Abstract:An inductive methodology simultaneously enabling the determination of grain- and intergrain critical current densities of YBa2Cu3O7−x coated conductors is developed. This noninvasive method is based on the identification of a clear peak in the reverse branch of the magnetization loop at a positive magnetic field, as a signature of the electromagnetic granularity inherent to these materials. A quantitative evaluation of the return magnetic field at the grain boundaries allows us to understand the existence of t… Show more
“…4 when |H a | is decreased. As mentioned already, our system can be regarded as granular, like a coated-conductor 42,43 . In the simplest view, the grains correspond to the graphene area overlapping with the Al pads, and the grain boundary, across which the dissipative/non-dissipative Josephson supercurrent flows, corresponds to the bare graphene weak link.…”
Section: Collapse Of the Josephson Supercurrent Close To Zero Magnmentioning
Superconducting hybrid junctions are revealing a variety of novel effects. Some of them are due to the special layout of these devices, which often use a coplanar configuration with relatively large barrier channels and the possibility of hosting Pearl vortices. A Josephson junction with a quasi ideal two-dimensional barrier has been realized by growing graphene on SiC with Al electrodes. Chemical Vapor Deposition offers centimeter size monolayer areas where it is possible to realize a comparative analysis of different devices with nominally the same barrier. In samples with a graphene gap below 400 nm, we have found evidence of Josephson coherence in presence of an incipient BerezinskiiKosterlitz-Thouless transition. When the magnetic field is cycled, a remarkable hysteretic collapse and revival of the Josephson supercurrent occurs. Similar hysteresis are found in granular systems and are usually justified within the Bean Critical State model (CSM). We show that the CSM, with appropriate account for the low dimensional geometry, can partly explain the odd features measured in these junctions.
“…4 when |H a | is decreased. As mentioned already, our system can be regarded as granular, like a coated-conductor 42,43 . In the simplest view, the grains correspond to the graphene area overlapping with the Al pads, and the grain boundary, across which the dissipative/non-dissipative Josephson supercurrent flows, corresponds to the bare graphene weak link.…”
Section: Collapse Of the Josephson Supercurrent Close To Zero Magnmentioning
Superconducting hybrid junctions are revealing a variety of novel effects. Some of them are due to the special layout of these devices, which often use a coplanar configuration with relatively large barrier channels and the possibility of hosting Pearl vortices. A Josephson junction with a quasi ideal two-dimensional barrier has been realized by growing graphene on SiC with Al electrodes. Chemical Vapor Deposition offers centimeter size monolayer areas where it is possible to realize a comparative analysis of different devices with nominally the same barrier. In samples with a graphene gap below 400 nm, we have found evidence of Josephson coherence in presence of an incipient BerezinskiiKosterlitz-Thouless transition. When the magnetic field is cycled, a remarkable hysteretic collapse and revival of the Josephson supercurrent occurs. Similar hysteresis are found in granular systems and are usually justified within the Bean Critical State model (CSM). We show that the CSM, with appropriate account for the low dimensional geometry, can partly explain the odd features measured in these junctions.
“…In this way they were able to determine the in-grain and grain boundary critical currents of an YBa 2 Cu 3 O 7−δ coated conductor sample. In a series of articles Palau and coworkers have extensively employed a similar technique, based on the identification of a peak in the M-H loop caused by material granularity, to study the in-grain and grain boundary contributions to the overall behaviour of IBAD and RABiTS based coated conductors [75,105]. In particular they have used magnetisation measurements to study the effect of the extent to which the superconducting layer adopts the granular structure of the substrate [106].…”
Section: Critical Currents From Magnetisation Measurementsmentioning
confidence: 99%
“…Magnetisation measurements have been developed to study separately IG and GB properties in coated conductors [75,76] but this method does not give satisfactory results with single boundaries. However, by lithographically patterning a current ring both Verebelyi [70] and Thompson [77] current to cross the grain boundary in two defined places.…”
Section: The In-field Properties Of Grain Boundariesmentioning
Abstract. Over the past ten years the perception of grain boundaries in YBa 2 Cu 3 O 7−δ conductors has changed greatly. They are no longer a problem to be eliminated but an inevitable and potentially favourable part of the material. This change has arisen as a consequence of new manufacturing techniques which result in excellent grain alignment, reducing the spread of grain boundary misorientation angles. At the same time there is considerable recent evidence which indicates that the variation of properties of grain boundaries with mismatch angle is more complex than a simple exponential decrease in critical current. This is due to the fact that low-angle grain boundaries represent a qualitatively different system to high angle boundaries. The time is therefore right for a targetted review of research into low-angle YBa 2 Cu 3 O 7−δ grain boundaries. This article does not purport to be a comprehensive review of the physics of grain boundaries as found in YBa 2 Cu 3 O 7−δ in general; for a broader overview we would recommend that the reader consult the comprehensive review of Hilgenkamp and Mannhart (Rev. Mod. Phys., 74, 485, 2002). The purpose of this article is to review the origin and properties of the low-angle grain boundaries found in YBa 2 Cu 3 O 7−δ coated conductors both individually and as a collective system.
“…This behavior has been found experimentally in cases in which the SC was granular and was associated to this granularity. 23,24 With the PM used in Fig. 3, unlike the cases of Fig.…”
Section: Tunability Of the Critical-current Density In Superconductormentioning
Important modifications on the magnetization loops of the superconductor have been observed in superconductor-ferromagnet hybrids due to the effects of the ferromagnetic components, which can be used for tuning the superconductor critical-current density Jc to desirable values. Here, a model based on an energy minimization procedure is presented to analyze the complex interaction between the superconductor and the ferromagnets. We show how the geometry and orientation of the ferromagnets can be chosen for shifting the position of the peaks appearing in the magnetization to positive or negative applied fields, and, consequently, to tune Jc in superconductor-ferromagnet hybrids.
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