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Semi-local behaviour of non-local hypoelliptic equations: divergence form

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arxiv 2404.05612 v4 pith:XXQPROV2 submitted 2024-04-08 math.AP

classification math.AP
keywords equationsharnackhypoellipticinequalitynon-localstrongboundbounds
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abstract

We derive the Strong Harnack inequality for a class of hypoelliptic integro-differential equations in divergence form. Our result is semi-local, in the sense that we require the equation to hold globally in velocity. In fact, it is known that the Strong Harnack inequality fails in the kinetic case if the equation is merely satisfied in a bounded velocity domain [arXiv:2405.05223]. This is in stark contrast to the case of parabolic equations, for which a local Strong Harnack inequality holds. In a first step, we derive a local bound on the non-local tail on upper level sets by exploiting the coercivity of the cross terms. In a second step, we perform a De Giorgi argument in $L^1$, since we control the tail term only in $L^1$. This yields a linear $L^1$ to $L^\infty$ bound. Consequently, we prove polynomial upper bounds for $s\in(0,1)$ and exponential lower bounds for $s\in(\frac12,1)$ on the fundamental solution by adapting Aronson's method to non-local hypoelliptic equations.

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  1. Pointwise upper bound for the fundamental solution of fractional Fokker-Planck equation

    math.AP 2025-01 reject novelty 3.0 of 10

    A Littlewood-Paley proof is given for a pointwise upper bound on the fundamental solution of the 1D fractional Fokker-Planck equation, with polynomial decay exponent 2+2s and an arbitrarily small epsilon.

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