Orientational epitaxy and lateral structure of the hexagonally reconstructed Pt(001) and Au(001) surfaces

D. L. Abernathy, S. G. J. Mochrie, D. M. Zehner, G. Grübel, and Doon Gibbs
Phys. Rev. B 45, 9272 – Published 15 April 1992
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Abstract

We present results of synchrotron-x-ray-scattering studies of the orientational epitaxy exhibited by clean, hexagonally reconstructed Pt(001) and Au(001) surfaces. For the Pt(001) surface, a high-symmetry direction of the hexagonal overlayer is aligned with a high-symmetry direction of the bulk between 1820 and 1685 K. Between 1685 and ∼1580 K, the relative rotation angle varies continuously from 0° to 0.75° with a one-half-power-law dependence on the reduced temperature. At ∼1580 K, domains with a rotation angle of 0.8° appear discontinuously, in coexistence with those with a rotation angle of 0.75°. The two rotation angles reach ∼0.9° and ∼0.75° for the continuously and discontinuously rotated components, respectively, at 300 K. At all temperatures, the overlayer is incommensurate along both directions of the surface, with weakly temperature-dependent incommensurabilities. The areal density of the Pt(001) overlayer is compressed by ∼8% with respect to the hexagonal (111) planes in the bulk. In addition, the extent of translational order within the surface layer decreases with decreasing temperature. The Au(001) surface exhibits a strongly discontinuous rotational transformation at ∼980 K and there is coexistence between rotated and unrotated domains, in agreement with previous measurements. Rotated domains appear at a rotation angle of ∼0.8° and their number grows with decreasing temperature at the expense of unrotated domains. Our measurements reveal the existence of additional favored rotation angles: one of 0.9° and one that varies smoothly from 0° to 0.5°. The relative domain populations depend on temperature. A mean-field theory of rotational transformations, which accounts for the continuous rotational behavior of the Pt(001) surface, is presented, and it is shown that there are no corrections to mean-field behavior from fluctuations for a rotational transformation.

  • Received 4 November 1991

DOI:https://doi.org/10.1103/PhysRevB.45.9272

©1992 American Physical Society

Authors & Affiliations

D. L. Abernathy and S. G. J. Mochrie

  • Research Laboratory of Electronics and Department of Physics, Massachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307

D. M. Zehner

  • Solid State Division, Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831-6057

G. Grübel and Doon Gibbs

  • Department of Physics, Brookhaven National Laboratory, Upton, New York 11973-5000

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Vol. 45, Iss. 16 — 15 April 1992

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