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Semiclassical transport in nearly symmetric quantum dots. I. Symmetry breaking in the dot

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Semiclassical transport in nearly symmetric quantum dots. I. Symmetry breaking in the dot. / Whitney, Robert S.; Schomerus, Henning; Kopp, Marten.
In: Physical Review E, Vol. 80, No. 5, 11.2009, p. 056209.

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Whitney RS, Schomerus H, Kopp M. Semiclassical transport in nearly symmetric quantum dots. I. Symmetry breaking in the dot. Physical Review E. 2009 Nov;80(5):056209. doi: 10.1103/PhysRevE.80.056209

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Whitney, Robert S. ; Schomerus, Henning ; Kopp, Marten. / Semiclassical transport in nearly symmetric quantum dots. I. Symmetry breaking in the dot. In: Physical Review E. 2009 ; Vol. 80, No. 5. pp. 056209.

Bibtex

@article{4a97310a321e44dd819d1b2a750bebd6,
title = "Semiclassical transport in nearly symmetric quantum dots. I. Symmetry breaking in the dot",
abstract = "We apply the semiclassical theory of transport to quantum dots with exact and approximate spatial symmetries; left-right mirror symmetry, up-down mirror symmetry, inversion symmetry, or fourfold symmetry. In this work—the first of a pair of articles—we consider (a) perfectly symmetric dots and (b) nearly symmetric dots in which the symmetry is broken by the dot's internal dynamics. The second article addresses symmetry-breaking by displacement of the leads. Using semiclassics, we identify the origin of the symmetry-induced interference effects that contribute to weak localization corrections and universal conductance fluctuations. For perfect spatial symmetry, we recover results previously found using the random-matrix theory conjecture. We then go on to show how the results are affected by asymmetries in the dot, magnetic fields, and decoherence. In particular, the symmetry-asymmetry crossover is found to be described by a universal dependence on an asymmetry parameter gamma_asym. However, the form of this parameter is very different depending on how the dot is deformed away from spatial symmetry. Symmetry-induced interference effects are completely destroyed when the dot's boundary is globally deformed by less than an electron wavelength. In contrast, these effects are only reduced by a finite amount when a part of the dot's boundary smaller than a lead-width is deformed an arbitrarily large distance.",
author = "Whitney, {Robert S.} and Henning Schomerus and Marten Kopp",
year = "2009",
month = nov,
doi = "10.1103/PhysRevE.80.056209",
language = "English",
volume = "80",
pages = "056209",
journal = "Physical Review E",
issn = "1539-3755",
publisher = "American Physical Society",
number = "5",

}

RIS

TY - JOUR

T1 - Semiclassical transport in nearly symmetric quantum dots. I. Symmetry breaking in the dot

AU - Whitney, Robert S.

AU - Schomerus, Henning

AU - Kopp, Marten

PY - 2009/11

Y1 - 2009/11

N2 - We apply the semiclassical theory of transport to quantum dots with exact and approximate spatial symmetries; left-right mirror symmetry, up-down mirror symmetry, inversion symmetry, or fourfold symmetry. In this work—the first of a pair of articles—we consider (a) perfectly symmetric dots and (b) nearly symmetric dots in which the symmetry is broken by the dot's internal dynamics. The second article addresses symmetry-breaking by displacement of the leads. Using semiclassics, we identify the origin of the symmetry-induced interference effects that contribute to weak localization corrections and universal conductance fluctuations. For perfect spatial symmetry, we recover results previously found using the random-matrix theory conjecture. We then go on to show how the results are affected by asymmetries in the dot, magnetic fields, and decoherence. In particular, the symmetry-asymmetry crossover is found to be described by a universal dependence on an asymmetry parameter gamma_asym. However, the form of this parameter is very different depending on how the dot is deformed away from spatial symmetry. Symmetry-induced interference effects are completely destroyed when the dot's boundary is globally deformed by less than an electron wavelength. In contrast, these effects are only reduced by a finite amount when a part of the dot's boundary smaller than a lead-width is deformed an arbitrarily large distance.

AB - We apply the semiclassical theory of transport to quantum dots with exact and approximate spatial symmetries; left-right mirror symmetry, up-down mirror symmetry, inversion symmetry, or fourfold symmetry. In this work—the first of a pair of articles—we consider (a) perfectly symmetric dots and (b) nearly symmetric dots in which the symmetry is broken by the dot's internal dynamics. The second article addresses symmetry-breaking by displacement of the leads. Using semiclassics, we identify the origin of the symmetry-induced interference effects that contribute to weak localization corrections and universal conductance fluctuations. For perfect spatial symmetry, we recover results previously found using the random-matrix theory conjecture. We then go on to show how the results are affected by asymmetries in the dot, magnetic fields, and decoherence. In particular, the symmetry-asymmetry crossover is found to be described by a universal dependence on an asymmetry parameter gamma_asym. However, the form of this parameter is very different depending on how the dot is deformed away from spatial symmetry. Symmetry-induced interference effects are completely destroyed when the dot's boundary is globally deformed by less than an electron wavelength. In contrast, these effects are only reduced by a finite amount when a part of the dot's boundary smaller than a lead-width is deformed an arbitrarily large distance.

U2 - 10.1103/PhysRevE.80.056209

DO - 10.1103/PhysRevE.80.056209

M3 - Journal article

VL - 80

SP - 056209

JO - Physical Review E

JF - Physical Review E

SN - 1539-3755

IS - 5

ER -