Abstract

Brewster angle microscopy (BAM), x-ray specular reflectivity and grazing-incidence x-ray diffraction (GID) studies of C60-propylamine adduct monolayers at the gas/water interface as a function of molecular area are reported. At large molecular areas (A>∼150 Å2/molecule), BAM images reveal macroscopic heterogeneity in the film, consisting of the coexistence between regions covered with uniform solidlike monolayer and bare water surface. After compression to a limiting molecular area of 150 Å2/molecule, the film is observed to be homogeneous, with the uniform monolayer covering the entire available surface. Both the x-ray reflectivity results and the GID patterns are consistent with the formation of a uniform monolayer at A∼150 Å2/molecule, while the little dependence that the GID patterns have on the molecular area for A>∼150 Å2/molecule is consistent with the heterogeneity in the film. Upon further compression to higher densities (A<∼120 Å2/molecule), the x-ray reflectivity results suggest the formation of a partial layer either at the molecule/gas interface or at the molecule/water interface. In this high density regime, the shift in the observed GID pattern with molecular area is much smaller than would be expected if the film were to remain a homogeneous monolayer, also consistent with the formation of an inhomogeneous partial layer. The analysis of the broad GID pattern observed from a uniform monolayer in terms of a model 2D radial distribution function, implies a short range positional correlation, extending to only a few molecular distances. The average nearest neighbor distance (d∼13 Å), extracted from the GID analysis, is consistent with the limiting molecular area (A∼150 Å2/molecule) assuming local hexagonal packing. These results together with the sharp facets observed in the BAM images demonstrate that the monolayer when uniform is a two-dimensional amorphous solid.

Highlights

  • One of the principal motivations behind many modern theoretical, computational, and experimental studies of surface and interfacial phenomena is to understand the effects of physical dimension on statistical physics

  • A principal challenge in this general area of physics has been to identify real, well defined physical systems that are suitable for experimental studies

  • We present here a combination of optical and x-ray scattering studies of a Langmuir monolayerLMof fullerenepropylamine adductabbreviated as C60-PAmolecules,52 which consists of a C60 molecule and twelve propylamineNH2͑CH2͒2CH3͔ chains attached to it

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Summary

INTRODUCTION

One of the principal motivations behind many modern theoretical, computational, and experimental studies of surface and interfacial phenomena is to understand the effects of physical dimension on statistical physics. A principal challenge in this general area of physics has been to identify real, well defined physical systems that are suitable for experimental studies. There are the numerous studies of the phase transitions and quasi-long-range correlations of thin films of various smectic liquid crystals.7,47,48,50,51 These are amongst the more important measurements of the structural correlations for 2D statistical systems; only the very thinnest films are strictly two dimensional. We will show that the LM monolayer of C60PA, both as-deposited and at low pressures, is a relatively incompressible solid that is either a two-dimensional amorphous glass or a two-dimensional microcrystalline solid This is in itself an interesting observation, even more important is that it demonstrates that if other fullerene derivatives that form liquid, rather than solid, Langmuir monolayers could be developed, x-ray scattering studies of both two-dimensional solidification and vaporization would be practical. IV, and the main conclusions from the analysis in the preceding section are highlighted

X-ray techniques
Langmuir trough
RESULTS AND DISCUSSION
Surface imaging by BAM
X-ray reflectivity
GID and rod scans
Application of the spherical model to the fitting of reflectivity data
SUMMARY
Full Text
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