分数相场系统的适定性、正则性及渐近分析

Asymptot. Anal. Pub Date : 2018-06-12 DOI:10.3233/ASY-191524
P. Colli, G. Gilardi
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引用次数: 11

摘要

本文研究了一类非守恒的Caginalp型相场系统,其中主算子为两个固定线性算子$A$和$B$的分数阶。对于有界光滑域$\Omega$,假设算子$A$和$B$在Hilbert空间$L^2(\Omega)$中是密集定义的、无界的、自伴随的、单调的,并且具有紧解。我们对算子的分数次幂的定义使用了谱理论的方法。在相方程中存在双井型非线性,我们的方法允许正则势或对数势以及包含指示函数的不可微势。我们给出了一般的适定性和正则性结果,扩展了已知的具有零Neumann条件或其他边界条件(如Dirichlet或Robin条件)的非分数阶椭圆算子的相应结果。然后,我们通过将$\omega$ -极限的每个元素完全表征为平稳解来研究系统的长期行为。在论文的最后一部分,我们研究了在相位方程中起作用的算子$B^{2\sigma}$中出现的参数$\sigma$逐渐趋于零时系统的渐近行为。我们可以证明在极限处的一个相松弛问题的收敛性,在这个问题中出现了一个附加项,其中包含了相变量在$B$核上的投影。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Well-posedness, regularity and asymptotic analyses for a fractional phase field system
This paper is concerned with a non-conserved phase field system of Caginalp type in which the main operators are fractional versions of two fixed linear operators $A$ and $B$. The operators $A$ and $B$ are supposed to be densely defined, unbounded, self-adjoint, monotone in the Hilbert space $L^2(\Omega)$, for some bounded and smooth domain $\Omega$, and have compact resolvents. Our definition of the fractional powers of operators uses the approach via spectral theory. A nonlinearity of double-well type occurs in the phase equation and either a regular or logarithmic potential, as well as a non-differentiable potential involving an indicator function, is admitted in our approach. We show general well-posedness and regularity results, extending the corresponding results that are known for the non-fractional elliptic operators with zero Neumann conditions or other boundary conditions like Dirichlet or Robin ones. Then, we investigate the longtime behavior of the system, by fully characterizing every element of the $\omega$-limit as a stationary solution. In the final part of the paper we study the asymptotic behavior of the system as the parameter $\sigma$ appearing in the operator $B^{2\sigma}$ that plays in the phase equation decreasingly tends to zero. We can prove convergence to a phase relaxation problem at the limit, in which an additional term containing the projection of the phase variable on the kernel of $B$ appears.
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