Averaging Dynamics Driven by Fractional Brownian Motion: Young Solutions of dxⁿ = fₙ(t, xⁿ)dB Converge in Probability in C^α to the Solution of dx = f̄(x)dB When |fₙ − f̄|_{−κ,γ} → 0Research Paper
Why oscillating coefficients matter
An equation driven by fractional Brownian motion can respond to a rapidly varying coefficient even when that coefficient has no useful pointwise limit. Hairer and Li study this issue for fractional Brownian motion with Hurst index above one half. Their Section 3 isolates a deterministic averaging statement: if the time antiderivatives of the coefficients approach those of a limiting coefficient in a suitable negative Hölder norm, the solutions approach the limiting solution in probability. This statement supplies a common target for averaging models whose fast variables have very different origins. The authors use it later with mixing fast processes, and also present a quasi-periodic example. The result and its role in the paper are stated in Hairer and Li, Section 3.
The problem sits at the boundary of two familiar views of differential equations. A pathwise Young equation is defined from individual sufficiently regular paths, whereas the available estimates for the oscillating coefficient and the fractional Brownian driver involve probability and conditional expectation. The mission records the precise point where these descriptions meet. It treats the published article, rather than a preprint, and targets its Theorem 3.13.
Driver, coefficients, and solutions
An -dimensional fractional Brownian motion with index is a centered Gaussian process with independent coordinates and covariance
The paper works with a two-sided process and . It uses a version whose sample paths are locally -Hölder for every . The mission names that version condition separately, because the covariance law alone does not select particular sample paths. The relevant past sigma algebra at time is generated by increments with . These conventions come from pp. 1826 and 1831–1832 of the article.
For a path on , write for its homogeneous Hölder seminorm and for its supremum norm. The norm on is . A Young integral is the limit of left-point sums over partitions of as the largest cell shrinks to zero. A Young solution from is an -Hölder path satisfying its integral equation at every time, with value at time zero. Here means bounded, twice continuously differentiable maps with bounded derivatives through order two; means -Hölder in time with values in . These are the paper's conventions on pp. 1829 and 1835–1838.
The negative Hölder bound means that the time antiderivative of has increments bounded by , and that the difference of those increments at spatial points is bounded by . Both bounds apply on the time window in question when . This is equation (3.12) in the article. It measures cancellation over time; it does not require itself to be small.
Formalization targets
The goal is the part of Theorem 3.13. Let be , let the limiting be autonomous and in , and suppose . The exponents satisfy , , , and . For Young solutions with the same starting point,
the target is
The milestone list follows the statements used around this target: the Hölder composition estimate of Lemma 2.1, the RKHS estimate of Lemma 3.3, the fractional Brownian integral estimate of Lemma 3.4, the stochastic sewing lemma of Lemma 3.5, the Young case of (3.18) from Lemmas 3.10 and 3.12, the Kolmogorov inclusions (3.24), and the deterministic stability estimate of Lemma 2.2. Each is a separate formal theorem. The authors' proofs follow their statements in Sections 2 and 3 and the Appendix; Lemma 3.5 is quoted from Lê, Theorem 2.1 without proof in the article.
What the result provides
The target gives convergence of entire solution paths in a Hölder topology, in probability. In the paper, this lets a model-specific estimate of the negative Hölder distance be used to conclude convergence of the corresponding dynamical system. Theorem A is obtained by adding such an estimate for a stationary mixing fast process; the deterministic statement here isolates the part independent of that model. These uses are described in Sections 1 and 3.
The published paper proves the result. This mission asks for machine-checked proofs of the stated Lean theorems. Its reusable work would include a pathwise Young integral over arbitrary partitions, Hölder norms that retain the value , a two-sided vector fractional Brownian motion interface, and stochastic estimates for time-dependent integrands. The goal and milestones in this proposal are statements with proof placeholders; the local build checks their types, not their proofs.
Main obstruction
Pointwise control of is unavailable: a rapidly oscillating function can be large at most times and still have small time antiderivatives. Applying a pathwise Young stability estimate directly to therefore leaves a coefficient norm that need not tend to zero. The integral estimate must connect cancellation measured by with bounds on the driven equation. The dependence on the past of the fractional Brownian motion makes this step more delicate than an estimate for a deterministic integrand. The required estimates and their domains appear in Lemmas 3.4–3.12.
Formalization scope
Time is for the two-sided driver; coefficient and solution assertions use with . State spaces are finite-dimensional real Euclidean spaces. The goal takes from the standing setting of Section 3.1, and it assumes the locally Hölder version of described on p. 1826. The solutions are required almost surely to satisfy the Young equation from the same . This requirement fixes the processes to the equations; the convergence claim cannot be obtained by choosing arbitrary paths. Probability of the norm event uses the measure of that set, and the conclusion is convergence in probability in the full norm.
The Lean definitions use for path and process seminorms, so unbounded suprema are not replaced by a default real value. The negative Hölder hypothesis uses real bounds instead of an infimum that could be meaningless on an empty class. The Young integral quantifies over every monotone partition and the mesh limit of its left-point sums. The fBm definition includes Gaussianity, means, and every cross-coordinate covariance; its path version is explicit. Interval integrals in the coefficient bound are applied to time-continuous coefficients in the goal. Lemmas 3.4 and 3.10 use the increment filtration, the case needed for this theorem.
The paper's Lemma 2.2 needs a common initial value for its homogeneous-seminorm estimate; the formal statement includes it and records the printed issue. The paper writes the limiting coefficient with a time argument but uses an autonomous coefficient in (3.23), which the goal adopts. This proposal covers the equation. The final extension in Theorem 3.13 and the conditional-expectation estimate (3.19) remain outside its current items. Contributions that close these gaps, or supply a general conditional Wiener integral matching the article's notation, would extend the development.