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CONTROLLABILITY OF THE HEAT EQUATION WITH AN INVERSE-SQUARE POTENTIAL LOCALIZED ON THE BOUNDARY?

机译:逆方势位于边界上的热方程的可控性?

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This article is devoted to analyzing control properties for the heat equation with singular potential -μ/|x|~2 arising at the boundary of a smooth domain Ω ? R~N, N ≥ 1. This problem was first studied by Vancostenoble and Zuazua [J. Funct. Anal., 254 (2008), pp. 1864-1902] and then generalized by Ervedoza [Comm. Partial Differential Equations, 33 (2008), pp. 1996-2019] in the context of interior singularity. Roughly speaking, these results showed that for any value of parameters μ ≤ μ(N):= (N - 2)~2/4, the corresponding parabolic system can be controlled to zero with the control distributed in any open subset of the domain. The critical value μ(N) stands for the best constant in the Hardy inequality with interior singularity. When considering the case of boundary singularity a better critical Hardy constant is obtained, namely, μN:= N~2/4. In this article we extend the previous results of Vancostenoble and Zuazua and of Ervedoza to the case of boundary singularity. More precisely, we show that for any μ ≤ μN, we can lead the system to zero state using a distributed control in any open subset. We emphasize that our results cannot be obtained straightforwardly from the previous works.
机译:本文致力于分析在光滑域Ω?的边界处出现奇异电位-μ/ | x |〜2的热方程的控制性质。 R〜N,N≥1。Vancostenoble和Zuazua首次研究了这个问题[J。功能Anal。,254(2008),pp。1864-1902],然后由Ervedoza [Comm。内在奇点的背景下,偏微分方程,33(2008),pp。1996-2019]。粗略地说,这些结果表明,对于任何参数μ≤μ(N):=(N-2)〜2/4的值,可以将相应的抛物线系统控制为零,并且控制分布在域的任何开放子集中。临界值μ(N)代表具有内部奇异性的Hardy不等式中的最佳常数。当考虑边界奇异性的情况时,可获得更好的临界Hardy常数,即,μN:= N〜2/4。在本文中,我们将Vancostenoble和Zuazua以及Ervedoza的先前结果扩展到边界奇异的情况。更确切地说,我们表明对于任何μ≤μN,我们都可以使用任何开放子集中的分布式控件将系统引导至零状态。我们强调,我们的结果不能直接从以前的作品中获得。

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