  The no-signaling theorem demonstrates that orthodox quantum mechanics excludes any possibility of superluminal signaling in the EPR/B experiment. According to this theory, no controllable physical factor in the L-wing, such as the setting of the L-measurement apparatus, can take advantage of the entanglement between the systems in the L- and the R-wing to influence the statistics of the measurement outcomes (or any other observable) in the R-wing. As we have seen in section 5.1.1, the orthodox theory is at best incomplete. Thus, the fact that it excludes superluminal signaling does not imply that other quantum theories or interpretations of the orthodox theory also exclude such signaling. Yet, if the orthodox theory is empirically adequate, as the consensus has it, its statistical predictions obtain, and accordingly superluminal signaling will be excluded as a matter of fact; for if this theory is empirically adequate, any quantum theory will have to reproduce its statistics, including the exclusion of any actual superluminal signaling.