Abstract:We consider the 3D Pauli operator with nonconstant magnetic field B of constant direction, perturbed by a symmetric matrix-valued electric potential V whose coefficients decay fast enough at infinity. We investigate the low-energy asymptotics of the corresponding spectral shift function. As a corollary, for generic negative V , we obtain a generalized Levinson formula, relating the low-energy asymptotics of the eigenvalue counting function and of the scattering phase of the perturbed operator.
“…The estimates of Proposition 6.10 are consistent with the ones of [27,Cor. 3.6], where the corresponding situation for magnetic Pauli operators is considered.…”
Section: In the First Lemma An Integrated Density Of States (Ids) Fosupporting
confidence: 78%
“…Our work is closely related to [27] where G. D. Raikov treats a similar issue in the case of magnetic Pauli operators. It can also be considered as a complement of [33], where general properties of the spectrum of Dirac operators with variable magnetic fields of constant direction and matrix perturbations are determined.…”
We consider a 3-dimensional Dirac operator H0 with non-constant magnetic field of constant direction, perturbed by a sign-definite matrix-valued potential V decaying fast enough at infinity. Then we determine asymptotics, as the energy goes to +m and −m, of the spectral shift function for the pair (H0 + V, H0). We obtain, as a by-product, a generalised version of Levinson's Theorem relating the eigenvalues asymptotics of H0 + V near +m and −m to the scattering phase shift for the pair (H0 + V, H0).
“…The estimates of Proposition 6.10 are consistent with the ones of [27,Cor. 3.6], where the corresponding situation for magnetic Pauli operators is considered.…”
Section: In the First Lemma An Integrated Density Of States (Ids) Fosupporting
confidence: 78%
“…Our work is closely related to [27] where G. D. Raikov treats a similar issue in the case of magnetic Pauli operators. It can also be considered as a complement of [33], where general properties of the spectrum of Dirac operators with variable magnetic fields of constant direction and matrix perturbations are determined.…”
We consider a 3-dimensional Dirac operator H0 with non-constant magnetic field of constant direction, perturbed by a sign-definite matrix-valued potential V decaying fast enough at infinity. Then we determine asymptotics, as the energy goes to +m and −m, of the spectral shift function for the pair (H0 + V, H0). We obtain, as a by-product, a generalised version of Levinson's Theorem relating the eigenvalues asymptotics of H0 + V near +m and −m to the scattering phase shift for the pair (H0 + V, H0).
“…and if there exists an integrated density of states for the operator P − 2 (see [29] definition (3.11)), then by [29, Lemma 3.3],…”
Section: Statement Of the Main Resultsmentioning
confidence: 99%
“…(i) The class of admissible magnetic fields described above is essentially the one introduced in [28,29]. We refer to these papers for more details and examples of admissible magnetic fields.…”
Abstract. In this work, we investigate the discrete spectrum generated by complex matrixvalued perturbations for a class of 2D and 3D Pauli operators with nonconstant magnetic fields. We establish a simple criterion for the potentials to produce discrete spectrum near the low ground energy of the operators. Moreover, in case of creation of nonreal eigenvalues, this criterion specifies also their location.
“…Beside the extensions already presented in Sections 6 and 8, others are appealing. For example, it would certainly be interesting to recast the generalized Levinson's theorem exhibited in [44,55] in our framework. Another challenging extension would be to find out the suitable algebraic framework for dealing with scattering systems described in a two-Hilbert spaces setting.…”
A topological version of Levinson's theorem is presented. Its proof relies on a C * -algebraic framework which is introduced in detail. Various scattering systems are considered in this framework, and more coherent explanations for the corrections due to thresholds effects or for the regularization procedure are provided. Potential scattering, point interactions, Friedrichs model and Aharonov-Bohm operators are part of the examples which are presented. Every concepts from scattering theory or from K-theory are introduced from scratch.
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