You are jumping too far in your assessments. Remember, you asked just for a "few more words". The conclusions you made aren't possible from the short outline I made. It was just meant to explain my reasoning and my intuition, nothing else.
xts said:
3. Your model is not related by any means to QM - it does not utilise any QM basic ideas (especially about the probability of experimental outcome being equal to square of modulus of deterministically evolving wavefunction)
Of course it relates to QM, but I'm reconstructing measurement theory, so it's different and certainly QM framework as it stands is completely incapable of addressing these issues, but that's the whole point of course.
QM is however something that is explained as "correspondence limit". But again, the whole justification for why reconstruction of QM is necessary is the rest of it - unification and QG.
QM and GR are correspondence limits and serve as early reality checks. So reproducing QM ang GR in the appropriate limits are just reality checks. But that's not the point, the point is wether I will succed at the unifications.
In my picture, the state space (analog of hilbert space; I ) is defined by the information structures that encode the observer. I construct this space from combinatorics and from lossy datacompressions. Fouriertransform with a lost phase informaton os you get powerspectrum is just a simple example that often relates q and p.
From this state space, one can define, at each state, a "differential space" which is defined by the possible ways the original information was wrong, but which respects information capacity. The way this space is constructed, implies that it has a builting arrow of time. And the time evolution is like a random walk on a evolving map. But during the walk, the map is distorted, so it's generally onlt the differential evolution that is unitary. The finite evolution contains feedback that causes the structure on which the random walk takes place to evolve.
This does not contradict QM, since unitarity is maintained as long as we consider eqvuivalent external observers, such as we do when computing S-matrix for example.
What I'm talking about are like measurement theory for open systems, but desribed from the inside.
Probabilites are defined from counting permutations of microstates. However there is no born rule simply because I don't need it in the basic construction. However, just for the sake of correspondence I expect to be able to explain it in the appropriate limit.
Edit: I realize this is clearly dritfing off topic so i won't entertain this disucssion more in this thread. Given time, I hope to be able to publish some papers. Until them a few words is all there will be I'm afraid. There are several reasons for that, it's not just about forum rules :)
/Fredrik