humanino said:
I see your point of view : nobody knows where QM comes from.
The principles of QM cannot be derived. Yet the wave equation can be derived. Schrodinger equation can be obtained from the classical hamiltonian by using the operator representations for p and E. In turn, those can be derived in the Hilbert space. The only thing you must postulate can be for instance the correspondance between the classical Poisson bracket, and the commutation rules in QM.
Can classical mechanics be demonstrated as well ?
That is incorrect. We KNOW where QM comes from. We know where a lot of physics came from. We however have no explanation for why certain things are that way. Physics are not meant to explain. Our understanding of our world is based on our ability to describe with accuracy how things behave.
Unlike people who work in other areas of our society who have no qualms in giving reasons (sometimes with alarming certainty that they are right) why certain things occur, we can only go by what we can test and verify. We dare not go beyond that by offering things that we simply have no business in saying. That is not a weakness, but the strength of physics and well-defined sciences that is unmatched in other areas of study. The fact that something WORKS seems to be sniffed and trivialized at.
When I used to teach intro physics in college many years ago, I came in the first day and wrote on the board "Conservation of Energy (or mass/energy)" and "Conservation of momentum (both linear and angular)".
I then told the students that throughout their undergraduate career, EVERYTHING they will be studying are nothing more than various manifestations of those two principles. Think about it. All the things you will be studying in undergraduate classical mechanics, E&M, QM, Thermo, etc, etc., are nothing more than various manifestation of those two principles!
Now, if you have learn anything about Noether theorem, you would know that for every conservation law, there is a corresponding symmetry principle behind it. So the conservation law is nothing more than a manifestation of that symmetry. The two conservation laws I mentioned above are directly due to the time-symmetry of our physical universe and the translation symmetry/isotropic nature of classical empty space.
These two symmetry principles are NOT DERIVABLE! They are just the way our universe is! These, in fact, are our starting postulates for almost all of our physical description of our universe! [I'll smack anyone with a large boson who brings up the CP violation in some weak decay events :)]
Again, this is why physics is physics and NOT mathematics. One should not confuse between the two and then think that it is why QM, for example, has a problem.
Zz.