Mosco convergence of the diffusion large-deviation functional

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Let ρ\rho and ρˉ\bar\rho be probability measures on Rd\mathbb R^d, and let

P2S(Rd):={ρ∈P(Rd):∫∣x∣2 dρ<∞, S(ρ)<∞}.\mathcal P_2^{\mathcal S}(\mathbb R^d):=\left\{\rho\in\mathcal P(\mathbb R^d):\int |x|^2\,d\rho<\infty,\ \mathcal S(\rho)<\infty\right\}.

For a fixed time step h>0h>0, let JDfh(ρ∣ρˉ)\mathcal J^h_{\mathrm{Df}}(\rho\mid\bar\rho) be the diffusion large-deviation rate functional, let dd denote the Wasserstein distance, and define

KDfh(ρ∣ρˉ):=12S(ρ)−12S(ρˉ)+14hd2(ρˉ,ρ).\mathcal K^h_{\mathrm{Df}}(\rho\mid\bar\rho):=\tfrac12\mathcal S(\rho)-\tfrac12\mathcal S(\bar\rho)+\frac{1}{4h}d^2(\bar\rho,\rho).

Mosco-convergence conjecture. For every fixed ρˉ∈P2S(Rd)\bar\rho\in\mathcal P_2^{\mathcal S}(\mathbb R^d),

JDfh( ⋅∣ρˉ)−14hd2(ρˉ, ⋅ )→h→0M12S(⋅)−12S(ρˉ)=KDfh( ⋅∣ρˉ)−14hd2(ρˉ, ⋅ ).\mathcal J^h_{\mathrm{Df}}(\,\cdot\mid\bar\rho)-\frac{1}{4h}d^2(\bar\rho,\,\cdot\,)\xrightarrow[h\to0]{M}\tfrac12\mathcal S(\cdot)-\tfrac12\mathcal S(\bar\rho)=\mathcal K^h_{\mathrm{Df}}(\,\cdot\mid\bar\rho)-\frac{1}{4h}d^2(\bar\rho,\,\cdot\,).

The lower-bound part is with respect to the narrow topology on P2(Rd)\mathcal P_2(\mathbb R^d), while the recovery sequence uses the topology given by convergence in Wasserstein distance together with convergence of the entropy S\mathcal S. This identifies the large-deviation functional and the Wasserstein gradient-flow functional beyond their minimisers; the statement was first proved under additional restrictions when both measures are sufficiently close to uniform distributions on a bounded interval, while the general assertion is the conjectural formulation presented here.

References

Primary source

Mark Peletier, Michiel Renger and Marco Veneroni, “Variational formulation of the Fokker-Planck equation with decay: a particle approach”, arXiv:1108.3181 (2013).

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