Dynamical resonances and SSF singularities for a magnetic Schroedinger operator
BRIET, Philippe
Centre de Physique Théorique - UMR 6207 [CPT]
Centre de Physique Théorique - UMR 7332 [CPT]
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Centre de Physique Théorique - UMR 6207 [CPT]
Centre de Physique Théorique - UMR 7332 [CPT]
BRIET, Philippe
Centre de Physique Théorique - UMR 6207 [CPT]
Centre de Physique Théorique - UMR 7332 [CPT]
< Réduire
Centre de Physique Théorique - UMR 6207 [CPT]
Centre de Physique Théorique - UMR 7332 [CPT]
Langue
en
Article de revue
Ce document a été publié dans
Serdica Mathematical Journal. 2008, vol. 34, p. 179-218
Bulgarian Academy of Sciences, Institute of Mathematics
Résumé en anglais
We consider the Hamiltonian $H$ of a 3D spinless non-relativistic quantum particle subject to parallel constant magnetic and non-constant electric field. The operator $H$ has infinitely many eigenvalues of infinite ...Lire la suite >
We consider the Hamiltonian $H$ of a 3D spinless non-relativistic quantum particle subject to parallel constant magnetic and non-constant electric field. The operator $H$ has infinitely many eigenvalues of infinite multiplicity embedded in its continuous spectrum. We perturb $H$ by appropriate scalar potentials $V$ and investigate the transformation of these embedded eigenvalues into resonances. First, we assume that the electric potentials are dilation-analytic with respect to the variable along the magnetic field, and obtain an asymptotic expansion of the resonances as the coupling constant $\varkappa$ of the perturbation tends to zero. Further, under the assumption that the Fermi Golden Rule holds true, we deduce estimates for the time evolution of the resonance states with and without analyticity assumptions; in the second case we obtain these results as a corollary of suitable Mourre estimates and a recent article of Cattaneo, Graf and Hunziker \cite{cgh}. Next, we describe sets of perturbations $V$ for which the Fermi Golden Rule is valid at each embedded eigenvalue of $H$; these sets turn out to be dense in various suitable topologies. Finally, we assume that $V$ decays fast enough at infinity and is of definite sign, introduce the Krein spectral shift function for the operator pair $(H+V, H)$, and study its singularities at the energies which coincide with eigenvalues of infinite multiplicity of the unperturbed operator $H$.< Réduire
Mots clés en anglais
magnetic Schroedinger operators
resonances
Mourre estimates
spectral shift function
Project ANR
Equations hyperboliques dans des espaces-temps de la relativité générale : diffusion et résonances. - ANR-05-JCJC-0087
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