Abstract
In this note we consider the self-adjoint Schrödinger operator in , , with a -potential supported on a Lipschitz hypersurface of strength . We show the uniqueness of the ground state and, under some additional conditions on the coefficient and the hypersurface , we determine the essential spectrum of . In the special case that is a hyperplane we obtain a Birman-Schwinger principle with a relativistic Schrödinger operator as Birman-Schwinger operator. As an application we prove an optimization result for the bottom of the spectrum of .
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