2010
DOI: 10.1016/j.jde.2010.02.011
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1-D Schrödinger operators with local point interactions on a discrete set

Abstract: MSC: 34L05 34L40 47E05 47B25 47B36 81Q10 Keywords: Schrödinger operator Local point interaction Self-adjointness Lower semiboundedness Discreteness Spectral properties of 1-D Schrödinger operators H X,αOur paper is devoted to the case d * = 0. We consider H X,α in the framework of extension theory of symmetric operators by applying the technique of boundary triplets and the corresponding Weyl functions. We show that the spectral properties of H X,α like self-adjointness, discreteness, and lower semiboundedness… Show more

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Cited by 121 publications
(250 citation statements)
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References 49 publications
(143 reference statements)
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“…This result was proved in [5] and can also be established by a method in [10], where a similar condition was obtained for a usual (continuous) potential.…”
Section: Introductionsupporting
confidence: 60%
See 1 more Smart Citation
“…This result was proved in [5] and can also be established by a method in [10], where a similar condition was obtained for a usual (continuous) potential.…”
Section: Introductionsupporting
confidence: 60%
“…First, we consider the case of α k < 0. Under certain conditions, the spectrum of A proves to be discrete (see [5]). We give asymptotic estimates of the spectrum.…”
Section: Introductionmentioning
confidence: 99%
“…The operator H X, α is known as the Hamiltonian with δ interactions of strengths α n at the centers x n [2]. The analogs of Lemma 1 and Theorem 3 hold true for the operator H X, α (see [11,Sect. 5]) and the role of the matrix (15) is played by the Jacobi matrix…”
Section: Corollarymentioning
confidence: 96%
“…By (16) and (26), the structure of matrices (15) and (25) are completely different in the case d * = 0. There fore, the spectral properties of Hamiltonians with δ' and δ interactions on X are essentially different in this case (see [11]). …”
Section: Corollarymentioning
confidence: 99%
“…We shall denote them generically by L. In the one-dimensional case they form a four-parameter family of operators, each of which is characterized by two boundary conditions at x = 0. These objects yield exactly solvable models [2,4,5,6,8,11,12,26,38,45] and have been widely used in applications in quantum mechanics (e.g. in models of low-energy scattering [3,13,14,35] and quantum systems with boundaries [22,23,24,27,32]), condensed matter physics [10,17,25] and, more recently, on the approximation of thin quantum waveguides by quantum graphs [1,15,16,20].…”
mentioning
confidence: 99%