1999
DOI: 10.1006/spmi.1999.0743
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Properties of superconductor–Luttinger-liquid hybrid systems

Abstract: In this paper we review some recent results concerning the physics of superconductor -Luttinger liquid proximity systems. We discuss both equilibrium (the pair amplitude, Josephson current, and the local density of states) and nonequilibrium (the subgap current) properties.

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Cited by 11 publications
(12 citation statements)
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References 31 publications
(18 reference statements)
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“…[10][11][12][13][14][15][16][17][18] Further extensions such as inclusion of effects due to electron-electron interactions on AR processes in case of NS junctions in the context of onedimensional ͑1D͒ wires have also been considered recently. [19][20][21][22][23][24] In this paper, we shall first develop a general formulation for studying the transport properties of a multiple quantum wire ͑QW͒ junction in the spirit of the "Landauer-Buttiker" approach, 25 where the junction itself is superconducting. We shall use this formulation to study the influence of the proximity effect on the transport properties of a superconducting junction specifically for the case of two and three 1D interacting quantum wires and show how the simple case of junction of a single 1D QW with a superconductor ͑NS junction͒ is different from the multiple wire junction counterpart.…”
Section: Introductionmentioning
confidence: 99%
“…[10][11][12][13][14][15][16][17][18] Further extensions such as inclusion of effects due to electron-electron interactions on AR processes in case of NS junctions in the context of onedimensional ͑1D͒ wires have also been considered recently. [19][20][21][22][23][24] In this paper, we shall first develop a general formulation for studying the transport properties of a multiple quantum wire ͑QW͒ junction in the spirit of the "Landauer-Buttiker" approach, 25 where the junction itself is superconducting. We shall use this formulation to study the influence of the proximity effect on the transport properties of a superconducting junction specifically for the case of two and three 1D interacting quantum wires and show how the simple case of junction of a single 1D QW with a superconductor ͑NS junction͒ is different from the multiple wire junction counterpart.…”
Section: Introductionmentioning
confidence: 99%
“…[4,5] was subsequently extended to account for a resonant energy dependence of the bare S matrix [11,12]. We demonstrate below that the intrinsic energy dependence of Andreev reflection, which was disregarded in earlier works [13,14], is crucial for understanding the transport properties of interacting normal-metal-superconductor nanostructures.One experimental realization of a quasi-onedimensional electron system is provided by a single-wall carbon nanotube. In recent experiments [15] the differential Andreev conductance was dominated by the interface between a carbon nanotube and a superconductor.…”
mentioning
confidence: 99%
“…Here Ξ(0, L) measures the amplitude for two spins of opposite orientation introduced at x = L to arrive at x = 0. Deep in the SILL regime where all the spins are randomized and spin exchange is highly suppressed, this is just the probability of finding neighboring sites of the spin chain housing oppositely aligned spins, (53) where η ≪ 1 is a short distance cut-off that ensures ultra violet convergence of the integrals over the charge fluctuations in the wire. Up to unimportant phase factors and other overall multiplicative constants, the Josephson current in the wire is then…”
Section: Josephson Effectmentioning
confidence: 99%
“…15 In the opposite limit of a tunnel contact between the SC and SILL, no proximity effects of the SC are felt other than those perturbative in the tunneling. 53 (In contrast to the Andreev limit where the behavior of the pair correlations and tunneling density of states follows directly from the form of the field expansions imposed by the boundary conditions. 15 ) As the proximity effects are already weak in the Andreev limit (they decay exponentially fast with distance, unlike the power law decay in the LL 33 ) we do not pursue the very weak proximity effects in the spin-incoherent regime in the limit of a weak tunneling SC-SILL junction.…”
Section: A Sc-sill Junctionsmentioning
confidence: 99%