On Spectral Properties of Restricted Fractional Laplacians with Self-adjoint Boundary Conditions on a Finite Interval
Jussi Behrndt, Markus Holzmann, Delio Mugnolo
TL;DR
This work develops a boundary-triplet framework for the restricted fractional Laplacian on a finite interval with $a\in(\tfrac{1}{2},1)$, parametrizing all self-adjoint realizations by 2-by-2 boundary data and establishing discrete, semibounded spectra. It delivers explicit $\gamma$-field and Weyl function formulas, including $\gamma^{(a)}(0)$ and $M^{(a)}(0)$, and uses Krein's formula to obtain resolvent expressions for general extensions, such as Friedrichs (Dirichlet), Krein--von Neumann, and Neumann-type realizations. A key finding is that, unlike the classical Laplacian, the Neumann-type extension for the fractional case has a simple negative eigenvalue, reflecting non-Markovian behavior. The analysis relies on Hörmander transmission spaces to define natural domains and to develop trace theory, illustrating how abstract extension theory yields precise spectral information for nonlocal operators on bounded domains and offering a framework for further spectral comparisons and estimates.
Abstract
We describe all self-adjoint realizations of the restricted fractional Laplacian $(-Δ)^a$ with power $a \in (\frac{1}{2}, 1)$ on a bounded interval by imposing boundary conditions on the functions in the domain of a maximal realization; such conditions relate suitable weighted Dirichlet and Neumann traces. This is done in a systematic way by using the abstract concept of boundary triplets and their Weyl functions from extension and spectral theory of symmetric and self-adjoint operators in Hilbert spaces. Our treatment follows closely the well-known one for classical Laplacians on intervals and it shows that all self-adjoint realizations have purely discrete spectrum and are semibounded from below. To demonstrate the method, we focus on three self-adjoint realizations of the restricted fractional Laplacian: the Friedrichs extension, corresponding to Dirichlet-type boundary conditions, the Krein--von Neumann extension, and a Neumann-type realization. Notably, the Neumann-type realization exhibits a simple negative eigenvalue, thus it is not larger than the Krein--von Neumann extension.
