The kinetic Schauder estimate for velocity Hessians

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Let Qr=(−r2,0]×Br3×Br⊂R×Rd×RdQ_r=(-r^2,0]\times B_{r^3}\times B_r\subset\mathbb{R}\times\mathbb{R}^d\times\mathbb{R}^d. For a bounded function hh on QQ, define

[h]Cvα(Q):=sup⁡(t,x,v),(t,x,v′)∈Q0<∣v−v′∣<1/2∣h(t,x,v)−h(t,x,v′)∣∣v−v′∣α[h]_{C_v^\alpha(Q)}:=\sup_{\substack{(t,x,v),(t,x,v')\in Q\\0<|v-v'|<1/2}}\frac{|h(t,x,v)-h(t,x,v')|}{|v-v'|^\alpha}

and analogously define [h]Cxβ(Q)[h]_{C_x^\beta(Q)} using spatial differences. For matrix-valued functions, let ∣M∣|M| denote the Frobenius norm. Let α∈(0,1)\alpha\in(0,1) and Λ>1\Lambda>1. There is a constant C=C(d,α,Λ)C=C(d,\alpha,\Lambda) such that every smooth solution ff of the kinetic Fokker–Planck equation in Q1Q_1 satisfying

Λ−1Id⁡≤a≤ΛId⁡,∣c∣≤Λ,∣g∣≤Λ,\Lambda^{-1}\operatorname{Id}\le a\le\Lambda\operatorname{Id},\qquad |c|\le\Lambda,\qquad |g|\le\Lambda,

and with f,Dv2f,a,c,g∈Cvα(Q1)f,D_v^2f,a,c,g\in C_v^\alpha(Q_1) obeys

[Dv2f]Cvα(Q1/2)≤C(1+[c]Cvα(Q1)+[a]Cvα(Q1)1+2/α)∥f∥L∞(Q1)+C(1+[a]Cvα(Q1))[g]Cvα(Q1).[D_v^2f]_{C_v^\alpha(Q_{1/2})}\le C\Bigl(1+[c]_{C_v^\alpha(Q_1)}+[a]_{C_v^\alpha(Q_1)}^{1+2/\alpha}\Bigr)\|f\|_{L^\infty(Q_1)}+C\Bigl(1+[a]_{C_v^\alpha(Q_1)}\Bigr)[g]_{C_v^\alpha(Q_1)}.

The kinetic Schauder estimate. The displayed estimate asserts a uniform interior Hölder bound for the velocity Hessian of smooth solutions in terms of the solution, the coefficient Hölder seminorms, and the source-term Hölder seminorm. The paper states that this conjecture is false, so the proposed estimate is refuted.

References

Primary source

Hongjie Dong and Weinan Wang, “Several counterexamples to kinetic Schauder estimates”, arXiv:2607.20682 (2026).

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