Two sigma-algebras are independent if every event in one is independent of every event in the other:
The same formula defines independence of the generating collections when restricted to their members.
Independence of the full sigma-algebras immediately gives independence of their generating pi-systems. For the converse, fix . On , define finite measures
They have the same total mass and agree on by assumption. The supplied measure-uniqueness theorem makes them equal on . Thus the independence formula holds for every and every .
Now fix such an arbitrary . The measures and on have equal total mass and agree on . A second application gives equality on all of . This proves independence extended from generating pi-systems.
For each , the collection of events , together with the empty event, is a pi-system. Its generated sigma-algebra is , because the half-lines generate the Borel sigma-algebra and inverse images preserve intersections and the sigma-algebra operations.
The displayed probability identity says precisely that these two pi-systems are independent. Part (ii) makes and independent, which is the definition of independent random variables. Conversely independence of the random variables applies to the half-line events and gives the identity. Thus the joint cumulative distribution function factors exactly when the variables are independent.

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