2004
DOI: 10.1103/physrevb.69.155317
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Electronic eigenstates in quantum rings: Asymptotics and numerics

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Cited by 42 publications
(38 citation statements)
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“…3, it becomes clear that the in-plane wave functions in this system are quite similar to those in quantum rings, as expected. [39,40,13] The difference between the two systems concerns the wave functions in z-direction, which are spatially restricted in the latter, but free in the former. As in the rings case, in the presence of an axially applied magnetic field, the eigenenergies of individual carriers display oscillations due to the Aharonov-Bohm effect (not shown, see e.g.…”
Section: Single Shell Confinementmentioning
confidence: 99%
See 1 more Smart Citation
“…3, it becomes clear that the in-plane wave functions in this system are quite similar to those in quantum rings, as expected. [39,40,13] The difference between the two systems concerns the wave functions in z-direction, which are spatially restricted in the latter, but free in the former. As in the rings case, in the presence of an axially applied magnetic field, the eigenenergies of individual carriers display oscillations due to the Aharonov-Bohm effect (not shown, see e.g.…”
Section: Single Shell Confinementmentioning
confidence: 99%
“…The main effect of the eccentricity is to create regions of higher curvature and, consequently, lower effective potential, [12,13] which work as traps to the otherwise circularly symmetric charge carriers wavefunctions. A similar effect is investigated e.g.…”
Section: Introductionmentioning
confidence: 99%
“…We treat a gently thickening guide, the thickness variation repeating periodically along the guide. The methodology is similar to, say, Postnova & Craster (2006) and references therein, where trapping is sought in infinite structures or in finite structures such as rings (Gridin et al 2004). Let us take the thickness variation within a cell to be symmetric about the centreline and the upper boundary to be hðexÞ Z 1 C a e where e is a small parameter and the cell is KB=3!x !…”
Section: K1mentioning
confidence: 99%
“…This differs from the WKBJ analysis in Shen et al (1968) for non-rotating free-surface waves and for rotating, stratified edge waves in Zhevandrov (1991), Smith (2004) and Adamou et al (2007) where the alongshore profile is fixed and the waves are short compared to the scale of offshore variations. Topography varying slowly in both horizontal directions is considered for non-rotating free-surface waves by Keller (1958), short topographic Rossby waves in Smith (1970), trapped modes in quantum rings by Gridin et al (2004) and Bruno-Alfonso & Latgé (2008), trapped modes in elastic plates by Gridin et al (2005) and trapped modes in slowly-varying acoustic waveguides by Biggs (2012). The quantum, elastic plate and acoustic problems are more straightforward than the shelf-wave problem in that the modal structure across the waveguide for corresponding forward-and backward-propagating modes is the same whereas in general the long forward-propagating shelf wave mode has cross-shelf structure different from the backward-propagating short shelf wave.…”
Section: Introductionmentioning
confidence: 99%