  To simplify things, in our discussion we shall focus on non-factorizable models of the EPR/B experiment that satisfy λ-independence (i.e., the assumption that the distribution of the states λ is independent of the settings of the measurement apparatuses). Superluminal signaling in the EPR/B experiment would be possible in theory just in case the value of some controllable physical quantity in the nearby wing could influence the statistics of measurement outcomes in the distant wing. And in non-factorizable models that satisfy λ-independence this could happen just in case the following conditions obtained: