Title: Calderón–Zygmund theory for strongly coupled linear system of nonlocal equations with Hölder-regular coefficient
Abstract We extend the Calderón–Zygmund theory for nonlocal equations tostrongly coupled system of linear nonlocal equations ℒAs⁢u =f {\mathcal{L}^{s}_{A}u=f}, where the operator ℒAs {\mathcal{L}^{s}_{A}}is formally given by ℒAs⁢u = ∫ℝn A⁢(x,y) |x-y| n+2⁢s ⁢ (x-y) ⊗ (x-y) |x-y| 2 ⁢ ( u⁢(x) - u⁢(y) ) ⁢𝑑y . \mathcal{L}^{s}_{A}u=\int_{\mathbb{R}^{n}}\frac{A(x,y)}{|x-y|^{n+2s}}\frac{(x-%y)\otimes(x-y)}{|x-y|^{2}}(u(x)-u(y))\,dy. For 0<s<1 {0and A: ℝn×ℝn→ℝ {A:\mathbb{R}^{n}\times\mathbb{R}^{n}\to\mathbb{R}}taken to be symmetric and serving asa variable coefficient for the operator, the system under consideration is the fractional version of the classical Navier–Lamé linearized elasticity system. The study of the coupled system of nonlocal equations is motivated by its appearance in nonlocal mechanics, primarily in peridynamics. Our regularity result states that if A⁢(⋅,y) {A(\,\cdot\,,y)}is uniformly Holder continuous and infx∈ℝn ⁡ A⁢(x,x) >0 {\inf_{x\in\mathbb{R}^{n}}A(x,x)>0}, then for f∈Llocp {f\in L^{p}_{\rm loc}}, for p≥2 {p\geq 2}, the solution vector u∈ Hloc 2⁢s-δ ,p {u\in H^{2s-\delta,p}_{\rm loc}}for some δ∈(0,s) {\delta\in(0,s)}.  more » « less
Award ID(s):
2044898 2206252
PAR ID:
10591513
Author(s) / Creator(s):
; ; ;
Publisher / Repository:
DeGruyter
Date Published:
Journal Name:
Advances in Calculus of Variations
Volume:
18
Issue:
2
ISSN:
1864-8258
Page Range / eLocation ID:
421 to 438
Format(s):
Medium: X
Sponsoring Org:
National Science Foundation
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