English

Perturbation by non-local operators

Probability 2016-09-30 v2 Analysis of PDEs

Abstract

Suppose that d1d\ge 1 and 0<β<α<20<\beta<\alpha<2. We establish the existence and uniqueness of the fundamental solution qb(t,x,y)q^b(t, x, y) to a class of (possibly nonsymmetric) non-local operators Lb=Δα/2+SbL^b=\Delta^{\alpha/2}+S^b, where Sbf(x):=A(d,β)Rd(f(x+z)f(x)f(x)z1{z1})b(x,z)zd+βdz S^bf(x):=A(d, -\beta) \int_{R^d} ( f(x+z)-f(x)- \nabla f(x) \cdot z 1_{\{|z|\leq 1\}} ) \frac{b(x, z)}{|z|^{d+\beta}}dz and b(x,z)b(x, z) is a bounded measurable function on Rd×RdR^d\times R^d with b(x,z)=b(x,z)b(x, z)=b(x, -z) for x,zRdx, z\in R^d. Here A(d,β)A(d, -\beta) is a normalizing constant so that Sb=Δβ/2S^b=\Delta^{\beta/2} when b(x,z)1b(x, z)\equiv 1. We show that if b(x,z)A(d,α)A(d,β)zβαb(x, z) \geq -\frac{{\cal A}(d, -\alpha)}{A(d, -\beta)}\, |z|^{\beta -\alpha}, then qb(t,x,y)q^b(t, x, y) is a strictly positive continuous function and it uniquely determines a conservative Feller process XbX^b, which has strong Feller property. The Feller process XbX^b is the unique solution to the martingale problem of (Lb,S(Rd))(L^b, {\cal S} (R^d)), where S(Rd){\cal S}(R^d) denotes the space of tempered functions on RdR^d. Furthermore, sharp two-sided estimates on qb(t,x,y)q^b(t, x, y) are derived. In stark contrast with the gradient perturbations, these estimates exhibit different behaviors for different types of b(x,z)b(x, z). The model considered in this paper contains the following as a special case. Let YY and ZZ be (rotationally) symmetric α\alpha-stable process and symmetric β\beta-stable processes on RdR^d, respectively, that are independent to each other. Solution to stochastic differential equations dXt=dYt+c(Xt)dZtdX_t=dY_t + c(X_{t-})dZ_t has infinitesimal generator LbL^b with b(x,z)=c(x)βb(x, z)=| c(x)|^\beta.

Cite

@article{arxiv.1312.7594,
  title  = {Perturbation by non-local operators},
  author = {Zhen-Qing Chen and Jie-Ming Wang},
  journal= {arXiv preprint arXiv:1312.7594},
  year   = {2016}
}
R2 v1 2026-06-22T02:36:35.349Z