1971
DOI: 10.1139/p71-033
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Scattering and Tunneling of Electronic Excitations in the Intermediate State of Superconductors

Abstract: We give a systematic discussion of the anomalous scattering of Bogoliubov excitations at sharp N–S and S–N boundaries as well as quasi-particle tunneling in N–S–N and S–N–S geometries. The relation between the transmission resonances (E > Δ) and the bound states (E < Δ) in N–S–N and S–N–S geometries is explicitly exhibited. We also work out the extra thermal resistance due to scattering by a normal layer imbedded in a superconductor and by a superconducting layer imbedded in a normal metal, with results … Show more

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Cited by 65 publications
(35 citation statements)
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“…Since early experiments by Tomasch, 30 the geometric resonance nature of the differential conductance oscillations in SNS and NSN tunnel junctions has been ascribed to the electron interference in the central film. 31,32,33,34 Recently, McMillan-Rowell oscillations were observed in SNS edge junctions of d-wave superconductors and used for measurements of the superconducting gap and the Fermi velocity. 35 In this paper we study coherent electronic transport in FSF double-barrier junctions (and NSN as a special case) within the framework of BCS theory.…”
Section: 2122mentioning
confidence: 99%
“…Since early experiments by Tomasch, 30 the geometric resonance nature of the differential conductance oscillations in SNS and NSN tunnel junctions has been ascribed to the electron interference in the central film. 31,32,33,34 Recently, McMillan-Rowell oscillations were observed in SNS edge junctions of d-wave superconductors and used for measurements of the superconducting gap and the Fermi velocity. 35 In this paper we study coherent electronic transport in FSF double-barrier junctions (and NSN as a special case) within the framework of BCS theory.…”
Section: 2122mentioning
confidence: 99%
“…If the thickness d of the superconducting slab is much larger than the coherence length ξ the electrons incident on the slab are reflected as holes, and the normal current converts into the supercurrent. Single-electron tunneling through an N-S-N structure decays exponentially with the slab thickness giving rise, in particular, to the exponential drop off of the electronic contribution to the thermal conductance [1,2]. A single-particle transport through NSN recovers by applying a strong magnetic field, which creates vortex lines where the gap in the spectrum is suppressed.…”
mentioning
confidence: 99%
“…where H (1,2) l are the Hankel functions, l = µ 2 + 1/4, assuming thatŵ = (w 1 , w 2 ) are slow functions of r and z. Following [14] we put x = √ r 2 − b 2 , b = −µ/k r and define the trajectories dx = ±ds ± sin θ, dz = ds ± cos θ forŵ (±) , respectively, where k z = k F cos θ and ds ± is the distance along the corresponding trajectory.…”
mentioning
confidence: 99%
“…We have already cited the thermal conductivity calculations of Demers and Griffin [6] and Ambegaokar and Griffin [21]. Another application which has been suggested [22] is the calculation of the local fields and energy dissipation in the mixed state of type I1 superconductors.…”
Section: Summary and Discussionmentioning
confidence: 99%