1998
DOI: 10.1088/0953-2048/11/4/002
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Current transfer and initial dissipation in high- superconductors

Abstract: Various aspects of the problem of current transfer in high- superconductors (HTSs) are reviewed. The spatial inhomogeneities of various types are identified as a primary cause of non-uniformity of both normal currents and supercurrents in real samples of HTSs. The role these inhomogeneities play in transport features of the samples is discussed. The case of grain boundaries in polycrystalline samples is elaborated in detail. The local structural and transport properties of isolated grain boundaries are first r… Show more

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Cited by 72 publications
(62 citation statements)
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References 225 publications
(373 reference statements)
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“…However, one can observe a change in curvature toward a linear regime when the temperature is lowered. This crossover effect shifts from 87 K down to 65 K, when magnetic field raises from 2 to 6 T. This might indicate that the initial drop in resistivity is initially due to Josephson or tunnel junctions [25]. Finally electrical resistivity vanishes at the percolation temperature shifting from 89 K at zero magnetic field down to 61 K at 6 T field.…”
Section: Electrical Resistivitymentioning
confidence: 92%
“…However, one can observe a change in curvature toward a linear regime when the temperature is lowered. This crossover effect shifts from 87 K down to 65 K, when magnetic field raises from 2 to 6 T. This might indicate that the initial drop in resistivity is initially due to Josephson or tunnel junctions [25]. Finally electrical resistivity vanishes at the percolation temperature shifting from 89 K at zero magnetic field down to 61 K at 6 T field.…”
Section: Electrical Resistivitymentioning
confidence: 92%
“…On the other hand, it is of great importance (from both fundamental and application points of view) to study the evolution of the different current transfer driven dissipation processes in doped superconductors [3]. Probably one of the most recognized dissipation mechanisms is the so-called Kosterlitz-Thouless (KT) topological transition.…”
mentioning
confidence: 99%
“…T cI the temperature at which dρ/dT presents its maximum, and T c0 , the minimum temperature for which ρ = 0 are indicated. In the CVC shown in figure 2, symbols represent the experimental data measured at the indicated temperatures and the solid lines the fits to the usual power law function (Prester, 1998;. In figure 3 circles correspond to the field cooling (FC) of the sample and squares to its zero field cooling (ZFC).…”
Section: Bulk Cylinders As Secondary Of Inductive Sfclmentioning
confidence: 99%
“…E − J curves measured in a piece of the superconducting elements employed in the limiter. The solid lines represent the fittings to the usual power law function (Prester, 1998). In figure 6(a) it is shown the rms values of the five voltage signals and in figure 6(b) the corresponding temperature readings.…”
Section: Samples' Behaviour Under a Current Faultmentioning
confidence: 99%