"suppose that Alice and Bob share a Bell state
$| \Phi ^ { + } \rangle =2 ^ { - 1 / 2 } ( | 00 \rangle + | 11 \rangle ) = 2 ^ { - 1 / 2 } ( | + + \rangle + | - - \rangle )$ . If Alice measures the Pauli Z observable on her system, then Bob can guess the outcome of her measurement with
certainty. Also, if Alice were instead to measure the Pauli X observable on her
system, then Bob would also be able to guess the outcome of her measurement
with certainty, in spite of the fact that Z and X are incompatible observables."