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hal.structure.identifierUniversité de Bordeaux [UB]
hal.structure.identifierInstitut de Mathématiques de Bordeaux [IMB]
hal.structure.identifierDepartamento de Matemáticas [Bilbao]
dc.contributor.authorBENHELLAL, Badreddine
dc.date.accessioned2024-04-04T02:47:09Z
dc.date.available2024-04-04T02:47:09Z
dc.identifier.urihttps://oskar-bordeaux.fr/handle/20.500.12278/191618
dc.description.abstractEnLet $\O\subset\mathbb{R}^3$ be an open set, we study the spectral properties of the free Dirac operator $ \mathcal{H} :=- i \alpha \cdot\nabla + m\beta$ coupled with the singular potential $V_\kappa=(\epsilon \mathit{I}_4 +\mu\beta + \eta(\alpha\cdot \mathit{N}))\delta_{\partial\Omega}$ , where $\kappa=(\epsilon,\mu,\eta)\in\mathbb{R}^3$. In the first instance, $\O$ can be either a $\mathcal{C}^2$-bounded domain or a locally deformed half-space. In both cases, the self-adjointness is proved and several spectral properties are given. In particular, we extend the result of \cite{BHOP} to the case of a locally deformed half-space, by giving a complete description of the essential spectrum of $ \mathcal{H}+V_\k $, for the so-called critical combinations of coupling constants. In the second part of the paper, the case of bounded rough domains is investigated. Namely, in the non-critical case and under the assumption that $\O$ has a $\mathrm{VMO}$ normal, we show that $ \mathcal{H}+V_\kappa $ is still self-adjoint and preserves almost all of its spectral properties. More generally, under certain assumptions about the sign or the size of the coupling constants, we are able to show the self-adjointness of the coupling $ \mathcal{H} + (\epsilon I_4 +\mu\beta )\delta_{\partial\Omega}$ , when $\Omega$ is bounded uniformly rectifiable. Moreover, if $\epsilon^2-\mu^2=-4$, we then show that $\partial\O$ is impenetrable. In particular, if $\Omega$ is Lipschitz, we then recover the same spectral properties as in the VMO case. In addition, we establish a characterization of regular Semmes-Kenig-Toro domains via the compactness of the anticommutator between $(\alpha\cdot \mathit{N})$ and the Cauchy operator associated to the free Dirac operator. Finally, we study the coupling $\mathcal{H}_{\upsilon}=\mathcal{H}+ i\u\beta(\alpha\cdot N)\delta_{\partial\Omega}$. In particular, if $\Omega$ is a bounded $\mathcal{C}^2$ domain, then we show that $\mathcal{H}_{ \pm2}$ is essentially self-adjoint and generates confinement.
dc.language.isoen
dc.subject.enFebruary 18
dc.subject.en2021. 2010 Mathematics Subject Classification. 81Q10
dc.subject.en81V05
dc.subject.en35P15
dc.subject.en58C40 Dirac operators
dc.subject.enself-adjoint extensions
dc.subject.enshell interactions
dc.subject.encritical interaction strength
dc.subject.enQuantum confinement
dc.subject.enSemmes-Kenig-Toro domains
dc.subject.enUniformly rectifiable domains
dc.title.enSPECTRAL PROPERTIES OF THE DIRAC OPERATOR COUPLED WITH δ-SHELL INTERACTIONS
dc.typeDocument de travail - Pré-publication
dc.subject.halMathématiques [math]/Théorie spectrale [math.SP]
bordeaux.hal.laboratoriesInstitut de Mathématiques de Bordeaux (IMB) - UMR 5251*
bordeaux.institutionUniversité de Bordeaux
bordeaux.institutionBordeaux INP
bordeaux.institutionCNRS
hal.identifierhal-03147409
hal.version1
hal.origin.linkhttps://hal.archives-ouvertes.fr//hal-03147409v1
bordeaux.COinSctx_ver=Z39.88-2004&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.au=BENHELLAL,%20Badreddine&rft.genre=preprint


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