Tomas Ekholm
Royal Institute of Technology
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by Tomas Ekholm.
Archive for Rational Mechanics and Analysis | 2008
Tomas Ekholm; H Kovarik; D Krejcirik
We show that twisting of an infinite straight three-dimensional tube with non-circular cross-section gives rise to a Hardy-type inequality for the associated Dirichlet Laplacian. As an application we prove certain stability of the spectrum of the Dirichlet Laplacian in locally and mildly bent tubes. Namely, it is known that any local bending, no matter how small, generates eigenvalues below the essential spectrum of the Laplacian in the tubes with arbitrary cross-sections rotated along a reference curve in an appropriate way. In the present paper we show that for any other rotation some critical strength of the bending is needed in order to induce a non-empty discrete spectrum.
Communications in Partial Differential Equations | 2005
Tomas Ekholm; Hynek Kovařík
Abstract The spectrum of the Schrödinger operator in a quantum waveguide is known to be unstable in two and three dimensions. Any local enlargement of the waveguide produces eigenvalues beneath the continuous spectrum. Also, if the waveguide is bent, eigenvalues will arise below the continuous spectrum. In this paper a magnetic field is added into the system. The spectrum of the magnetic Schrödinger operator is proved to be stable under small local deformations and also under small bending of the waveguide. The proof includes a magnetic Hardy-type inequality in the waveguide, which is interesting in its own right. *Also on leave of absence from Nuclear Physics Institute, Academy of Sciences, Rez, near Prague, Czech Republic.
Annales Henri Poincaré | 2005
Denis Borisov; Tomas Ekholm; Hynek Kovařík
Abstract.We consider the magnetic Schrödinger operator in a two-dimensional strip. On the boundary of the strip the Dirichlet boundary condition is imposed except for a fixed segment (window), where it switches to magnetic Neumann {For the definition of magnetic Neumann boundary conditions see Section 2, Eq. (2.2)}. We deal with a smooth compactly supported field as well as with the Aharonov-Bohm field. We give an estimate on the maximal length of the window, for which the discrete spectrum of the considered operator will be empty. In the case of a compactly supported field we also give a sufficient condition for the presence of eigenvalues below the essential spectrum.
Advances in Mathematics | 2011
Tomas Ekholm; Rupert L. Frank; Hynek Kovařík
We consider Schrodinger operators on radial metric trees and prove Lieb–Thirring and Cwikel–Lieb–Rozenblum inequalities for their negative eigenvalues. The validity of these inequalities depends on the volume growth of the tree. We show that the bounds are valid in the endpoint case and reflect the correct order in the weak or strong coupling limit.
Journal of Mathematical Physics | 2014
Tomas Ekholm; Fabian Portmann
We study the quadratic form associated to the kinetic energy operator in the presence of an external magnetic field in d = 3. We show that if the radial component of the magnetic field does not vanish identically, then the classical lower bound given by Hardy is improved by a non-negative potential term depending on properties of the magnetic field.
Calculus of Variations and Partial Differential Equations | 2015
Tomas Ekholm; Rupert L. Frank; Hynek Kovařík
We consider the p-Laplacian in
Journal of Differential Equations | 2010
Tomas Ekholm; Andreas Enblom; Hynek Kovarik
Companion to the first International Conference on the Art, Science and Engineering of Programming on | 2017
Lucas Wiener; Tomas Ekholm; Philipp Haller
\mathbb {R}^d
Communications in Mathematical Physics | 2006
Tomas Ekholm; Rupert L. Frank
Nonlinear Analysis-theory Methods & Applications | 2015
Tomas Ekholm; Hynek Kovarik; Ari Laptev
Rd perturbed by a weakly coupled potential. We calculate the asymptotic expansions of the lowest eigenvalue of such an operator in the weak coupling limit separately for