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Ion Scattering Study of the W(001)-(5x1)-C Surface

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The Structure of Surfaces II

Part of the book series: Springer Series in ((SSSUR,volume 11))

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Abstract

There have been several investigations of the surface of carburized W(100), and various models for its structure have been proposed. It is known that the surface exhibits a sequence of LEED patterns with increasing C coverage which can be indexed as p(1×1), c(2×2), c(3√2x√2)-R45° and p(5×1) [1,2,3]. Most authors agree that the c(2×2) and c(3√2 x √2)-R45° patterns are due to ordered C over layers with coverages near 1/2 and 2/3 mono layers, respectively. The p(5×1), accompanied by domains of p(1×5), can be formed by large exposures of ethylene at elevated temperature, and it is stable at temperatures up to 2000K and high pressures of hydrocarbon [1]. Because of this stability and the fact that heavily carburized polycrystalline W forms α-W2C, OLLIS and BOUDART [1] proposed that the p(5×1) LEED pattern is due to the formation of an over layer of α-W2C(0001). It was assumed that a coincidence occurs between the thin distorted hexagonal over layer and the W(001) substrate leading to the (5x1) pattern. BENZIGER et al. [2] accepted this structure but concluded from the lower than expected C Auger electron spectroscopy (AES) signal that the C must reside below the first W layer for the W(001)-(5×1)-C surface (Fig. 1, model 1). An alternate explanation offered by RAWLINGS et al. [3] was that the C is present above the surface, but at lower concentration than for a single (0001) layer of α-W2C. They proposed that the first W layer is reconstructed yielding a single layer of strained W(110) on top of W(001) (Fig. 1, model II). The first layer W atoms form the same coincidence mesh with respect to the W(001) substrate as in the case of the α-W2C (0001) layer. We have examined the structure of the carburized W(001) surface by incident angle dependent alkali ion scattering and find that the surface is not reconstructed to the quasi-hexagonal structure previously proposed. Instead, the p(5×1) LEED pattern is attributed principally to an ordered C over layer (Fig. 1, model III).

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References

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© 1988 Springer-Verlag Berlin Heidelberg

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Overbury, S.H., Mullins, D.R. (1988). Ion Scattering Study of the W(001)-(5x1)-C Surface. In: van der Veen, J.F., Van Hove, M.A. (eds) The Structure of Surfaces II. Springer Series in Surface Sciences , vol 11. Springer, Berlin, Heidelberg. https://doi.org/10.1007/978-3-642-73343-7_40

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  • DOI: https://doi.org/10.1007/978-3-642-73343-7_40

  • Publisher Name: Springer, Berlin, Heidelberg

  • Print ISBN: 978-3-642-73345-1

  • Online ISBN: 978-3-642-73343-7

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