Abstract:Abstract. We consider the unperturbed operatorHere A is a magnetic potential which generates a constant magnetic field b > 0, and the edge potential W is a non-decreasing non-constant bounded function depending only on the first coordinate x 2 R of .x; y/ 2 R 2 . Then the spectrum of H 0 has a band structure and is absolutely continuous; moreover, the assumption lim x!1 .W .x/ W . x// < 2b implies the existence of infinitely many spectral gaps for H 0 . We consider the perturbed operators H˙D H 0˙V where the e… Show more
“…In that context the main asymptotic term is (ln | ln λ|) −1 | ln λ| which goes to infinity faster than the one presented here, | ln λ| 1/2 , implying that the accumulation of the eigenvalues is stronger in our case. Similar results to our was previously obtained in [3], [4], for other magnetic Hamiltonians with compact supported electric potentials (see Remark after Theorem 2.1).…”
Section: Introductionsupporting
confidence: 91%
“…Remark : Similar results to Theorem 2.1 appear in [3] and [4]. In [3] the discrete spectrum of operators of the form…”
Section: )supporting
confidence: 68%
“…Using the Ky-Fan inequalities (3.2) we get (3.22) (see Proposition 3.1 and Theorem 3.2 in [3] for a detailed proof of a similar result). Now we are ready to finish the proof of Theorem 2.1.…”
Section: It Is Satisfied the Asymptotic Formulamentioning
We consider the discrete spectrum of the two-dimensional Hamiltonian H = H0 + V , where H0 is a Schrödinger operator with a non-constant magnetic field B that depends only on one of the spatial variables, and V is an electric potential that decays at infinity. We study the accumulation rate of the eigenvalues of H in the gaps of its essential spectrum. First, under certain general conditions on B and V , we introduce effective Hamiltonians that govern the main asymptotic term of the eigenvalue counting function. Further, we use the effective Hamiltonians to find the asymptotic behavior of the eigenvalues in the case where the potential V is a power-like decaying function and in the case where it is a compactly supported function, showing a semiclassical behavior of the eigenvalues in the first case and a non-semiclassical behavior in the second one. We also provide a criterion for the finiteness of the number of eigenvalues in the gaps of the essential spectrum of H.
“…In that context the main asymptotic term is (ln | ln λ|) −1 | ln λ| which goes to infinity faster than the one presented here, | ln λ| 1/2 , implying that the accumulation of the eigenvalues is stronger in our case. Similar results to our was previously obtained in [3], [4], for other magnetic Hamiltonians with compact supported electric potentials (see Remark after Theorem 2.1).…”
Section: Introductionsupporting
confidence: 91%
“…Remark : Similar results to Theorem 2.1 appear in [3] and [4]. In [3] the discrete spectrum of operators of the form…”
Section: )supporting
confidence: 68%
“…Using the Ky-Fan inequalities (3.2) we get (3.22) (see Proposition 3.1 and Theorem 3.2 in [3] for a detailed proof of a similar result). Now we are ready to finish the proof of Theorem 2.1.…”
Section: It Is Satisfied the Asymptotic Formulamentioning
We consider the discrete spectrum of the two-dimensional Hamiltonian H = H0 + V , where H0 is a Schrödinger operator with a non-constant magnetic field B that depends only on one of the spatial variables, and V is an electric potential that decays at infinity. We study the accumulation rate of the eigenvalues of H in the gaps of its essential spectrum. First, under certain general conditions on B and V , we introduce effective Hamiltonians that govern the main asymptotic term of the eigenvalue counting function. Further, we use the effective Hamiltonians to find the asymptotic behavior of the eigenvalues in the case where the potential V is a power-like decaying function and in the case where it is a compactly supported function, showing a semiclassical behavior of the eigenvalues in the first case and a non-semiclassical behavior in the second one. We also provide a criterion for the finiteness of the number of eigenvalues in the gaps of the essential spectrum of H.
“…Since our extremal points are only the limits on the band functions, it is necessary to modify the analysis of previous works. The phenomenon of thresholds given by limits of the band functions is also present for some quantum Hall effect models (see [6]) and for some Iwatsuka models (see [26]). In these works, the SSF was studied only in the region where it counts the number of discrete eigenvalues.…”
We consider the Schrödinger operator with constant magnetic field defined on the halfplane with a Dirichlet boundary condition, H 0 , and a decaying electric perturbation V . We analyze the spectral density near the Landau levels, which are thresholds in the spectrum of H 0 , by studying the Spectral Shift Function (SSF) associated to the pair (H 0 + V, H 0 ). For perturbations of a fixed sign, we estimate the SSF in terms of the eigenvalue counting function for certain compact operators. If the decay of V is power-like, then using pseudodifferential analysis, we deduce that there are singularities at the thresholds and we obtain the corresponding asymptotic behavior of the SSF. Our technique gives also results for the Neumann boundary condition.
“…By applying the Mourre theory, they proved that a part of the absolutely continuous spectrum of P (b, ω) persists. On the other hand, we can consider the model (1.1) as the quantum hall system Hamiltonian with the unbounded edge potential W (x) = ω 2 x 2 (see [4,6,20]). In this work, we give a complete asymptotic expansion in powers of b −1 of the trace of the operators f (P (b, ω)) and f (P (b, ω))F and the stationary techniques developed by M. Dimassi [7] (see also M. Dimassi-J.…”
Abstract. In this paper we study the perturbed quadratic Hamiltonian in two-dimensional case,Here, b is the strong constant magnetic field, ω = 0 is a fixed constant, and the potential V vanishes at infinity. For f ∈ C ∞ 0 ((−∞, 0); R) and b large enough, we give a full asymptotic expansion in powers of b −1 of the trace of f (P (b, ω)). Moreover, we also obtain a Weyl formula with optimal remainder estimate of the counting function of eigenvalues of P (b, ω) as b → ∞.
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