“…Like in standard quantum theory, the notion of complementary observables is represented by the noncommutativity of the corresponding operators and that of entanglement by the nonfactorability of the vector-state. It has been shown in (Uzan 2014;2020) that Bell's test, its extensions to non-local correlations and its consequences regarding causation, which have already been successfully used in the strict quantum domain (Clauser and al 1969) where S(a a') is the mean value of the product of outcomes of the joint measure of observables A and A'(which have been normalized), and similarly for the other terms, with the following two theoretical bounds: the Bell bound, which is 2, marking the border between classical correlations due to a local determination and non-local correlations (Bell 1964) (Uzan2014a). If the absolute value R of the correlation factor is greater than these correlations can be regarded as causal interactions and if R is less than , the correlations studied are no-signaling, they cannot be explained by the exchange of any signal between the two considered sub-systems.…”