Fix and a finite horizon . Begin under Wiener measure with , and let bound . The bounded progressively measurable process is an admissible Itô integral integrand. Put
The Novikov condition follows from . With , the Girsanov theorem says that is Brownian motion. Therefore a weak stochastic solution exists, since
Consistent finite-horizon densities on canonical continuous path space give a solution for all finite times. No uniform integrability at infinite time is needed for this extension.
For uniqueness in law, take any weak stochastic solution under a measure and reverse the change of measure:
Again the Novikov condition holds. Under , is Brownian motion, so the law of is the fixed shifted Wiener measure. Substitution of gives
Under shifted Wiener measure, the stochastic integral on the right has a fixed measurable version as a functional of the canonical path. It can be defined by simple predictable processes converging in the integrand norm and an almost surely convergent subsequence of their integrals. Equivalence of the two finite-horizon measures preserves that version. Thus for every bounded measurable path functional ,
The right-hand side depends only on , not on the chosen solution. This proves uniqueness in law on every finite horizon, and hence on the whole continuous path space. This is Weak existence and uniqueness in law for an additive-noise SDE with bounded drift. For merely measurable , one should not assume that naive deterministic left-endpoint samples of converge; the predictable approximation is the appropriate definition.

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