  Like in the minimal Bohm theory, the non-separability of the wave function in the EPR/B experiment dictates that the evolution of the particles’ trajectories, properties and dispositions is non-separable, but the behavior of the particles is somewhat different. In the earlier z-spin measurement on the L-particle, the quantum potential continuously changes, and this change induces an immediate change in the z-spin of the R-particle. If the L-particle starts to spin ‘up’ (‘down’) in the z-direction, the R-particle will start to spin ‘down’ (‘up’) in the same direction (see the little arrows in Fig.  4).[20]  Accordingly, the L-measurement induces instantaneous action at a distance between the L- and the R-wing. Yet, similarly to the minimal Bohm theory, while the disposition of the R-particle to emerge above or below the center plane aligned orthogonally to the z-direction in a z-spin measurement may change instantaneously, the actual trajectory of the R-particle along the z-direction does not change before the measurement of the R-particle's z-spin occurs. Only during the R-measurement, the spin and the position of the R-particle get correlated and the R-particle's trajectory along the z-direction is dictated by the value of its (intrinsic) z-spin.