 The second important thing to notice is how Bohr’s response needs to be implemented in order to block the argument of EPR and Einstein’s later arguments that pose a dilemma between principles of locality and completeness. In these arguments the locality principle makes explicit reference to the reality of the unmeasured system: the reality pertaining to Niels’ system does not depend on what measurements (if any) are made locally on Albert’s system. Hence Bohr’s suggestion that those measurements influence conditions for specifying types of predictions would not affect the argument unless one includes those conditions as part of the reality of Niels’ system. This is exactly what Bohr goes on to say, “these conditions constitute an inherent element of the description of any phenomena to which the term ‘physical reality’ can be properly attached” (Bohr 1935a, p. 700). So Bohr’s picture is that these “influences”, operating directly across any spatial distances, result in different physically real states of Niels’ system depending on the type of measurement made on Albert’s. (Recall EPR warning against just this move.) 