首页> 外文期刊>The Journal of integral equations and applications >BOUNDARY BEHAVIOR OF THE LAYER POTENTIALS FOR THE TIME FRACTIONAL DIFFUSION EQUATION IN LIPSCHITZ DOMAINS
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BOUNDARY BEHAVIOR OF THE LAYER POTENTIALS FOR THE TIME FRACTIONAL DIFFUSION EQUATION IN LIPSCHITZ DOMAINS

机译:LIPSCHITZ域中时间分数阶扩散方程的层势的边界行为

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This paper investigates the boundary behavior of layer potentials for the time fractional diffusion equation ( TFDE) in Lipschitz domains. The paper is a continuation of [9]. Since now the boundary of the spatial domain Ω admits only Lipschitz smoothness, we have to replace the classical technique used in [9] with a more delicate harmonic analysis technique. We prove that certain nontangential maximal functions related to the layer potentials are bounded in L~p(Σ_T), which in particular implies the usual jump relations known for the heat equation. Although the results are well known in the case of the heat potential corresponding to the case a = 1, the proofs of the same properties seem not to be available in the case 0 < a < 1.
机译:本文研究了Lipschitz域中时间分数扩散方程(TFDE)的层势的边界行为。本文是[9]的延续。由于现在空间域Ω的边界仅允许Lipschitz平滑度,因此我们必须用更精细的谐波分析技术代替[9]中使用的经典技术。我们证明与层电势相关的某些非切线最大函数在L〜p(Σ_T)内有界,这特别意味着对于热方程而言,通常存在跳跃关系。尽管在与a等于1的情况对应的热势的情况下结果是众所周知的,但是在0 <1的情况下似乎无法获得相同性质的证明。

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