Synthesis and properties of YBa2Cu3O7 thin films grown in situ by 90° off-axis single magnetron sputtering

Abstract High quality superconducting films of YBa 2 Cu 3 O 7− x were deposited in situ using single target 90° off-axis sputtering. We have investigated their superconducting DC and RF properties, their normal state properties, and their microstructures. These films are distinctly different from bulk crystals and post-deposition annealed films. Sharp superconducting transition temperatures can be reproducibly obtained by control of deposition parameters. The T c can be varied from 75 to 89 K. The optimization of properties other than T c and the control of film texture occur under conditions different from those for which the highest T c is obtained. Normal state conductivities are as high as or higher than those of single crystals. Critical current densities reach 6 × 10 7 A/cm 2 at 4.2 K. All the above properties are relatively insensitive to compositional variations. The T c 's have a much weaker dependence on the c -axis lattice parameters than do those of bulk samples. The measured low-temperature penetration depth is 1400 A and surface resistance at 4.2 K and 10 GHz is as low as 16 μΩ. Microstructural studies show sharp interfaces between films and their substrates and a variety of defect structures. Many of the properties of in situ films can be explained by clean grain boundaries and the characteristics of the surface growth occuring during in situ deposition.

[1]  Gallagher,et al.  Direct observation of electronic anisotropy in single-crystal Y1Ba2Cu3O7-x. , 1987, Physical review letters.

[2]  D. Frankel Critical‐state model for the determination of critical currents in disk‐shaped superconductors , 1979 .

[3]  Michael Tinkham,et al.  Introduction to Superconductivity , 1975 .

[4]  J. Turneaure,et al.  Microwave Surface Resistance of Superconducting Niobium , 1968 .

[5]  E. Kramer Summation curves for flux pinning in superconductors , 1978 .

[6]  M. Beasley,et al.  Reactive magnetron sputtering of thin‐film superconductor YBa2Cu3O7−x , 1987 .

[7]  T. F. Smith,et al.  Time-dependent magnetization behaviour for type II superconductors - V3Si , 1989 .

[8]  H. C. Li,et al.  In situ preparation of Y‐Ba‐Cu‐O superconducting thin films by magnetron sputtering , 1988 .

[9]  M. Tachiki,et al.  Strong vortex pinning intrinsic in high-Tc oxide superconductors , 1989 .

[10]  McGuire,et al.  Critical currents in , 1988, Physical review letters.

[11]  J. Ekin Irregularity in NbTi filament area and electric field versus current characteristics , 1987 .

[12]  G. K. Wehner,et al.  Angular Distribution of Sputtered Material , 1960 .

[13]  C. Eom,et al.  In situ grown YBa2Cu3O7−d thin films from single‐target magnetron sputtering , 1989 .

[14]  M. Beasley,et al.  In situ growth of superconducting YBaCuO using reactive electron-beam coevaporation , 1989 .

[15]  T. R. Dinger,et al.  Reliable single‐target sputtering process for high‐temperature superconducting films and devices , 1988 .

[16]  Malozemoff,et al.  Giant flux creep and irreversibility in an Y-Ba-Cu-O crystal: An alternative to the superconducting-glass model. , 1988, Physical review letters.

[17]  M. Tinkham,et al.  Physical Properties of the New Superconductors , 1989 .

[18]  Larkin,et al.  Theory of collective flux creep. , 1989, Physical review letters.

[19]  T. L. Hylton,et al.  Growth and properties of sputtered high-T/sub c/ oxide thin films , 1989 .

[20]  J. Sun,et al.  Magnetic flux motion and its influence on transport properties of the high Tc oxide superconductors , 1989 .

[21]  Nathan Newman,et al.  Microwave surface resistance of epitaxial YBa2Cu3O7 thin films on sapphire , 1990 .

[22]  B. Wilkens,et al.  YBa2Cu3O7-δ superconducting films with low microwave surface resistance over large areas , 1990 .

[23]  Brandt Eh Range and strength of pins collectively interacting with the flux-line lattice in type-II superconductors. , 1986 .

[24]  Hoi Sing Kwok,et al.  Deposition of superconducting Y‐Ba‐Cu‐O films at 400 °C without post‐annealing , 1988 .

[25]  M. Kitabatake,et al.  Low‐temperature process for the preparation of high Tc superconducting thin films , 1987 .

[26]  Wu,et al.  Temperature dependence of electrodynamic properties of YBa2Cu3Oy crystals. , 1989, Physical review letters.

[27]  M. Beasley,et al.  Measurements of the magnetic penetration depth in YBa2Cu3O7−δ thin films by the microstrip resonator technique , 1989 .

[28]  M. S. Hegde,et al.  Microstructure of in situ epitaxially grown superconducting Y‐Ba‐Cu‐O thin films , 1989 .

[29]  S. Casadio,et al.  Small field behavior of critical current in Y1Ba2Cu3O7 sintered samples , 1988 .

[30]  R. V. Dover,et al.  Magnetization and critical currents of Bi‐Sr‐Ca‐Cu‐O and Ba2YCu3O7 superconductors , 1988 .

[31]  Aly E. Fathy,et al.  Microwave properties of highly oriented YBa2Cu3O7−x thin films , 1990 .

[32]  H. Jones,et al.  The Detailed Investigation of the Critical Current Density of Optimized Nb3Sn Modified Jelly Roll Wire throughout Its Entire Superconducting Phase Including a Comparative Study with a Similar Non-Optimized Composite , 1987 .

[33]  T. Venkatesan,et al.  Preparation of Y‐Ba‐Cu oxide superconductor thin films using pulsed laser evaporation from high Tc bulk material , 1987 .