2010
DOI: 10.1088/0957-4484/21/27/272001
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Charge transport through single molecules, quantum dots and quantum wires

Abstract: Abstract. We review recent progresses in the theoretical description of correlation and quantum fluctuation phenomena in charge transport through single molecules, quantum dots, and quantum wires. A variety of physical phenomena is addressed, relating to co-tunneling, pair-tunneling, adiabatic quantum pumping, charge and spin fluctuations, and inhomogeneous Luttinger liquids. We review theoretical many-body methods to treat correlation effects, quantum fluctuations, nonequilibrium physics, and the time evoluti… Show more

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Cited by 109 publications
(105 citation statements)
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References 238 publications
(440 reference statements)
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“…At appropriate conditions, these systems consist of discrete energy levels of quantum dots, which are hybridized with the leads, having continuous energy bands. It is well known that physical properties of such zero-dimensional structures are strongly influenced by Coulomb electron interaction effects, leading to non-trivial interactioninduced effects [16][17][18] (e.g., the Kondo effect [19]). …”
Section: Introductionmentioning
confidence: 99%
“…At appropriate conditions, these systems consist of discrete energy levels of quantum dots, which are hybridized with the leads, having continuous energy bands. It is well known that physical properties of such zero-dimensional structures are strongly influenced by Coulomb electron interaction effects, leading to non-trivial interactioninduced effects [16][17][18] (e.g., the Kondo effect [19]). …”
Section: Introductionmentioning
confidence: 99%
“…The search for new paradigms in electronics has spurred interest in other quantum phenomena at the nanoscale: electron correlations offer the promise of new functionality in nanoelectronics related to the possible manipulation of manybody ground states in suitably produced nanostructures such as quantum dots and nanoribbons [12][13][14] . An important example that has attracted a great deal of attention is the Kondo state, realized by coupling a magnetic impurity to conduction electrons [see, for example, section VII of Ref.…”
Section: Introductionmentioning
confidence: 99%
“…Further, let us take c 1 (0) = c 10 and c 2 (0) = c 20 ; we will assume that the deviations of c 1 (t) and c 2 (t) from c 10 and c 20 respectively will be of order V at all values of t. At first order, we can replace c 1 (t) and c 2 (t) by c 10 and c 20 on the right hand sides in Eqs. (42). This gives …”
Section: Resonant Case With Ementioning
confidence: 90%