Heat kernel bounds for a large class of Markov process with singular jump

preprint2020arXivOpen access

Abstract

Let Z=(Z1,…,Zd)Z=(Z^{1}, \ldots, Z^{d}) be the dd-dimensional Lévy processes where ZiZ^{i}'s are independent 11-dimensional Lévy processes with jump kernel Jϕ,1(u,w)=∣u−w∣−1ϕ(∣u−w∣)−1J^{ϕ, 1}(u,w) =|u-w|^{-1}ϕ(|u-w|)^{-1} for u,w∈Ru, w\in \mathbb R. Here ϕϕ is an increasing function with weak scaling condition of order α‾,α‾∈(0,2)\underline α, \overline α\in (0, 2). Let J(x,y)≍Jϕ(x,y)J(x,y) \asymp J^ϕ(x,y) be the symmetric measurable function where \begin{align*} J^ϕ(x,y):=\begin{cases} J^{ϕ, 1}(x^i, y^i)\qquad&\text{ if xi≠yix^i \ne y^i for some ii and xj=yjx^j = y^j for all j≠ij \ne i}\\ 0\qquad&\text{ if xi≠yix^i \ne y^i for more than one index ii.} \end{cases} \end{align*} Corresponding to the jump kernel JJ, we show the existence of non-isotropic Markov processes X:=(X1,…,Xd)X:=(X^{1}, \ldots, X^{d}) and obtain sharp two-sided heat kernel estimates for the transition density functions.

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