By Shoji Tanaka (auth.), Tsutomu Yamashita, Kei-ichi Tanabe (eds.)
The twelfth overseas Symposium on Superconductivity was once held in Morioka, Japan, October 17-19, 1999. Convened each year when you consider that 1988, the symposium covers the total box of superconductivity from primary physics and chemistry to quite a few functions. on the twelfth Symposium, a mini-symposium concentrating on the two-dimensionality of high-temperature superconductors, or the c-axis shipping, and a consultation on vortex physics have been geared up. there have been additionally many studies at the fresh advancements of YBCO-based covered conductors either within the usa and in Japan, AC losses of wires and tapes, advancements of bulk fabrics with powerful flux pinning, the new development in skinny movie and junction applied sciences, and the demonstration of varied electronics purposes utilizing SQUIDs, microwave units, and single-flux-quantum (SFQ) electronic units. This quantity is a priceless source for all these operating within the box of superconductivity.
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Additional resources for Advances in Superconductivity XII: Proceedings of the 12th International Symposium on Superconductivity (ISS ’99), October 17–19, 1999, Morioka
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This year the NEC group tried to integrate 1000 junctions and the obtained spread of the critical current was less than 10%. These results mentioned above give us hope in obtaining in a few years 10000 junctions integration having spread of the critical current of 5%. Fig. 6. HRTEM image at the junction area of the NEC junction. The period of 3-times provskite for YBCO is absent in the barrier layer. 1A). 5 n - V ....... ::! I. 0 -:1~ ~:'I 4 ~ --- ... 1 102 Jc (A/cm2) Fig. 7. Relation between Ie and leRn for surface modified junctions.
The pinning mechanism, known as intrinsic pinning, is similar to that by normal particles in LTS. The density of pins is, however, much greater than the density of flux lines. This explains the relative insensitivity of the current density to external magnetic field in the middle region of the Je versus B curve. When the applied field is normal to the ab planes, the intrinsic pinning no longer acts to hinder flux line motion; critical current densities are much lower than when the field is parallel to the planes.