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This paper is related to the spectral stability of traveling wave solutions of partial
differential equations. In the first part of the paper we use the Gohberg-Rouche Theorem
to prove equality of the algebraic multiplicity of an isolated eigenvalue of an abstract
operator on a Hilbert space, and the algebraic multiplicity of the eigenvalue of the
corresponding Birman-Schwinger type operator pencil. In the second part of the paper we
apply this result...
We prove the existence of the density of states of a local, self-adjoint operator determined by a coercive, almost periodic quadratic form on . The support of the density coincides with the spectrum of the operator in .
We establish necessary and sufficient conditions on the real- or complex-valued potential
defined on for the relativistic Schrödinger operator to be bounded as an operator from the Sobolev space to its
dual .
We shall show that every differential operator of 2-nd order in a real separable Hilbert space can be decomposed into a regular and an irregular operator. Then we shall characterize irregular operators and differential operators satisfying the maximum principle. Results obtained for the Lévy laplacian in [3] will be generalized for irregular differential operators satisfying the maximum principle.
We solve, in two dimensions, the "square root problem of Kato". That is, for L ≡ -div (A(x)∇), where A(x) is a 2 x 2 accretive matrix of bounded measurable complex coefficients, we prove that L1/2: L12(R2) → L2(R2).[Proceedings of the 6th International Conference on Harmonic Analysis and Partial Differential Equations, El Escorial (Madrid), 2002].
We shall consider the Schrödinger operators on with the magnetic field given by a nonnegative constant field plus random magnetic fields of the Anderson type or of the Poisson-Anderson type. We shall investigate the spectrum of these operators by the method of the admissible potentials by Kirsch-Martinelli. Moreover, we shall prove the lower Landau levels are infinitely degenerated eigenvalues when the constant field is sufficiently large, by estimating the growth order of the eigenfunctions...
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