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nucl34rgg said:Knowing the axiomatic framework upon which QM is based, what the limitations are of QM, along with how to apply QM is equivalent to understanding QM.
We don't know the limitations of QM. And, as I said, we don't know how to apply QM except in a "rule of thumb" way. The ambiguous part, as I said, is knowing when a measurement has been made. What's a measurement? The formalism doesn't tell you, but it does tell you that after a measurement, the system will be in a eigenstate of the operator corresponding to the observable being measured. So the rules depend crucially on knowing what a measurement is, and they don't tell us. I would say that this is very different from classical physics. For classical physics, it's also true that whether something is a measurement or not is fuzzy. But the laws of physics don't depend in any way on that distinction.
There is an inherent ambiguity in the Rules of Quantum Mechanics. Suppose we prepare a system in some state, and then later we let it interact with a detector, and then even later, we perform some other measurement on it. There are two different ways to analyze it: (1) We can consider the detector to be performing a measurement of some observable. In this case, the wave function collapses to an eigenstate after interacting with the detector, and we use this eigenstate to compute the probabilities for the final measurement. (2) We can consider the detector to be a quantum system in its own right, evolving according to Schrodinger's equation. In this case, the detector doesn't perform a measurement, and there is no collapse of the wave function to an eigenstate.
In principle, these two different ways of analyzing the situation could lead to different results, because if we treat the detector as a quantum system, there is the possibility for interference effects. In practice, interference effects involving macroscopic objects are unobservable.