64 research outputs found

    Singular continuous spectrum of half-line Schr\"odinger operators with point interactions on a sparse set

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    We say that a discrete set X =\{x_n\}_{n\in\dN_0} on the half-line 0=x0<x1<x2<x3<...<xn<...<+∞0=x_0 < x_1 <x_2 <x_3<... <x_n<... <+\infty is sparse if the distances Ξ”xn=xn+1βˆ’xn\Delta x_n = x_{n+1} -x_n between neighbouring points satisfy the condition Ξ”xnΞ”xnβˆ’1β†’+∞\frac{\Delta x_{n}}{\Delta x_{n-1}} \rightarrow +\infty. In this paper half-line Schr\"odinger operators with point Ξ΄\delta- and Ξ΄β€²\delta^\prime-interactions on a sparse set are considered. Assuming that strengths of point interactions tend to ∞\infty we give simple sufficient conditions for such Schr\"odinger operators to have non-empty singular continuous spectrum and to have purely singular continuous spectrum, which coincides with \dR_+.Comment: 14 pages, submitte

    Asymptotics of resonances induced by point interactions

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    We consider the resonances of the self-adjoint three-dimensional Schr\"odinger operator with point interactions of constant strength supported on the set X={xn}n=1NX = \{ x_n \}_{n=1}^N. The size of XX is defined by VX=maxβ‘Ο€βˆˆΞ Nβˆ‘n=1N∣xnβˆ’xΟ€(n)∣V_X = \max_{\pi\in\Pi_N} \sum_{n=1}^N |x_n - x_{\pi(n)}|, where Ξ N\Pi_N is the family of all the permutations of the set {1,2,…,N}\{1,2,\dots,N\}. We prove that the number of resonances counted with multiplicities and lying inside the disc of radius RR behaves asymptotically linear WXΟ€R+O(1)\frac{W_X}{\pi} R + \mathcal{O}(1) as Rβ†’βˆžR \to \infty, where the constant WX∈[0,VX]W_X \in [0,V_X] can be seen as the effective size of XX. Moreover, we show that there exist configurations of any number of points such that WX=VXW_X = V_X. Finally, we construct an example for N=4N = 4 with WX<VXW_X < V_X, which can be viewed as an analogue of a quantum graph with non-Weyl asymptotics of resonances.Comment: 14 pages, 1 figure, submission to the proceedings of the 8th Workshop on Quantum Chaos and Localisation Phenomena, Warsaw, May 201
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