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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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Figure 29 Transmission electron micrographs and electron diffraction (ED)patterns for CdSe NQD superlattices (SLs) of different orientations: (a) Main:h111i SL -oriented array of 6.4-nm-diameter NQDs five layers thick; upper right: HR-TEM of a single NQD with its h110i axis parallel to the electron beam and its h002iaxis in the plane of the SL; lower right: small-angle ED pattern. (b) Main: facecentered-cubic(fcc) array of 4.8-nm-diameter NQDs (h101i SL projection); lowerright: small-angle ED pattern. (c) Main: fcc array of 4.8-nm-diameter NQDs (h100i SLoriented); lower right: small-angle ED pattern. (From Ref. 90, reprinted withpermission.)The process is similar for particles ranging in size from cluster molecules tomicron-sized colloidal particles [8]. It entails controlled destabilization andprecipitation from a slowly evaporating solvent (Fig. 30). As the solutionconcentrates, interactions between particles become mildly attractive. Particleassociation is sufficiently slow, however, to prevent disordered aggregation.Instead, ordered assembly dominates <strong>by</strong> a reversible process of particleaddition to the growing superlattice [10]. Fully formed ordered solids arecommonly called colloidal crystals (Fig. 31), where the cluster, NQD, orcolloid serves as the ‘‘artificial atom’’ building block. In the case of NQDs, theprocess is controlled <strong>by</strong> manipulating the polarity and the boiling point of thesolvent [10]. The solvent polarity is chosen to ensure that mild attractiveforces develop between the nanoparticles as the solvent evaporates. Theboiling point is chosen to ensure that the evaporation process is sufficientlyslow [10]. At the other extreme of very fast destabilization, <strong>by</strong> fast solventevaporation or nonsolvent addition, a rapid increase in the ‘‘sticking coefficient’’(particle attraction) and in the rate at which particles are added to thegrowing surface yields loosely associated fractal aggregates. Moderate destabilizationrates, implemented <strong>by</strong> using ‘‘moderate-boiling’’ solvents, produceclose-packed glassy solids having local order but lacking long-range order(Fig. 30a) [8]. For assembly of well-ordered NQD superlattices, the chosensolvent is typically a mixed solvent, involving both a lower-boiling alkane anda higher-boiling alcohol. The alkane evaporates more quickly than thealcohol, yielding relatively higher concentrations of the ‘‘destabilizing’’<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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