A new structural modification of superconducting La<sub>2−x</sub>M<sub>x</sub>CuO<sub>4</sub>

J. D. Axe, D. E. Cox, K. M. Mohanty, H. Moudden, A. R. Moodenbaugh, Y. Xu, T. R. Thurston

IBM Journal of Research and Development · 1989 · 82 citations · 9 references

Concepts

Abstract

La <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1.9</inf> Ba <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.1</inf> CuO <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">4</inf> has been observed to undergo the following sequence of transformations upon cooling from 300 K: tetragonal (I4/mmm) equation orthorhombic (Cmca) equation tetragonal (P4 <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</inf> /ncm). The newly discovered low-temperature tetragonal structure can be understood geometrically as arising from a coherent superposition of the two domain modifications of the orthorhombic structure. Dynamically, it results from a second instability in the twofold degenerate soft modes of the high-temperature tetragonal phase. Energetically, the system can be modeled as an XY-spin system with temperature-dependent quartic anisotropy ν(T), and the low-temperature transformation coincides with an isotropic point ν(T <inf xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">1</inf> ) = 0. The relationship of the newly discovered transformation to other anomalous properties and to superconductivity is discussed briefly.

References

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