2001
DOI: 10.1063/1.1415432
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Möbius structure of the spectral space of Schrödinger operators with point interaction

Abstract: Abstract. The Schrödinger operator with point interaction in one dimension has a U (2) family of self-adjoint extensions. We study the spectrum of the operator and show that (i) the spectrum is uniquely determined by the eigenvalues of the matrix U ∈ U (2) that characterizes the extension, and that (ii) the space of distinct spectra is given by the orbifold T 2 /Z Z 2 which is a Möbius strip with boundary.We employ a parametrization of U (2) that admits a direct physical interpretation and furnishes a coherent… Show more

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Cited by 45 publications
(68 citation statements)
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“…which provides a physical length scale to the system [10]. The condition (2.16) can then be solved by…”
Section: Supersymmetry On a Line With Point Singularitymentioning
confidence: 99%
“…which provides a physical length scale to the system [10]. The condition (2.16) can then be solved by…”
Section: Supersymmetry On a Line With Point Singularitymentioning
confidence: 99%
“…On the theoretical side, they have been found to exhibit a number of intriguing features, many of which have been seen before only in connection with quantum field theories. Examples include renormalization [1,2,3,4,5], Landau poles [6], anomalous symmetry breaking [5], duality [7,8,9], supersymmetry [9] and spectral anholonomy [9,10,11]. On the experimental side, the rapid developments of nanotechnology forecast that nano-scale quantum devices can be designed and manufactured into desired specifications.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, the levels of the mirror-S 3 singlets depend on neither of the parameters ξ and ζ and hence are independent on the choice of V in U = V σ 3 V −1 . In fact, these are a consequence of the spectral preserving SU(2) (or its subgroup U(1)) transformations [29] which are found in the family of inequivalent quantizations we are considering here.…”
Section: Spectral Preserving Su (2) and The Angular Spectrummentioning
confidence: 99%
“…It can be shown [29] that by choosing c i appropriately one finds σ such that σ U σ = V −1 UV for any V ∈ SU(2). In other words, the transformation generated by Q in (5.12) yields the change 14) without altering the spectrum.…”
Section: Spectral Preserving Su (2) and The Angular Spectrummentioning
confidence: 99%