Heat kernels and analyticity of non-symmetric jump diffusion semigroups (1306.5015v2)

Abstract: Let $d\geq 1$ and $\alpha \in (0, 2)$. Consider the following non-local and non-symmetric L\'evy-type operator on $\mR^d$: $$ \sL^\kappa_{\alpha}f(x):=\mbox{p.v.}\int_{\mR^d}(f(x+z)-f(x))\frac{\kappa(x,z)}{|z|^{d+\alpha}} \dif z, $$ where $0<\kappa_0\leq \kappa(x,z)\leq \kappa_1$, $\kappa(x,z)=\kappa(x,-z)$, and $|\kappa(x,z)-\kappa(y,z)|\leq\kappa_2|x-y|^\beta$ for some $\beta\in(0,1)$. Using Levi's method, we construct the fundamental solution (also called heat kernel) $p^\kappa_\alpha (t, x, y)$ of $\sL^\kappa_\alpha $, and establish its sharp two-sided estimates as well as its fractional derivative and gradient estimates of the heat kernel. We also show that $p^\kappa_\alpha (t, x, y)$ is jointly H\"older continuous in $(t, x)$. The lower bound heat kernel estimate is obtained by using a probabilistic argument. The fundamental solution of $\sL^\kappa_{\alpha}$ gives rise a Feller process ${X, \mP_x, x\in \mR^d}$ on $\mR^d$. We determine the L\'evy system of $X$ and show that $\mP_x$ solves the martingale problem for $(\sL^\kappa_{\alpha}, C^2_b(\mR^d))$. Furthermore, we obtain the analyticity of the non-symmetric semigroup associated with $\sL^\kappa_\alpha $ in $L^p$-spaces for every $p\in[1,\infty)$. A maximum principle for solutions of the parabolic equation $\partial_t u =\sL^\kappa_\alpha u$ is also established.