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Title: Thermal expansion of LaAlO{sub 3} and (La,Sr)(Al,Ta)O{sub 3}, substrate materials for superconducting thin-film device applications

Journal Article · · Journal of Applied Physics
DOI:https://doi.org/10.1063/1.366925· OSTI ID:573943
 [1];  [2];  [3];  [4]
  1. Solid State Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6393 (United States)
  2. Department of Materials Science and Engineering, Pennsylvania State University, University Park, Pennsylvania 16802-5005 (United States)
  3. Commercial Crystal Laboratories, Inc., 4406 Arnold Avenue, Naples, Florida 33942 (United States)
  4. TRW, One Space Park, Redondo Beach, California 90278 (United States)

The thermal expansion for the perovskite (La,Sr)(Al,Ta)O{sub 3}, i.e., LSAT, grown from the formulation 0.29(LaAlO{sub 3}):0.35(Sr{sub 2}AlTaO{sub 6}), was determined by Rietveld refinement of neutron powder diffraction data over the temperature range of 15{endash}1200 K. In comparison to LaAlO{sub 3} the relative volume thermal expansion is the same, although the cell volume of LSAT is slightly larger. Site occupation refinement for LSAT gives a structural formula of (La{sub 0.29(5)}Sr{sub 0.71(5)}){sub A site}(Al{sub 0.65(1)}Ta{sub 0.35(1)}){sub B site}O{sub 3}. At and below 150 K, LSAT shows a small distortion from cubic symmetry. Unlike the cubic-to-rhombohedral transition (800 K) observed in LaAlO{sub 3}, the low temperature structural phase transition in LSAT appears to be cubic-to-tetragonal or cubic-to-orthorhombic. The rms displacement of the A site in LSAT is significantly larger than that for LaAlO{sub 3}, and about half of the difference can be accounted for by a static displacement component. {copyright} {ital 1998 American Institute of Physics.}

OSTI ID:
573943
Journal Information:
Journal of Applied Physics, Vol. 83, Issue 4; Other Information: PBD: Feb 1998
Country of Publication:
United States
Language:
English