  In various counterfactual and probabilistic accounts of causation violations of PI entail superluminal causation between the setting of the nearby measurement apparatus and the distant measurement outcome, whereas violations of OI entail superluminal causation between the distant measurement outcomes (see Butterfield 1992b, 1994, Berkovitz 1998b, section 2). Thus, it seems that theories that violate PI postulate a different type of superluminal causation than theories that violate OI. Yet, as Berkovitz (1998b, section 2.4) argues, the violation of PI in Bohm's theory does involve some type of outcome dependence, which may be interpreted as a generalization of the violation of OI. In this theory, the specific R-measurement outcome in the EPR/B experiment depends on the specific L-measurement outcome: For any three different directions x, y, z, if the probabilities of x-spin ‘up’ and y-spin ‘up’ are non-zero, the probability of R-outcome z-spin ‘up’ will generally depend on whether the L-outcome is x-spin ‘up’ or y-spin ‘up’.  Yet, due to the determinism that Bohm's theory postulates, OI trivially obtains. Put it another way, OI does not reflect all the types of outcome independence that may exist between distant outcomes.  Accordingly, the fact that a theory satisfies OI does not entail that it does not involve some other type of outcome dependence. Indeed, in all the current quantum theories that violate factorizability there are correlations between distant specific measurement outcomes — correlations that may well be interpreted as an indication of counterfactual superluminal causation between these outcomes.