Ugh, this is a lot of words. Sorry.
Hurkyl has just started talking about ignorance interpretations, which makes me wonder if he doesn't intend for wavefunctions to be the actual states of things after all.
That's to describe the way
you're thinking about things. An ignorance interpretation is "reality is in one of those states, but I don't know which and I'm assigning probabilities to capture my ignorance". "Probability distributions are real" is not an ignorance interpretation.
mitchell porter said:
OK, so you flip a coin, I don't see the outcome. I could say that it is actually heads or that it is actually tails, I just don't know which. Or, I could say that the actual reality is 50% heads and 50% tails ... I am just to believe that the probability distribution itself is the reality - whatever that could mean.
Right, we start with something like this. And we run with classical mechanics for a while to get used to the shift in perspective.
While before we described the coin with an actual value "Heads" or "Tails", we now describe the coin with a random variable.
We consider the fact that when I observe the coin, I will see one of the two values in the set {heads, tails}. Ah, that's accounted for in the fact the sample space of the random variable is the set {heads, tails}.
The fact that actual observation sees only one outcome? The trivial fact that P(X=a | X=a) = 1. We just used to using conditional probabilities with random variables, when before we talked about absolute probabilities involving indeterminate variables.
Happy? The important thing at this point isn't that you think "this is a wonderful way to think about classical mechanics" -- it's that "huh; this is self-consistent and physically indistinguishable to the ordinary way of thinking, even if it seems a little weird."
Now, let's continue applying this to quantum states. Traditionally, we think of results of measurements being classical ignorance probabilities across definite outcomes. But now, we're thinking of probability distributions as reality -- but it's a bit more convenient than the classical case, because it's already built into the mathematical description of quantum state -- e.g. a quantum state could be written as a weighted positive linear combination of density matrices -- rather than us having to layer probability theory on top of the quantum state space. Also, quantum states are somewhat more general.
Now we run into the question you had before:
Suppose that we have a qubit whose density matrix is as described. What is the physical reality?
The answer is: the physical reality is the wave-function. Everything else follows from that. I mentioned a quantum state earlier that was a mixed state that could be written as
60% Z+ and 40% Z-
Since we made ourselves happy with probability distributions as reality, it's not difficult to understand a quantum particle as really being in this state that is a probability distribution over pure states.
We understand that this is completely indistinguishable from a definite-outcomes interpretation where we view it as an ignorance probability over definite states.
Also, we can understand a quantum particle as really being in the state
20% Z+ and 40% Y+ and 40% Y-
Now, you were having a problem with the fact these were different sums describing the same quantum state. What is the reality?? But the question was already answered -- reality is the wave-function. A little thought should convince you that the difference between the sums is entirely superficial -- the two decompositions cannot be distinguished by any physical experiment, and therefore we shouldn't be quick to insist that we must interpret them as different.
(and if it doesn't, try computing the expectation of some observable -- say, spin around the axis half-way between the Z+ and Y+ axes)
Are you with me this far? Again, I've not said anything to answer "why should we think this way" (except possibly for comments about things being physically indistinguishable), but instead have discussed "why
can we think this way".
We've seen that something we might have thought as classical ignorance probabilities weighted 60% Z+ and 40% Z- give the same results as thinking of a qubit in a certain mixed quantum state. And that classical ignorance probabilities weighted 20% Z+ and 40% Y+ and 40% Y- gives the same results as thinking of the cubit in a certain mixed quantum state.
And we saw the interesting new physics that the two mixed states are the same -- and the interesting result that the two superficially different classical ignorance probabilities actually describe the same physics... something we might not have otherwise noticed if we
weren't thinking about mixed states.
The next two major points are the relative state of a subsystem (I was probably going to talk about the entangled photon scenario as an example), and the fact that relative states provide a way around the old no-go theorem -- when a system undergoes unitary evolution, its subsystems can decohere.
Can you see where I'm going with these, or do I need to continue?
Anyways, once we have these points, we have the basic premise behind the family of decoherence-based
interpretations of quantum mechanics -- the ignorance probabilities that QM was traditionally thought in terms of work out to be indistinguishable from mixed states. Mixed states can be produced by decoherence of relative states of subsystems. Decoherence of subsystems can occur through unitary evolution ala the Schrödinger equation. We have a framework where unitary evolution at least has the potential to produce the same mathematical descriptions of state that appear in a collapse-with-ignorance-probabilities point of view.
Aside: the "good" reason to use ignorance probabilities I mentioned earlier was Occam's razor -- in classical statistical mechanics, the decomposition of a probability distribution into a weighted combination of individual states is absolute and eternal, unlike the weighted combinations that appear in the framework I described above. For classical mechanics, we lose nothing (except possibly a wider point of view) by deciding to interpret everything as ignorance probabilities, so Occam can be applied. But in QM, we
do lose something by insisting on thinking in terms of ignorance probabilities, so Occam doesn't apply anymore.