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Y-123 Films on technical substrates
Affiliation:1. Institut für Metallphysik, Universität Göttingen, Windausweg 2, D-37073 Göttingen, Germany;2. Zentrum für Funktionswerkstoffe gem. GmbH, Göttingen, Windausweg 2, D-37073 Göttingen, Germany;1. Laboratory of Physics of Materials - Structures and Properties, Department of Physics, Faculty of Sciences of Bizerte, University of Carthage, Zarzouna, 7021, Tunisia;2. Department of Physics Research, Institute for Research & Medical Consultations (IRMC), Imam Abdulrahman Bin Faisal University, P.O. Box 1982, Dammam, 31441, Saudi Arabia;3. Department of Physics, Faculty of Sciences & Letter, Çukurova University, 01330, Adana, Turkey;4. Department of Chemistry, Bharath Institute of Higher Education and Research (BIHER), Bharath University, Chennai, 600073, Tamil Nadu, India;5. Department of Physics, College of Science, Imam Abdulrahman Bin Faisal University, P.O. Box 1982, Dammam, 31441, Saudi Arabia;6. Basic and Applied Scientific Research Center, Imam Abdulrahman Bin Faisal University, P.O. Box 1982, 31441, Dammam, Saudi Arabia;1. Institute of Experimental Physics, Slovak Academy of Sciences, Watsonova 47, 04001, Kosice, Slovakia;2. Helmholtz Zentrum Berlin, Hahn-Meitner Platz 1, 14109, Berlin, Germany;3. National Institute for Materials Science (NIMS), International Center for Materials Nanoarchitectonics (WPI-MANA), Center for Functional Sensor & Actuator (CFSN), Namiki 1-1, Tsukuba, 305-0044, Japan;4. University of Tsukuba, Graduate School of Pure and Applied Sciences, 1-1-1 Tennoudai, Tsukuba, 305-8671, Japan;1. University of Craiova, Faculty of Sciences, Department of Physics, Str. A.I. Cuza, Nr 13, 200585 Craiova, Romania;2. University Politehnica of Bucharest, Faculty of Applied Sciences, Department of Physics, Blvd. Splaiul Independenţei, Nr. 313, 060042 Bucharest, Romania;3. IMEM-CNR Institute of Materials for Electronics and Magnetism-National Council for Research, Via alla Cascata 56/C, Povo I-38123, Trento, Italy;4. ICTP-International Centre for Theoretical Physics, High Temperature Superconductivity Laboratory, P.O. Box 34100, Trieste, Italy;5. University of Craiova, Faculty of Horticulture, Department of Horticulture and Food Science, Str. A.I. Cuza, Nr 13, 200585 Craiova, Romania;6. INFLPR-National Institute for Laser, Plasma and Radiation Physics, Bvd. Atomistilor, Nr. 409, 077125 Magurele (Ilfov), Bucharest, Romania;1. Ankara University, Faculty of Science, Department of Physics, Ankara, Turkey;2. Ankara University, Center of Excellence for Superconductivity Research, Ankara, Turkey;3. Kastamonu University, Faculty of Art and Science, Department of Physics, Kastamonu, Turkey;4. Kastamonu University, Faculty of Engineering and Architecture, Department of Electrical and Electronics Engineering, Kastamonu, Turkey;5. Kastamonu University Research and Application Center, Kastamonu, Turkey;1. Department of Materials Engineering, Faculty of Engineering, Imam Khomeini International University, Qazvin, Iran;2. Dipartimento di Fisica “E. Pancini”, Università di Napoli “Federico II”, Complesso Universitario di Monte S. Angelo-Via Cintia, 80126 Napoli, Italy;3. CNR-SPIN UO Napoli, Italy;4. Non-Metallic Materials Research Group, Niroo Research Institute, Tehran, Iran;1. Department of Biophysics, Institute for Research and Medical Consultations (IRMC), Imam Abdulrahman Bin Faisal University, P.O. Box 1982, 31441, Dammam, Saudi Arabia;2. Laboratory of Physics of Materials - Structures and Properties, Department of Physics, Faculty of Sciences of Bizerte, University of Carthage, 7021, Zarzouna, Tunisia;3. Department of Physics, Faculty of Sciences & Letter, Çukurova University, 01330, Adana, Turkey;4. College of Science, Department of Physics, Imam Abdulrahman Bin Faisal University, Dammam, Saudi Arabia
Abstract:For high-current applications, homogeneous well-textured high-temperature superconducting Y1Ba2Cu3O7−δ (Y-123) films on technical ceramic or metallic substrates are required. The ion-beam-assisted deposition (IBAD) of yttria-stabilized zirconia (YSZ) buffer layers, which serve as a template for Y-123, was extended to large-area substrates as well as differently shaped long substrates. TEM, as well as XRD investigations, was performed to observe the relevant growth mechanisms. The influence of nucleation, growth selection, and homoepitaxial growth on the development or the maintenance of a preferential orientation of the YSZ buffer is discussed. Y-123 films were prepared by a modified pulsed-laser-deposition (PLD) technique based on a quasi-equilibrium substrate heating and variable azimuth scanning of the target. The method allows a PLD coating of long pieces of tapes and tubular substrates because no direct mechanical contact of a substrate with the heater is required. Critical current densities, Jc, above 106 A cm−2 were achieved on polycrystalline Ni tapes as well as on polycrystalline YSZ sheets at 77 K and self fields. The dependence of Jc on magnetic field resembles that of Y-123 deposited on single-crystalline substrates and demonstrates the absence of weak links due to grain boundaries. The thickness dependence of Jc is interpreted in terms of a nucleation layer appearing in the early stage of film growth. A growth model is proposed which seems to be in agreement with the experimental observations. The measured strain tolerance of the films does not impede their application.
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