Long Chain n-Alkanes at SiO₂/Air Interfaces:  Molecular Ordering, Annealing, and Surface Freezing of Triacontane in the Case of Excess and Submonolayer Coverage

Abstract

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

Nanoscale observation of delayering in alkane films

“…These changes indicate a transition in the film from the orthorhombic structure described above to a phase characterized by a higher symmetry (probably a hexagonal structure) and much a shorter coherence length than in the lowtemperature C phase. Following previous suggestions of a rotator phase for interfacial alkane molecules of intermediate length [9,10], we interpret the changes in the X-ray scans in the range 56-58…”

Crystalline-to-plastic phase transitions in molecularly thin n-dotriacontane films adsorbed on solid surfaces

“…12 On top of this bilayer, molecules with their long axis perpendicular to the surface coexist with monoclinic and orthorhombic bulk particles. 13,14 The mesa-shaped orthorhombic particles are surrounded by an area depleted of perpendicular layers. 4,15 Moreover, Bai et al 4 have recently shown that thin films of intermediate-length alkanes do not completely wet SiO 2 surfaces.…”

“…Schollmeyer et al 13 conducted a comprehensive study of triacontane ͑n-C 30 H 62 or C30͒ films grown by spin coating on solid substrates. From their x-ray diffraction measurements, they found that some of their thin films had a different number of solid phases than the bulk material and suggested that these additional phases were stabilized by interfacial interactions.…”

Atomic force microscopy measurements of topography and friction on dotriacontane films adsorbed on a SiO2 surface

“…Riegler and co-workers [5][6][7][8] have proposed that a similar surface freezing effect can occur with intermediate-length alkane molecules if air is replaced by a solid substrate ͑SiO 2 ͒. In their model of a thick alkane film, a crystalline monolayer of perpendicularly oriented alkane molecules adsorbs immediately adjacent to the SiO 2 surface.…”