Bell's theorem makes precise an obstruction to reproducing
quantum correlations with
a local causal completion. Let
measurement settings be
a,b, outcomes
A,B=±1 and
a more complete state
λ. Bell locality factorizes
P(A,B∣a,b,λ)=P(A∣a,λ)P(B∣b,λ); setting independence takes the distribution of
λ to be independent of the freely chosen settings. These assumptions imply
a Bell inequality. For example deterministic assignments satisfy
∣A(B+B′)+A′(B−B′)∣≤2, and averaging gives the
CHSH bound
∣S∣≤2. The
stochastic version follows by averaging local response
probabilities too.