the CP-violating terms. I would guess these terms will be created only by distortions of the ether, thus, may be even different in different regions and times.
In general I would not expect that the ether model will allow to predict all the details from simple first principles and a few qualitative properties of the model, there will be also some quantative material properties of the ether which will influence the masses.