By John Clarke, Du Quan, M. J. Ferrari, J. J. Kingston, A. H. Miklich, F. C. Wellstood (auth.), Dr. Koji Kajimura, Prof. Dr. Hisao Hayakawa (eds.)
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Extra info for Advances in Superconductivity III: Proceedings of the 3rd International Symposium on Superconductivity (ISS ’90), November 6–9, 1990, Sendai
14 123 100A 211 Fig. 5. High resolution transmISSIOn electron micrograph of the interface between the 211 and the 123 matrix. Transmission electron micrographs for MPMG grown YBaCuO crystals (a) Fig. 6. with and (b) without 211 observed from the direction perpendicular to the c axis. 0 pinned fluxold 1 / 0 0 0 0 0 0 0 0 0 0 1 0 0 pinning center • • 0 0 0 0 0 - 0 Lorenz force Fig. 7. Schematic illustration of the interaction between flux line lattice and a large non -superconducting particle. 15 DISCUSSION All the above observations support that the dispersion of 211 inclusions into the However, there remains the question 123 matrix can contribute to the increase in Ic.
Figure 3 shows the irreversibility line for YBaCuO single crystal and MPMG grown YBaCuO containing the 211 inclusions when the magnetic field was applied parallel to the c axis I4 ). The line was determined from the peak of imaginary component of AC susceptibility in the presence of DC magnetic field. The irreversibility line can be shifted toward higher H-T region by the 211 doping. : - e. "i) c: i CD a C 10 4 ! 0 100 103 0 5 Magnetic Field (kOe) .... 8 fti g (5 .... ~ u 17K ... -- -.... 1000 Time (s) • ' ......
Appl. Phys. 27: L1902 Slakey F, Klein MV, Bukowski EO, Ginsberg OM '(1990) Phys. Rev. B 41: 2109 Phillips NE, Fisher RA, Gordon JE, Kim S, Stacy AM, Crawford MK, McCarron EM (1990) Phys. Rev. Letters 65: 357 Ginsberg OM, private communication Loram J, private communication Slakey F, Klein MY, Rice JP, and Ginsberg DM (1990) Phys. Rev. B 42: 2643 Orenstein J, Thomas GA, Millis AJ, Cooper SL, Rapkine DH, Timusk T, Schneemeyer LF, Waszczak JV (1990) Phys. Rev. -Ansermet, 1211 Geneva 4, Switzerland Department of Applied Physics, Stanford University, Stanford CA 94305, USA Laboratoire de Chimie Minerale B, University of Rennes I, avo du General Leclerc, Cedex 35042, France Siemens Research Laboratories, Otto Hahn Ring 6, D-8000 Munich, Germany ABSTRACT YBa2Cu307/PrBa2Cu307 (YBCO/PrBCO) superlattices grown by single target dc planar magnetron sputtering are used as a model system to investigate flux motion in high T c superconductors.
Advances in Superconductivity III: Proceedings of the 3rd International Symposium on Superconductivity (ISS ’90), November 6–9, 1990, Sendai by John Clarke, Du Quan, M. J. Ferrari, J. J. Kingston, A. H. Miklich, F. C. Wellstood (auth.), Dr. Koji Kajimura, Prof. Dr. Hisao Hayakawa (eds.)