T. Seletskaia has pointed out to me
Arnold Neumaier's paper
"Bohmian mechanics contradicts quantum mechanics", discussed earlier in this thread.
So far as I can see, no-one made the analogy with momentum... If you want this sort of disagreement between Bohmian mechanics and quantum mechanics, you can just consider momentum. The distribution of momenta, exhibited by the Bohmian trajectories corresponding to a generic wavefunction, is not the same as the probability distribution for the momentum observable, predicted by QM for the same wavefunction.
To get a Bohmian, ontological, realist explanation of the quantum momentum operator, you have to include a physical interaction which "measures" the momentum, and you must consider the overall wavefunction for "original system" + "second system which interacts with the first". This is the sort of wavefunction considered e.g. in studies of measurement-induced decoherence; but here you are to consider the Bohmian trajectories corresponding to this overall wavefunction. When you do this, you once again have predictive agreement between QM and BM.
All this would be well-known to modern Bohmians. What's interesting here is that Arnold has found an analogous problem just involving position, which was supposed to be the part of Bohmian mechanics which matches with quantum mechanics in a direct and uncomplicated way. However, to find this problem, he had to consider correlations between position at different times. So we can refine our understanding as follows:
The
single-time distribution for position is the same in Bohmian mechanics and quantum mechanics. The multi-time correlations for
unmeasured position in Bohmian mechanics are
not the same as the multi-time correlations for position in quantum mechanics, just as the distribution for the unmeasured momentum in Bohmian mechanics is not the same as the distribution for momentum in quantum mechanics.
However, if there is a physical interaction such as is required for measurement, then multi-time correlations for
measured position, and a distribution for
measured momentum, are produced, which are the same as in QM. (This was the point of
Marchildon's response.)
While I agree with Arnold's critics, who say that he is ignoring Bohmian measurement theory, I still think it's interesting to grasp the ways in which physical ontology, according to Bohmian mechanics, behaves differently than "quantum appearances" or "quantum intuition" suggest. Though I would not be surprised to learn that this is all old news for Bohmians who have specialized in issues of time (dwell time, time of flight, etc).