vanesch
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Count Iblis said:The Born rule can be derived from a much weaker postulate. All you need is a postulate that says that if the wavefuntion is in an eigenstate of an observable, then measuring it will yield the corresponding eigenvalue with probability 1.
But the difficulty resides in the following: suppose I give you the physical description of an apparatus. What's the physical description of an apparatus ? I would say, a beginning state vector and a corresponding hamiltonian, no ? That's the quantum mechanical description of an apparatus. Now, given that, and only that, how do you deduce WHICH KIND OF MEASUREMENT BASIS goes with that apparatus ?
One can in fact do that, by fully assuming quantum theory all the way. One will then see that the interaction hamiltonian is such, that certain subspaces of states of the "system-under-study" couple with subspaces of states of the "measurement apparatus" in a kind of coarse-grained Schmidt decomposition of the overall state. Furthermore, if one introduces a quantum description of the environment (thermodynamical heat reservoir), usually, these couples ("subspace of states of measurement apparatus" and "subspace of states of system-under-study") remain stable against interaction with the environment ; again, by assuming that all this has a quantum description and that we don't leave the quantum-domain or the schroedinger equation. If one calls these subspaces of states of the measurement apparatus "the pointer states", then one can see that they are close to "classical states with different outcomes".
The whole above story is called "decoherence" and singles out specific subspaces of states of "macroscopic systems" which remain stable against interaction with the environment. From it, one can derive as such the "stable pointer states" and from this, and the interaction hamiltonian, one can then derive the "measurement basis" that the apparatus applies to the system.
But in order to do all this, we cannot collapse the wavefunction and we have to assume that quantum interactions and state descriptions are valid all the way up.
There is of course a way out, and that is by saying that there IS a preferred measurement basis, which is "position measurement". All measurements are then position measurements. When you do that, you can arrive at Bohmian mechanics, but the interpretational issues of Bohmian mechanics are not as simple as one might think at first, because the Bohmian ontology consists of two interacting worlds: the particle/position world (which we are used to from Newton), and on the other hand the quantum-mechancal wavefunction world which continues to evolve with superpositions and all that, just as in non-collapsing MWI quantum theory. This last world influences the former (the particle world), but not vice versa: the particle positions have no influence on the wave world. The problem as many people see it with Bohmian mechanics (except, of course, proponents of this view), is that the interaction between the wave world and the particle world is not relativistically invariant.