 According to the quantum formalism, for a system with wave function \(\psi\) the probability density for finding its configuration to be \(q\) is \(\lvert\psi(q)\rvert^2\). To the extent that the results of measurement are registered configurationally, at least potentially, it follows that the predictions of Bohmian mechanics for the results of measurement must agree with those of orthodox quantum theory (assuming the same Schrödinger equation for both) provided that it is somehow true for Bohmian mechanics that configurations are random, with distribution given by the quantum equilibrium distribution \(\lvert\psi(q)\rvert^2\). Now the status and justification of this quantum equilibrium hypothesis is a rather delicate matter, one that has been explored in considerable detail (Dürr, Goldstein, &amp; Zanghì 1992a). Here are a few relevant points.