  To see the nature of non-locality postulated by the minimal Bohm theory, consider again the EPR/B experiment and suppose that the measurement apparatuses are Stern-Gerlach (S-G) magnets which are prepared to measure z-spin. In any run of the experiment, the measurement outcomes will depend on the initial positions of the particles and the order of the measurements. Here is why. In the minimal Bohm theory, the spin singlet state denotes the relevant state of the guiding field rather than the intrinsic properties of the particle pair. If the L-measurement occurs before the R-measurement, the guiding field and the position of the L-particle at the emission time jointly determine the disposition of the L-particle to emerge from the S-G device either above or below a plane aligned in the z-direction; where emerging above (below) the plane means that the L-particle z-spins ‘up’ (‘down’) about the z-axis and the L-apparatus ‘pointer’ points to ‘up’ (‘down’) (see Fig. 4 above). All the L-particles that are emitted above the center plane aligned orthogonally to the z-direction, like the L-particles 1-3, will be disposed to spin ‘up’; and all the particles that are emitted below this plane, like the L-particles 4-6, will be disposed to spin ‘down.’ Similarly, if the R-measurement occurs before the L-measurement, the guiding field and the position of the R-particle at the emission time jointly determine the disposition of the R-particle to emerge either above the z-axis (i.e., to z-spin ‘up’) or below the z-axis (i.e., to z-spin ‘down’) according to whether it is above or below the center plane, independently of the position of the L-particle along the z-axis.