Layering transitions in colloidal crystals as observed by diffraction and direct-lattice imaging.
Layering transitions in colloidal crystals as observed by diffraction and direct-lattice imaging.
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通过衍射和直接晶格成像观察胶体晶体中的层状转变。
DOI:
10.1103/physreva.34.562
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发表时间:
1986
期刊:
影响因子:
--
通讯作者:
C. A. Murray
中科院分区:
文献类型:
--
作者:
D. H. Winkle;C. A. Murray
Layering transitions of colloidal crystals confined between two smooth glass surfaces have been studied by transmission diffraction of light as well as direct-lattice imaging with an optical microscope. The polystyrene spheres we studied have diameter Φ= 0.305 μm and a surface charge of∼ 10 4 electronic charges, and form three-dimensional (3D) colloidal crystals in completely deionized water at a volume concentration above≊ 0.3%. A 3D suspension of these spheres in completely deionized water forms both body-centered-cubic (bcc) and face-centered-cubic (fcc) crystalline structures as a function of colloid density n≡(1/a s) 3, with lattice constants ranging between 0.7 and 1.5 μm. When the colloid is confined between glass plates separated by distances D∼ 0.5–1 μm, the spheres form a single-layer 2D fluid. For D near 1 μm, a transition occurs to a single-layer 2D hexagonal crystal. As D increases, the evolution from two-to three-dimensional crystals is observed as a series of structural transitions distinguished by the number of crystal planes between the plates and by the preferred crystal symmetry parallel to the glass boundaries. We present here a study of colloidal crystals confined in a wedge cell that allows diffraction and imaging from the same crystallite. We present diffraction and imaging measurements of structural phases of one-through seven-layer colloidal crystals confined between two smooth glass surfaces, for a range of densities such that 2< a s/Φ< 6. The sequence of structural phases we observe for this range of densities for clean samples is similar but not identical to that observed for a s/Φ< 2 by Pieranski, Strzlecki, and Pansu, which was modeled as a hard-sphere system. We also observe differences between the clean thin crystalline phases and ‘‘dirtier’’thin phases to which a stray electrolyte has been added. The use of both diffraction and imaging was found necessary to fully characterize the system.