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Reversed kernels, generator, and martingale problem
Statement
Let have continuous paths on and be Markov on , meaning its conditional future law given the past depends only on its current state; nonexplosive means it remains in throughout this finite interval. Let it have forward generator where is symmetric and . Assume positive marginal densities and positive transition densities satisfy the marginal identity and Chapman–Kolmogorov identity, and that and hold classically. Assume for every that the transition-density integrals can be differentiated in time, the resulting derivatives are integrable, and integration by parts in the state variable has no boundary term.
Define by the Bayes-reversed kernel formula for . Then the reversed process is Markov with transitions . For compact smooth , define the formal adjoint candidate operator The product rule gives the identity with . These Bayes-kernel and formal product identities use only the preceding hypotheses.
For the martingale conclusion, impose additionally the following forward analytic conditions. For every compact , with and , For every and , the actual forward conditional expectation has a version on , solves , and satisfies for each compact smooth and almost every . All coefficient expressions in these conditions are Borel. These are conditions on the original forward transition family.
Under these additional forward analytic conditions, is the extended martingale generator of : for its natural reversed filtration , every compact-test compensated process is a martingale, hence a local martingale. The unconditional formal candidate identity alone makes no martingale or pointwise transition-quotient assertion.
Statement references
Anderson, Section 5, printed pp. 322–324: gives the reverse Kolmogorov-equation approach as context; the full kernel and martingale argument is proved here.
Tang and Zhao, Section 2.2, PDF pp. 3–5: states the reverse-drift formula and explicitly gives a heuristic derivation.
Facts & Assumptions
Given: the positive density, forward equation, regularity, differentiation, and no-boundary-term hypotheses in the Statement; is the formal adjoint of . The additional forward analytic hypotheses are imposed when proving the martingale conclusion.
The Bayes-reversed kernels are probability kernels and compose in reverse order by the forward marginal and Chapman–Kolmogorov identities. Bayes-reversed transition kernels for a diffusion
The forward backward-Kolmogorov and local weighted integrability conditions in the Statement imply the finite-time reversed compact-test martingale identity by differentiating and integrating in time. Forward Kolmogorov duality gives reversed martingales
The explicit local weighted bound makes finite for each compact smooth test; Fubini then justifies the conditional time integral. No varying-endpoint transition quotient or partition limit is used. Fubini's theorem for L^1 functions on a sigma-finite product
For , symmetry of and the product rule give This is an algebraic expansion of the displayed formal adjoint.
Proof
Given: the process and base hypotheses in the Statement; impose its additional forward analytic conditions for steps 2.1–3.1.
Bayes' formula gives the one-step reversed conditional law: for Borel , the joint density of is , while the later marginal is . Their ratio is exactly . The kernel is normalized and composes by [F1], so the finite-dimensional reversed laws have the Markov factorization with these kernels.
Put and . Under the additional forward analytic conditions in the Statement, the hypotheses are exactly those of [F2], so that result gives the compensated-test martingale with coefficient . Thus the displayed operator is the extended martingale generator. This argument uses the finite-time product identity for the actual forward transition family.
Under the same additional conditions, [F2] gives for and every bounded Borel the identity . Reversed Markov conditioning and [F3] therefore give zero conditional expectation of every compensated increment given , as required. The explicit bound gives a true martingale, hence a local martingale.
Expanding the adjoint in step 2.1, the drift part contributes . The second-order product rule contributes after summing and using symmetry of . Divide by and use to obtain the stated reverse drift and diffusion matrix.
Depends on
Used by
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Sources
- B. D. O. Anderson, Reverse-time diffusion equation models, Section 5 (standard reference, not scraped)
- Y. Tang and H. Zhao, Score-based diffusion models via stochastic differential equations: a technical tutorial, Section 2.2 (standard reference, not scraped)