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Maximum principles for Laplacian and fractional Laplacian with critical integrability

Abstract

In this paper, we study maximum principles for Laplacian and fractional Laplacian with critical integrability. We first consider Δu(x)+c(x)u(x)0-\Delta u(x)+c(x)u(x)\geq 0 in B1B_1 where c(x)Lp(B1)c(x)\in L^{p}(B_1), B1RnB_1\subset \mathbf{R}^n. As is known that p=n2p=\frac{n}{2} is the critical case. We show that the maximum principle holds for pn2p\geq \frac{n}{2}. On the other hand, the strong maximum principle requires p>n2p>\frac{n}{2}. In fact, we give a counterexample to illustrate that no matter how small cLp(B1)\|c\|_{L^{p}(B_1)} is, the strong maximum principle is false as p=n2p=\frac{n}{2}. Next, we investigate Δu(x)+b(x)u(x)0-\Delta u(x)+\vec{b}(x)\cdot \nabla u(x)\geq 0 in B1B_1 where b(x)Lp(B1)\vec{b}(x)\in L^p(B_1). Here p=np=n is the critical case. In contrast to the previous case, the maximum principle and strong maximum principle both hold for pnp\geq n. We also extend some of the results above to fractional Laplacian. The non-locality of the fractional Laplacian brings in some new difficulties. Some new methods are needed

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