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14 - Controlling the structure and properties of high Tc thin-film devices

Published online by Cambridge University Press:  21 August 2009

Nigel D. Browning
Affiliation:
University of Illinois, Chicago
Stephen J. Pennycook
Affiliation:
Oak Ridge National Laboratory, Tennessee
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Summary

Introduction

The highly anisotropic crystal structures of the layered high Tc superconducting cuprates induce the necessity of using epitaxial films in most devices based on high Tc thin films. Each individual application demands a specific crystallographic orientation of the film as well as a certain combination of substrate, high Tc superconducting film and non-superconducting layer materials. The intention of this chapter is to provide examples of what aspects need to be considered when designing the device and predicting its behavior. The behavior depends on the detailed microstructure of the thin films. The examples are therefore discussed in terms of microstructure and how it can be controlled and manipulated.

As in all epitaxial structures, the interfacial interactions are crucial for the resulting microstructures. The direct interaction between the substrate and a single-layer high Tc thin film is illustrated in the following section. The description is followed by a discussion of different aspects of the use of buffer layers. The text is restricted to high Tc YBa2Cu3O7–x (YBCO), mainly owing to the fact that the vast majority of published data concern this superconductor. However, there are common characteristics of epitaxial film growth between different high Tc superconductors. Results from the YBCO films can thus be used when considering the other high Tc superconducting thin films which is pointed out in Section 14.10.

The mechanical interaction between the different epitaxial layers may result in the formation of misfit dislocations. Nucleation and propagation of cracks can ensue if the mismatch in thermal expansion coefficient is relatively large.

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Publisher: Cambridge University Press
Print publication year: 2000

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