2021
DOI: 10.1007/s11005-021-01369-2
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Optimization of the lowest eigenvalue of a soft quantum ring

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Cited by 8 publications
(6 citation statements)
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“…While the two situations are of primary interest to us, they are particular cases of a more general channel profile. In the spirit of [EL21] one can consider the operator (e) H Γ,µ associated with the quadratic form…”
Section: Problem Settingmentioning
confidence: 99%
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“…While the two situations are of primary interest to us, they are particular cases of a more general channel profile. In the spirit of [EL21] one can consider the operator (e) H Γ,µ associated with the quadratic form…”
Section: Problem Settingmentioning
confidence: 99%
“…Recently an alternative, more realistic model of 'soft' waveguides attracted attention, see [Ex20] and further developments in [KKK21,EL21,EKL22,EV23], where the interaction term is a regular potential 'ditch' the axis of which is a fixed curve. In such a description the tunneling between different parts of the guide is not suppressed while its transverse width need not be zero.…”
Section: Introductionmentioning
confidence: 99%
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“…In the mentioned paper it was shown that two-dimensional soft waveguides share an important property with their more idealized counterparts, namely that a bend of the potential channel can give rise to bound states of such a Hamiltonian, although the existence condition derived in [Ex20] lacks the universality known in the said two models. Other recent results concern the existence of a discrete spectrum in the example of a 'bookcover' guide [KKK21] and a spectral optimization for ring-shaped soft guides [EL21]; related results can be also found in [EKP20,WT14].…”
Section: Introductionmentioning
confidence: 96%
“…The results obtained there concern mainly the existence of the discrete spectrum points below the threshold of the essential spectrum. For example, it has been proved in [12,14,23,25] that the local bending acts as an attractive potential inducing a new spectrum below the essential threshold. In [10], it has been shown that for a weak deformation the existence of the discrete spectrum points depends on the total area of deformation which is assumed to be positive if the deformation is localized on Σ \ Ω and negative if the deformation is situated on Ω \ Σ.…”
Section: Introductionmentioning
confidence: 99%