Abstract

We investigate the self-adjointness of the two-dimensional Dirac operator $D$, with $quantum$-$dot$ and $Lorentz$-$scalar$ $\\delta$-$shell$ boundary conditions, on piecewise $C^2$ domains (with finitely many corners). For both models, we prove the existence of a unique self-adjoint realization whose domain is included in the Sobolev space $H^{1/2}$, the formal form domain of the free Dirac operator. The main part of our paper consists of a description of the domain of the adjoint operator $D^\*$ in terms of the domain of $D$ and the set of harmonic functions that verify some $mixed$ boundary conditions. Then, we give a detailed study of the problem on an infinite sector, where explicit computations can be made: we find the self-adjoint extensions for this case. The result is then translated to general domains by a coordinate transformation.

Highlights

  • In this paper we study the self-adjoint realizations of the two-dimensional Dirac operator with boundary conditions on corner domains

  • The free massless Dirac operator in R2 is given by the differential expression

  • Dirac operator describes the evolution of a relativistic particle with spin

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Summary

Introduction

In this paper we study the self-adjoint realizations of the two-dimensional Dirac operator with boundary conditions on corner domains. Quantum-dot, Lorentz-scalar δ-shell, boundary conditions, self-adjoint operator, conformal map, corner domains. In Theorem 1.6, we characterize the domain of the adjoint operator in terms of the operator defined on H1 plus the set of C2-valued harmonic functions that verify some mixed boundary condition, see Theorem 1.6 for more details. This fact holds independently of details about the domain and may generalize to other or the three-dimensional case. By the result for smooth domains (see [20]), it is in H1

Separation of variables in the wedge
Curvilinear polygons
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