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bhobba said:Well Copenhagen states the state is subjective, the ensemble states its a conceptual very large number of possible outcomes (actually infinite - but I don't know about you but I can't imagine that) associated with each observable.
But it seems to me that there is a "preferred basis" problem with such an ensemble view. In a classical use of ensembles, you have some undetermined variable, such as the precise location of the system in phase space, and the ensemble consists of many similar systems in which this variable has a definite value (but different in different elements of the ensemble). So you could try to do something similar with quantum uncertainty: You have an uncertain variable, such as the spin of a particular particle along the z-axis. And then you have an ensemble of similar systems that differ in the value of that variable.
But here's where the basis problem comes in, it seems to me. Why in the ensemble do the individual systems have definite values for spin in the z-direction, as opposed to, say, spin in the y-direction? You could answer: Because spin in the z-direction is what we're measuring---there would be a different ensemble for each kind of measurement you might want to perform.
Okay, that's fine for some purposes, but presumably the measurement device and the observer doing the measurement are themselves quantum systems, although very complex ones. Presumably what it is that you're trying to measure is a fact about the configuration of atoms making up the measurement devices. And the fact that the outcome was "spin up in the z-direction" rather than "spin up in the x-direction" is again a fact about the configuration after the measurement. So it seems to me that in principle, it should not be necessary to specify what is being measured, because that is itself a property of the state.
The other view is every theory, every single one has things that are simply accepted as true - that improper mixed states become proper ones is simply one that's accepted as true
Well, I'm fine with it just being an additional assumption of the theory. However, there is no way for that transition to take place in a basis-independent manner. The usual assumption, in agreement with our intuitions and observations, is that the transition happens so that after the transition to proper mixed states, macroscopic variables--whether cats are alive or dead, whether you are in London or Beijing--have definite values. That seems to me to be a breaking of the basis-independence of the quantum formalism.
I know that there is a reason for "preferring" a position basis for macroscopic objects, because only in the position basis are interactions local. That's a clue, but it isn't an answer. The question is whether adding a transition from improper to proper mixed states involves some violation of quantum mechanics, or is it derivable from quantum mechanics, or is it merely consistent (thought not implied by) quantum mechanics? I don't think that just assuming that it happens actually answers the questions.