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    Accurate numerical methods for two and three dimensional integral fractional Laplacian with applications

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    In this paper, we propose accurate and efficient finite difference methods to discretize the two- and three-dimensional fractional Laplacian (−Δ)α2(-\Delta)^{\frac{\alpha}{2}} (0<α<20 < \alpha < 2) in hypersingular integral form. The proposed finite difference methods provide a fractional analogue of the central difference schemes to the fractional Laplacian, and as α→2−\alpha \to 2^-, they collapse to the central difference schemes of the classical Laplace operator −Δ-\Delta. We prove that our methods are consistent if u∈C⌊α⌋,α−⌊α⌋+ϵ(Rd)u \in C^{\lfloor\alpha\rfloor, \alpha-\lfloor\alpha\rfloor+\epsilon}({\mathbb R}^d), and the local truncation error is O(hϵ){\mathcal O}(h^\epsilon), with ϵ>0\epsilon > 0 a small constant and ⌊⋅⌋\lfloor \cdot \rfloor denoting the floor function. If u∈C2+⌊α⌋,α−⌊α⌋+ϵ(Rd)u \in C^{2+\lfloor\alpha\rfloor, \alpha-\lfloor\alpha\rfloor+\epsilon}({\mathbb R}^d), they can achieve the second order of accuracy for any α∈(0,2)\alpha \in (0, 2). These results hold for any dimension d≥1d \ge 1 and thus improve the existing error estimates for the finite difference method of the one-dimensional fractional Laplacian. Extensive numerical experiments are provided and confirm our analytical results. We then apply our method to solve the fractional Poisson problems and the fractional Allen-Cahn equations. Numerical simulations suggest that to achieve the second order of accuracy, the solution of the fractional Poisson problem should {\it at most} satisfy u∈C1,1(Rd)u \in C^{1,1}({\mathbb R}^d). One merit of our methods is that they yield a multilevel Toeplitz stiffness matrix, an appealing property for the development of fast algorithms via the fast Fourier transform (FFT). Our studies of the two- and three-dimensional fractional Allen-Cahn equations demonstrate the efficiency of our methods in solving the high-dimensional fractional problems.Comment: 24 pages, 6 figures, and 6 table
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