4.4 Article

Structure of an ultrathin TiOx film, formed by the strong metal support interaction (SMSI), on Pt nanocrystals on TiO2(110)

期刊

SURFACE SCIENCE
卷 492, 期 1-2, 页码 L677-L687

出版社

ELSEVIER SCIENCE BV
DOI: 10.1016/S0039-6028(01)01460-1

关键词

density functional calculations; insulating films; surface structure, morphology, roughness, and topography; surface stress; titanium oxide; metal-insulator interfaces; catalysis; platinum

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We use first-principles density functional theory to study ultrathin TiOx films on Pt(1 1 1). The preferred interface with Pt has Ti with O as an overlayer. However, this ordering, preferred over Ti/O/Pt by 2.9 eV/Ti-O unit, produces > 10% stress. This explains a complex structure, seen using STM, of TiOx bilayers encapsulating Pt(1 1 1) nanofacets: the energetics of stress relief is about ten times that of differences in the various possible O/Ti/Pt(1 1 1)-layer site occupations, thus favoring dislocation formation. A structure is found that is stable. It consists of a series of linear misfit dislocations at the relatively weak Ti/Pt interface that are 6/7 Ti/Pt rows wide. In addition, strong interactions at the O/Ti interface and O-layer strain also cause the Ti/Pt interface to abruptly change from hcp- to fee-site Ti, producing linear canyons (Ti/Pt dislocation cores occur between these stripes). Furthermore, alternating hcp- and fcc-site triangles, each with ten O-atoms, are separated by bridging O in an abrupt O/Ti misfit dislocation, thus producing a zigzag pattern. The above dislocations release strain along both the x- and y-directions in the surface plane. However, we have been unable to find a stable structure if the zigzag ends consist of O, but stability is found if they consist of Ti. Finally, reverse bias STM images indicate the ends might indeed different than the line portions of the zigzag features. (C) 2001 Published by Elsevier Science B.V.

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