Demystifier said:
Also an analogy could help. Suppose that someone said: "I have heard that statistical mechanics always makes the same predictions as thermodynamics. But I want to see how statistical mechanics explains the working of refrigerator. Is there a paper that explains the working of refrigerator by statistical mechanics?" It is likely that there is no such paper, and those who understand both thermodynamics and statistical mechanics will understand why.
Thank you for your response. I think the analogy is useful, but I do not think it fully applies.
Bohmian mechanics involves the assumption of a guiding equation, which is derived from the position space wavefunction of a system, which, of course, is derived via the Schrodinger equation. Assuming certain initial distributions of the initial conditions of the particles in a system governed by such a guiding equation, the probability distribution of particle trajectories will match the shape of the position space wavefunction. Therefore, all of the predictions of Bohmian mechanics will match those of standard quantum theory, (in analogy to the way in which all of the predictions of statistical mechanics will match all of those of thermodynamics). However, we can only be assured that this is the case as long as the predictions of standard quantum theory make use only of a position space wavefunciton. There are certain predictions made in standard quantum theory which make no use of the position space wavefunction whatsoever.
Take, for instance, the standard QM prediction of the expectation value of the product of the outcome of two spin measurements on a singlet state in a Bell test experiment, (which turns out to be proportional to the cosine of the angle between the orientations of the detectors-- in violation of Bell's inequality). This prediction makes no use of position wavefunctions whatsoever. It makes use only of spin operators and the singlet state. Unlike the eigenstates of regular angular momentum, the spin eigenstates are not expressible as position space wavefuncitons. Therefore, in this example, there is no position space wavefunction that we can use to derive the Bohmian guiding equation which is necessary to make predictions in accordance with Bohm's hidden variable theory in the first place. Therefore, it is not at all clear (to me) how Bohmian mechanics is to predict Bell inequality violations.
That said, if there were another way to predict Bell inequality violations using only position space wavefunctions in standard quantum mechanics, then, of course, it would be trivial to see how Bohm's theory would make the same prediction.
It seems that one might predict Bell inequality violations using only position wavefuncitons in standard QM in the following way: Properly define the initial conditions and Hamiltonian for a system of a pair of spin 1/2 particles each moving through differently oriented Stern-Gerlatch magnetic fields. From this derive a position space wavefunction which turns out to give you the right probabilities that the particles will move up or down in their respective analyzers in a way that reproduces the result that the expectation values of the product of the measurements violates Bell inequalities (by being proportional to the cosine of the angle between the orientations of the SG analyzer fields).
However, it seems to me that this is not a viable approach, since there seems to be no difference between the Hamiltonian for such a system in which the two particles are in the entangled singlet state (in which case Bell inequality violations are observed), and the Hamiltonian for such a system in which the two particles are just in a mixed state of spin up and spin down (in which case Bell inequality violations are not observed).
Thank you for the reference. I will see if it answers some of these questions.