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RandallB said:I don’t find the measurement solution any more satisfying than the QM case. At least not until the two theories can predict different results that experiments can select between.
I wonder if you're not sure exactly what is meant by "the measurement problem." This is actually a serious problem for Orthodox QM, which literally gives two different dynamical rules for the evolution of wave functions (depending on whether or not a "measurement" is being made). The *problem* is that the theory does not say what constitutes a "measurement", so it is, to use Bell's phrase "unprofessionally vague and ambiguous." This is the problem that is supposed to be raised by Schroedinger's cat: if you follow the time evolution described by Schroedinger's equation, you get nonsense results like cats being in superpositions of alive and dead. Since we never *see* such states, that description must be wrong. The wave function must have collapsed, at some point in the development, to a more definite state. But where did this collapse occur? When we consciously registered the state of the cat? Or when some photons flew from the cat and interacted with our eyeballs? Or when some poison molecules interacted with the cat? Or when the hammer interacted with the vial of poison? etc. The theory just doesn't tell us where along this chain the wf collapses, i.e., where the normal Schroedinger time evolution gives way to the alternate "collapse" dynamics. Put another way, the problem is that OQM doesn't seem able to explain why experiments have definite outcomes; or rather, the only way it can explain why experiments have definite outcomes, is by importing some very dubious concepts (such as "measurement") into the fundamental laws of nature where they don't seem to belong. This is a serious foundational problem for the theory.
In Bohmian Mechanics, we simply do not have this problem. Because particles always have definite positions (even when not being "measured"), there is no problem whatsoever associated with measurements having definite outcomes. The needle on your detector ends up in some definite spot (registering some definite outcome) because it's made of *particles* and particles are always in some definite spot. So, there simply is no problem associated with measurement in Bohm's theory. Measurement is just another ordinary physical process, the same in principle (meaning, obeying the same dynamical laws) as any other "non-measurement" physical process.
Your worry that the two theories make the same predictions (and that it is therefore difficult to tell which one is right) is a completely different issue. Yes, it would be nice if the various theories made different predictions so we could just do the experiment and rule some of them out. But it's not so, so, if we're going to have an opinion about which theory is better, it has to be based on some criteria other than agreement with experiment. (For example, whether a given theory is plagued by the measurement problem, or whether it asks us to believe in gazillions of copies of unobservable parallel universes inhabited by mindless hulks, etc...) And by the way, this is not at all an abnormal thing in the history of science. Lots of times people have been confronted with differing theories which make the same predictions (at least for the time being).