Inverse problems for the fractional-Laplacian with lower order non-local perturbations

2021 ◽  
Vol 374 (5) ◽  
pp. 3053-3075
Author(s):  
S. Bhattacharyya ◽  
T. Ghosh ◽  
G. Uhlmann
Author(s):  
Humberto Prado ◽  
Margarita Rivero ◽  
Juan J. Trujillo ◽  
M. Pilar Velasco

AbstractThe non local fractional Laplacian plays a relevant role when modeling the dynamics of many processes through complex media. From 1933 to 1949, within the framework of potential theory, the Hungarian mathematician Marcel Riesz discovered the well known Riesz potential operators, a generalization of the Riemann-Liouville fractional integral to dimension higher than one. The scope of this note is to highlight that in the above mentioned works, Riesz also gave the necessary tools to introduce several new definitions of the generalized coupled fractional Laplacian which can be applied to much wider domains of functions than those given in the literature, which are based in both the theory of fractional power of operators or in certain hyper-singular integrals. Moreover, we will introduce the corresponding fractional hyperbolic differential operator also called fractional Lorentzian Laplacian.


2011 ◽  
Vol 5 (2) ◽  
pp. 511-530 ◽  
Author(s):  
Gabriel Peyré ◽  
◽  
Sébastien Bougleux ◽  
Laurent Cohen ◽  

2016 ◽  
Vol 16 (1) ◽  
pp. 115-124 ◽  
Author(s):  
Francesco Petitta

AbstractWe deal with existence, uniqueness and regularity for solutions of the boundary value problem$\left\{\begin{aligned} \displaystyle\mathcal{L}^{s}u&\displaystyle=\mu&&% \displaystyle\text{in }\Omega,\\ \displaystyle u(x)&\displaystyle=0&&\displaystyle\text{on }\mathbb{R}^{n}% \backslash\Omega,\end{aligned}\right.$where Ω is a bounded domain of ${\mathbb{R}^{n}}$, μ is a bounded Radon measure on Ω, and ${\mathcal{L}^{s}}$ is a non-local operator of fractional order s whose kernel K is comparable with the one of the fractional Laplacian.


Author(s):  
Raffaella Servadei ◽  
Enrico Valdinoci

In this paper we deal with two non-local operators that are both well known and widely studied in the literature in connection with elliptic problems of fractional type. More precisely, for a fixed s ∈ (0,1) we consider the integral definition of the fractional Laplacian given bywhere c(n, s) is a positive normalizing constant, and another fractional operator obtained via a spectral definition, that is,where ei, λi are the eigenfunctions and the eigenvalues of the Laplace operator −Δ in Ω with homogeneous Dirichlet boundary data, while ai represents the projection of u on the direction ei.The aim of this paper is to compare these two operators, with particular reference to their spectrum, in order to emphasize their differences.


Sign in / Sign up

Export Citation Format

Share Document