Each is a bounded Borel measurable function of , including the specified value at . Therefore is an adapted process for and consists of integrable random variables.
Fix an atom of a sigma-algebra in with positive probability, corresponding to the dyadic interval , with . By the uniform distribution, each half has conditional probability . The conditional expectation of on that atom is therefore
The middle values cancel. On the zero-probability atom the conditional expectation can be chosen as zero, agreeing with our version of . Hence
so is a martingale. This is the dyadic slope martingale associated with the Lipschitz function .
The uniformly integrable martingale convergence theorem states that a uniformly integrable martingale has an integrable terminal random variable such that almost surely and in the L1 norm, and
The last identity follows by passing to the limit of a sequence in for and , using convergence in L1.
Part (b)(iii) verifies uniform integrability for , so
Moreover almost surely. In this particular problem the common bound also yields convergence in Lp for every finite , including convergence in L2: the dominated convergence theorem applies to . General uniform integrability alone does not assert these higher-power conclusions.
Choose as the pointwise limit of a sequence of where it exists, and as zero otherwise. The convergence event and every are -measurable, so this is an exactly -measurable version, bounded by . Part (a)(ii), the Doob-Dynkin lemma, supplies a Borel measurable function on such that . Applying scalar clipping to with bounds preserves that equality and ensures everywhere.
Part (c)(ii) and the conditional expectation formula from part (b)(iv) now give
Since the indices form a countable family, these identities may be taken on one common full-probability event.
For fixed , both the slope and the displayed average are constant on the atom , whose probability is . An equality holding almost surely of these constants forces the deterministic equality
Sum over . The telescoping sum gives
Thus the desired identity holds at every dyadic endpoint, including , without evaluating the undefined slope at .
Finally, given , take dyadic endpoints . The Lipschitz condition implies , and the bound on the Borel measurable function gives
Passing to the limit of a sequence proves
This is a martingale proof of the integral representation of a Lipschitz function. It constructs a bounded Lebesgue integrable function representing the increments of , and in particular proves absolute continuity of . No prior assumption that has a derivative is needed.

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