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We report on a novel technique to nucleate nanometer-sized droplets on a solid substrate and to image them with minimal perturbation by noncontact atomic force microscopy (NC-AFM). The drop size can be accurately controlled, thus permitting hysteresis measurements. We have studied the nanoscale wettability of several methyl-terminated substrates prepared by the self-assembly of organic molecules. These substrates are alkyltrichlorosilanes on silica, alkylthiols on gold, alkyl chains on hydrogen-terminated silicon, and crystalline hexatriacontane chains on silica. For each of these systems, we report a deviation of the wetting contact angle from the macroscopic value, and we discuss this effect in term of mesoscale surface heterogeneity and long-range solid-liquid interactions.

Long-chain n alkanes on solid surfaces can form partially wetting liquid alkane droplets coexisting with solid multilayer terraces. We propose a diffusivelike alkane flow between terrace edge and droplet perimeter through a molecularly thin "precursorlike" film. Depending on the (uniform!) sample temperature, either droplet or terrace edge are not in thermodynamic equilibrium. This leads to a chemical potential gradient, which drives the reversible alkane flow. The gradient can be adjusted and calculated independently from the phenomenological diffusion coefficient.

We present a comprehensive study on the interfacial molecular ordering of an n-alkane, triacontane, at the SiO2/air interface, for submonolayer and excess coverage. The molecular ordering was studied by X-ray diffraction and reflectivity at temperatures from far below bulk melting to above the surface freezing temperature. It is found that the phase behavior of bulk and that of interfacial triacontane are quite different. From the literature it is known that bulk triacontane has three solid phases: one crystalline phase (monoclinic) and two rotator phases (RIII and RIV) with solid/solid transitions at ≈61 °C and close to the melting point into the liquid phase (≈67 °C), respectively. All solid bulk phases have inclined molecules. We show that interfacial triacontane has only two ordered solid phases: a crystalline phase (orthorhombic) and a rotator phase. In both phases the molecules are oriented normal to the interface. At the interface, the temperature of the transition from the crystalline phase to the rotator phase can be as low as 40 °C. For both submonolayer and excess coverage, the interfacial rotator phase can persist up to ≈70 °C. This means that above 67 °C, for excess coverage, the solid rotator phase coexists with liquid bulk triacontane ("surface freezing"). The different phase behavior in bulk and at the interface is explained with different interlayer interactions. We also find that, directly after solidification, the interfacial layer is usually in a highly amorphous, nonequilibrium state. This we attribute to rapid solidification because of the efficient cooling at the interface. Depending on thermal treatment and time, the interfacial layer can anneal to various degrees of molecular ordering, which is reflected in the phase behavior. LA026989F