1999
DOI: 10.1038/20880
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Origin of high critical currents in YBa2Cu3O7−δ superconducting thin films

Abstract: Thin films of the high-temperature superconductor YBa 2 Cu 3 O 7 ؊ ␦ exhibit both a large critical current (the superconducting current density generally lies between 10 11 and 10 12 A m −2 at 4.2 K in zero magnetic field) and a decrease in such currents with magnetic field that point to the importance of strong vortex pinning along extended defects 1,2 . But it has hitherto been unclear which types of defect-dislocations, grain boundaries, surface corrugations and anti-phase boundaries-are responsible. Here w… Show more

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Cited by 443 publications
(316 citation statements)
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“…At the same time, at the low field region (self-field region), the 5 Hz film exhibits the most optimal properties at low temperatures. These differences are likely the ground for existing inconsistencies in determining the pinning mechanism in the PLD YBCO films, ranging from dislocation dominance 28,29,61,85 and twin boundaries 81 to small non-superconducting inclusions of Y 2 O 3 83,84 and even surface pinning 86 and Josephson-like weak-links 79 , which may simply represent different but limited aspects of the entire picture, as shown in this work.…”
Section: B Ybco Thin Filmsmentioning
confidence: 99%
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“…At the same time, at the low field region (self-field region), the 5 Hz film exhibits the most optimal properties at low temperatures. These differences are likely the ground for existing inconsistencies in determining the pinning mechanism in the PLD YBCO films, ranging from dislocation dominance 28,29,61,85 and twin boundaries 81 to small non-superconducting inclusions of Y 2 O 3 83,84 and even surface pinning 86 and Josephson-like weak-links 79 , which may simply represent different but limited aspects of the entire picture, as shown in this work.…”
Section: B Ybco Thin Filmsmentioning
confidence: 99%
“…Note, B * can be defined as the field at which the critical current reaches the 90% 79 or 95% 77,78 of the value obtained for zero applied field. However, in this work it is sufficient to qualitatively demonstrate that B * is the transition from a plateau-like J c (B a ) dependence to the power-law dependence and is directly proportional to dislocation density (as well as to the island density at any thickness of the film) 61,77 . The characteristic field B * increases with increasing laser frequency [ Fig.…”
Section: B Ybco Thin Filmsmentioning
confidence: 99%
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“…On the other hand, randomly distributed localized defects (uncorrelated pinning centers) can produce very strong pinning, but do not give rise to a peak for H//c in the J c angular dependence at 77 K. One of the first attempts of correlating J c performance for H//c with the density of extended pinning centers along the c axis was carried out in 1999 [28]. The defects targeted by this study were threading edge and screw dislocations normally occurring during the YBCO growth process, especially in PLD films with their columnar growth mode.…”
Section: Enhancing Naturally Occurring Nanoscale Defectsmentioning
confidence: 99%