The finite sigma-algebra is partitioned by the nonempty eventsThese are its atoms. Define the random variableand give it any finite value on the union of the null atoms. It is -measurable and integrable. Every is a union of atoms, soThis constructs the requested variable directly, without invoking the general existence theorem for conditional expectation.
Uniqueness means almost sure equality. Suppose that two -measurable integrable random variables and satisfy the integral identity from part (a). The event belongs to , and henceThe integrand is nonnegative and is positive precisely on , so . Interchanging and gives , and therefore almost surely.
The atom formula also provesLet . Then by Markov inequality, whileThe uniform absolute continuity for a finite measure makes the right-hand side uniformly small as . Thus is uniformly integrable. The Martingale convergence theorem now supplies an integrable random variable such that both almost surely and in .
Let . The limit from part (c) is -measurable because each is. If , then for some , and for every ,The convergence lets us pass to the limit and obtain .
The sets on which this identity holds form a Dynkin system, and is a generating pi-system. The Dynkin lemma therefore extends the identity to every . Consequently has both defining properties of , established here without appealing to the general existence theorem.
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