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Faceting and Commensurability in Crystal Structures of Colloidal Thin Films - Notes

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Published abstract

This Letter investigates the influence of finite size effects on the particle arrangement of thin film colloidal crystals. A rich variety of crystallographic faceting with large single domain microcrystallites is shown. Optical reflectance experiments together with scanning electron microscopy permit the identification of the crystal symmetry and the facet orientation, as well as the exact number of monolayers. When the cell thickness is not commensurable with a high symmetry layering, particles arrange themselves in a periodic distribution of (111)- and (100)-orientated face centered cubic (fcc) microcrystallites separated by planar defects. These structures can be described as a fcc ordering orientated along a vicinal surface, modified by a periodic distribution of fcc (111) stacking faults.

Figures

Complete Figure 1 composition with reflectance spectra and SEM panels
Figure 1. Summary. Successive reflectance spectra and scanning electron micrographs follow a confined colloidal film as its thickness increases from seven to eight monolayers. The structure evolves continuously from a (100)-oriented face-centred-cubic prismatic arrangement, through progressively finer faceted domains and additional interfacial rows, to long-range (111)-oriented face-centred-cubic order. The displacement of the Bragg feature provides the optical signature of the structural sequence seen in the micrographs.

Source: F. Ramiro-Manzano et al., Phys. Rev. Lett. 97, 028304 (2006); reproduced on an author's personal website.

Complete Figure 2 composition with reflectance spectra and SEM panels
Figure 2. Summary. For a colloidal film near nine monolayers, the paired spectra and micrographs trace the transition from long-range (111)-oriented face-centred-cubic order to a (100)-oriented hexagonal-close-packed facet. Intermediate states contain progressively smaller face-centred-cubic microcrystallites separated by line defects, while the Bragg peak shifts to longer wavelength as the local thickness increases. Together, the optical and structural data show that the change proceeds through stacking faults rather than an abrupt reconstruction.

Source: F. Ramiro-Manzano et al., Phys. Rev. Lett. 97, 028304 (2006); reproduced on an author's personal website.

Complete Figure 3 composition with vicinal fcc model and SEM panels
Figure 3. Summary. (a) Top and side views of a vicinal fcc (100) crystal ordering. Models (b) and (c) show how the system produces stacking faults planes to maximize filling fraction.

Source: F. Ramiro-Manzano et al., Phys. Rev. Lett. 97, 028304 (2006); reproduced on an author's personal website.

Complete Figure 4 composition with vicinal fcc model and SEM panels
Figure 4. Summary. (a) Top and side views of a vicinal fcc (111) crystal ordering. (b-d): Side views of the prismatic (111) phases.

Source: F. Ramiro-Manzano et al., Phys. Rev. Lett. 97, 028304 (2006); reproduced on an author's personal website.

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Research fields

Bottom-up

Colloidal spheres assemble under wedge confinement into films whose preferred orientation changes with layer number. When the gap is incommensurate with an ideal facet, the crystal introduces prismatic domains, terraces and periodic stacking faults to preserve dense packing.

Simulations & fits

Geometrical models and filling-fraction arguments reconstruct the fcc(100), fcc(111) and intermediate prismatic arrangements. They explain how the number and spacing of stacking faults evolve as the cell thickness moves between commensurate states.

Characterization

Position-dependent reflectance spectra are matched with top and cleaved-edge SEM images. This correlation assigns each spectral region to a three-dimensional facet and distinguishes a true structural transition from a gradual optical shift caused only by thickness.