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Copyright 2004 by Marcel Dekker, Inc. All Rights Reserved.

Copyright 2004 by Marcel Dekker, Inc. All Rights Reserved.

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of the stabilizing ligand, and the steric interactions between particles.Polydisperse nanocrystals (r typically >10%) do not form superlattices[13,34] and the coordination number is lower than in close-packed orderedsolids because long-range order does not exist. The radial distributionfunctions, however, for these films exhibit regular oscillations characteristicof the average particle diameter and interparticle separation, as in the case formolecular liquids [13]. Scattering from these dense fluids has enabled thecalculation of pair interparticle potentials in the absence of solvent withreasonable accuracy [13]. Monodisperse nanocrystals form lattices that giverise to sharp diffraction peaks. These peaks are readily indexed to determinethe superlattice crystal structure and lattice parameters [9,13].III.SUPERLATTICE FORMATIONNanocrystal superlattices require size-monodisperse nanocrystals that arewell stabilized <strong>by</strong> organic capping ligands. Although this is a necessarycondition for superlattice formation, it is not sufficient. The formation processis also extremely important in determining the dimensionality and the extentof order. Superlattices have been formed <strong>by</strong> essentially two different approaches:(1) Langmuir–Blodgett processing in which the density of thenanocrystal dispersion is carefully controlled through the disorder–orderphase transition in two dimensions [35] and (2) evaporative crystallization,which yields superlattices in either two or three dimensions [10,36].A. Two-Dimensional Order in Langmuir–BlodgettTechniquesNanocrystal dispersions can be drop cast onto liquid surfaces to form twodimensionalsuperlattices, or monolayers, at an air–liquid interface. Depositionon a Langmuir–Blodgett (LB) trough provides the ability to controlthe surface density of the nanocrystal layer <strong>by</strong> compressing the trough. Twodetailed studies have been reported for CdSe nanocrystals [37] and Agand Au nanocrystals [36]. Bawendi and co-workers [37] used monodisperseCdSe nanocrystals capped with triotylphosphine oxide with nanocrystals thatvaried in size from 25 to 53 A˚ in diameter. Surface pressure versus areaisotherms showed strong hysteresis, indicating attractive interactions betweenthe nanocrystals in the rigid monolayer. TEM analysis of films transferredonto glass substrates and carbon-coated TEM grids showed short-range translationalorder and long-range nearest-neighbor orientational order—characteristics of a hexatic phase. It was also determined that the lack oflong-range translational order was caused <strong>by</strong> dislocation defects, not the<strong>Copyright</strong> <strong>2004</strong> <strong>by</strong> <strong>Marcel</strong> <strong>Dekker</strong>, <strong>Inc</strong>. <strong>All</strong> <strong>Rights</strong> <strong>Reserved</strong>.

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