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October 29, 2003

Investigating a Surface Science Mystery: The Case of the Disappearing Monolayer

K.S. Schneider1, T.M. Owens1, D.R. Fosnacht1, B.G. Orr2,3, and M.M. Banaszak Holl1,3
1Chemistry Department, The University of Michigan, Ann Arbor, MI; 2Physics Department and the 3Applied Physics Program, Harrison M. Randall Laboratory, The University of Michigan, Ann Arbor, MI

A recent X-ray photoemission spectroscopy (XPS) and scanning tunneling microscopy (STM) investigation of an alkylsilane-based monolayer has yielded intriguing chemical and physical phenomena. In particular, oxidation of an octylsilane (C8H17SiH3) monolayer chemisorbed to Au(111) via ambient atmosphere exposure yields two surprising results. First, the Au(111)-23×√3 surface reconstruction typical of a clean gold surface spontaneously regenerates underneath the oxidized (alkylsiloxane) monolayer. Furthermore, the physisorbed alkylsiloxane monolayer is completely transparent to STM imaging.

Frequently, the STM image contrast mechanism of organized organics—such as alkanethiols—on Au(111) is explained as a consequence of hydrocarbon chain crystallization and/or variations in chain angle or orientation. Similarly, subtle variations in alkyl chain angle or orientation may yield differing apparent heights of alkylsilane monolayer features as observed by STM. However, a recent XPS and STM investigation of an alkylsilane monolayer prior to and following oxidation suggests the alkyl chains are “transparent” to STM imaging and impart a negligible contrast contribution to the STM images.

A STM image of clean Au(111) displays the parallel striped features intrinsic to the 23×√3 surface reconstruction (Figure 1a). Monolayer formation via the exposure of Au(111)-23×√3 to a saturating gaseous pressure of octylsilane (C8H17SiH3) in ultrahigh vacuum (UHV) yields a complex pattern of interwoven, sinuous ridge features containing numerous interstitial Au islands 20 – 40 Å in diameter (Figure 1b). The presence and quantity of the Au islands (~7% areal coverage in Figure 1b) indicates the underlying 23×√3 surface reconstruction has fully relaxed to the unreconstructed Au(111)-1×1 phase.

Oxidation of the octylsilane monolayer via ambient atmosphere exposure results in the disappearance of monolayer features from the STM image (Figure 1c). The resulting substrate terraces are indistinguishable from clean Au(111)-23×√3 (having identical lateral and vertical dimensions) under the imaging conditions employed. STM image features of the exposed monolayer do not vary with changes in tunneling current (0.01 – 2 nA) or applied sample bias (± 2 V). However, exposure to additional octylsilane does not regenerate the image shown in Figure 1b. Instead, an image identical to clean Au(111)-23×√3 remains (Figure 1d). Therefore, the “clean gold” surface displayed in Figure 1c does not have identical chemical properties of the authentic clean gold surface illustrated in Figure 1a. On the basis of STM data alone, this set of results was mysterious!

Direct chemical analysis of oxidized sample surfaces has been performed using soft X-ray photoemission spectroscopy (SXPS) at beamline U8B at the National Synchrotron Light Source at Brookhaven National Laboratory. Beamline U8B is perfectly suited to obtaining the high-resolution Si 2p core-level needed for this study as well as the valence band region. Note that due to the presence of an Au plasmon trailing the Au 4f core level, conventional XPS of the Si 2p core-level for these monolayers provides no information. Following exposure to ambient atmosphere, the Si 2p core level of the unoxidized octylsilane monolayer (Figure 2a) shifts by 2.3 eV to higher binding energy and the peak full width at half-maximum (fwhm) increases (Figure 2b). The binding energy shift and peak broadening indicate formation of a cross-linked RSiO3 and/or (ROSiO1.5)n network. The C 2s features arising from the octyl chain are retained in the valence band data (-12 to -20 eV), indicating the presence of intact alkyl chains in the oxidized monolayer (Figure 2d). In summary, the XPS data indicate that exposure to ambient atmosphere effectively oxidizes the silicon head-groups; however, all of the silicon and alkyl chains are retained within the oxidized monolayer. Thus, the STM image displayed in Figure 1c does indeed have the monolayer present, albeit it in an oxidized form.

The combination of SXPS and STM data suggest the original octylsilane monolayer image in Figure 1b is the result of significant mixing of Au and Si states. Oxidation of the Si head-groups removes this interaction, causing the underlying substrate to regenerate the Au(111)-23×√3 surface reconstruction, and leaving only the Au states to image. In this case, the alkyl chains are “transparent” in both Figures 1b and 1c and it is only the Au-Si interaction that changes upon oxidation. Since monolayer oxidation severs all Au-Si bonds, a completely “transparent” physisorbed alkylsiloxane layer remains on top of the reconstructed Au(111)-23×√3 surface.

BEAMLINE
U8B

FUNDING
National Science Foundation
RHK Technology, Inc.
Division of Materials Sciences and Division of Chemical Sciences, U.S. Department of Energy.

PUBLICATION
Kevin S. Schneider, Thomas M. Owens, Daniel R. Fosnacht, Bradford G. Orr, and Mark M. Banaszak Holl, “The Case of the Disappearing Monolayer: Alkylsilane Monolayer Formation, Oxidation, and Subsequent Transparency to Scanning Tunneling Microscopy,” ChemPhysChem, 4, 111-1114, (2003).

FOR MORE INFORMATION
Mark M. Banaszak Holl
Chemistry Department and Applied Physics Program
University of Michigan, Ann Arbor, MI
Email: mbanasza@umich.edu