1996
DOI: 10.1103/physrevb.54.15530
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Origin of the irreversibility line in thinYBa2Cu3O

Abstract: We report on measurements of the angular dependence of the irreversibility temperature T irr (θ) in Y Ba 2 Cu 3 O 7−δ thin films, defined by the onset of a third harmonic signal and measured by a miniature Hall probe. From the functional form of T irr (θ) we conclude that the origin of the irreversibility line in unirradiated films is a dynamic crossover from an unpinned to a pinned vortex liquid. In irradiated films the irreversibility temperature is determined by the trapping angle.

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Cited by 20 publications
(6 citation statements)
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References 74 publications
(129 reference statements)
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“…Note that similar results were obtained in YBCO crystals and thin films, 8,12,15 but no explanation was proposed. First of all, the absence of a peak cannot be ascribed merely to a 2D behavior of vortices, 42 for that would yield a ⌬M () independent of at fixed H c , in contrast to the strong angular dependence seen in Fig.…”
Section: Discussionmentioning
confidence: 59%
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“…Note that similar results were obtained in YBCO crystals and thin films, 8,12,15 but no explanation was proposed. First of all, the absence of a peak cannot be ascribed merely to a 2D behavior of vortices, 42 for that would yield a ⌬M () independent of at fixed H c , in contrast to the strong angular dependence seen in Fig.…”
Section: Discussionmentioning
confidence: 59%
“…For the latter, in the case of two sets of tilted defects, the angular dependences of resistivity and of the magnetic properties are similar: maxima of current densities, 15,21,22 of H irr , 8,12 and minima of resistivity 19,20 are obtained when the magnetic field is applied along the mid-direction of the defects ͓i.e., along the c axis for defects tilted by Ϯ i from c ͑see, e.g., Ref. 15͒, or for example 10°from c for defects tilted by 5°a nd 15°͑Ref.…”
Section: Discussionmentioning
confidence: 88%
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“…Hence the interpretation of the parameters derived from resistive data can equally be in terms of giving the boundary for zero-resistance percolation in a highly disordered or inhomogeneous superconductor 46 or in terms of a transition from a pinned to unpinned vortex liquid. 47,48 To contribute to unravelling the complexity of magnetic phase diagrams, we suggest that measurements of B IRR and can be improved to give data closer to the ultimate sensitivity of the instrument rather than limited by the field inhomogeneity of the magnet.…”
Section: A the Magnetic Phase Diagram Of Superconductorsmentioning
confidence: 99%