my2cts said:
Staye of what? Eigenstates of what? The reason is that you discuss the wave function without referring to the equation that it is the solution of (!), is that you tacitly presuppose the QM formalism. My point is that we do understand the formalism, but not QM.
It's as I said - position eigenstates. Why didn't you note the key word I said before eigenstate?
The problem is you have got the cart before the horse. What a wave-function is has nothing to do with Schroedinger's equation - its got to do with the foundational axioms of QM which are (as per Ballentine):
1. To every observation there exists a Hermitian operator O such that the possible outcomes are the eigenvalues of the observation.
2. There exists a positive operator P, of unit trace, called the state of the system, such that the expected outcome of an observation O, E(O), is E(O) = Trace (PO). This is called the Born Rule.
Axiom 2 is to some extent determined by axiom 1 via Gleason's theorem (you have to add non contextuality to it).
States of the form P= |u><u| are called pure and because Trace (|u><u|) = 1, <u|u> = 1, hence they are of unit length, which is the normalisation condition you were talking about. It follows directly from the Born Rule.
Consider the eigenvectors |xi> of the position operator X. These, by definition, are position eigenstates. Then, by the properties of Hermitian operators (ie its eigenvectors form an orthonormal basis) we have |u> = Σ |xi>< xi|u> with what I said in the previous post following.
That the wave-function is normalised to 1 and |< xi|u>|^2 is the probability of getting position xi follows directly from the axioms of QM. The Schroedinger equation is not involved.
Where the Schroedinger equation comes from is that the probabilities defined by the Born Rule should not depend on the frame.
I think you are a bit confused about understanding in science. In science you understand something when its explained by known premises - which is exactly what we have in QM. The two axioms I gave are the known premises from which we explain QM phenomena.
The issue here is they are not premises in the mould of the usual ones in physics. That's why people say no one understands QM. But what they really mean is no one understands it in terms of everyday intuitive pictures. That is different from understanding - and why I say - We have met the enemy and he is us.
Thanks
Bill