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The crystallization [HN1] of matter on any length scale, from atoms and ions to biomolecules to nano- and microparticles, has long been a major thrust in science and technology. On page 420 of this issue, Kalsin et al.[HN2] (1) report the cocrystallization of equally sized metallic nanoparticles into large crystals with diamond-like symmetry [HN3]. The oppositely charged gold and silver nanoparticles attract each other at very short distances and assemble into unusual lattices [HN4]. This work provides new insights into crystallization on the nanoscale, and fills in a gap in the overall picture of particle and biomolecule crystallization.
It has been known for decades that micrometer- and submicrometer-sized spheres suspended in liquids readily form "colloidal crystals" [HN5] during sedimentation or drying. The spheres crystallize when their free volume is restricted below a certain threshold, but this occurs only when the interactions between the spheres are repulsive, which allows their rearrangement. Such closely packed crystals allow facile fabrication of materials with controlled porosity and long-range organization (2). Volume-restricted repulsive spheres, however, always crystallize in a trivial lattice of hexagonally close-packed layers [HN6]. This limits the range of their application as other types of crystal symmetries are required for photonic, optoelectronic, and memory storage applications.
The formation of colloid crystals with other symmetries can, in principle, be achieved if the particles are assembled by attractive interactions. Two seemingly simple ideas for crystallization by particle attraction have been considered, yet they have proven notoriously difficult to realize experimentally. The first idea is to use binary mixtures of oppositely charged particles that could cocrystallize in a manner broadly similar to crystallization of ionic salts from liquid solutions. The problem with this system is that strongly attractive particles rapidly and irreversibly stick to each other, forming gel-like aggregates. Only recently have Leunissen et al.[HN7] designed a procedure whereby micrometer-sized colloidal spheres having small positive or negative charges are synthesized and cocrystallized in density-matched organic liquids (3). The particles, whose attractive interaction energies are estimated to be on the order of a few kBT units (where kB is Boltzmann's constant and T is temperature), come together in mixed CsCl-type lattices [HN8] of alternating positive and negative charges. A variety of crystals of other symmetries and particle compositions have been assembled, and the method could be versatile enough to be used in the routine synthesis of ionic colloidal crystals.
A second idea for particle crystallization by attractive interactions that has also proven difficult to realize is the crystallization of particles by functionalizing them with complementary DNA strands. DNA hybridization locks the particles together when they come into contact; however, the strong irreversible "snapping" into place does not allow crystallization. The key to making this idea work has been to reduce the strength of the interactions by adjusting the temperature of the suspension very near the melting point of DNA, where hybridization is weak and reversible (4) [HN9]. Thus, colloidal crystallization may be achieved by various attractive forces, but only when the interaction energy is precisely adjusted within a certain small range (see the figure).
Systems of nanoparticles 1 to 10 nm in size provide a natural link between the areas of molecular and colloidal crystallization. Crystals from such particles can find applications in nanoelectronics, plasmonics, high-density data storage, catalysis, and biomedical materials. The formation of binary crystals from nanoparticle mixtures as a likely result of cocrystallization under restricted volume conditions was reported some time ago (5). Only recently has the role of electrostatics in the formation of nanoparticle crystals emerged as a parameter that can be controlled in order to assemble various crystals of new symmetry and composition (6) [HN10]. The report by Kalsin et al. conclusively proves that large crystals can be produced by controlled electrostatic self-assembly [HN11]. The crystallization has been achieved by precise adjustment of the attraction between the oppositely charged nanoparticles, but the data also point to the existence of unusual effects of electrostatic screening of the larger particles by the smaller ones that do not scale up to interactions between microspheres.
Packing together. The crystallization of colloidal particles and biomacromolecules is intrinsically related to the interactions between the particles, which often can be controlled by their charge (graph at left). Repulsive spheres can easily be crystallized by restricting their volume. Proteins and binary mixtures of oppositely charged particles can be crystallized by precise adjustment of the interactions into a weakly attractive regime. However, if the interactions between the particles are strongly attractive, rapid precipitation of amorphous aggregates occurs. The micrograph images are of colloidal crystals assembled by restricting the free volume of repulsive latex spheres (left), crystals of the protein lysozyme obtained under slightly attractive interactions (center), and a nanoparticle crystal assembled under controlled electrostatic attraction (1) (right).
CREDITS: O. VELEV
Interestingly, the idea that the key to crystallization is achieving a precise balance among weak attractive interactions has been actively explored in the field of protein crystallization [HN12] for more than a decade. Proteins are large, complex molecules of nonuniform shape and charge, which have been shown to crystallize only under conditions of slightly attractive interactions when both positively and negatively charged groups are present on their surfaces (7). The intricate fundamentals of the attractive electrostatic interactions between nanoparticles in a crystal are still not understood in depth. It seems that the concepts developed for proteins may now provide a roadmap for nanoparticle crystallization.
Future research in nanoparticle assembly may bring closer the areas of biomacromolecule and nanoparticle crystallization. Could a similar charge-balancing approach be applied to binary mixtures of proteins, or mixtures of proteins and nanoparticles? A large variety of nanoparticles of special shape and properties have been synthesized in the past few years, but little is yet known about their self-assembly [HN13]. New "zwitterionic" [HN14] particles, having patches of negative and positive charges on their surfaces, could soon be synthesized and crystallized by adjustment of the interactions in a manner similar to the crystallization of proteins. Thus, nanoparticle crystallization and assembly may not only yield new nanomaterials, but could also provide insights into how to control colloidal forces on the nanoscale.
References
A. M. Kalsin et al., Science312, 420 (2006); published online 23 February 2006 (10.1126/science.1125124).
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M. E. Leunissen et al., Nature437, 235 (2005) [CrossRef].
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E. V. Shevchenko, D. V. Talapin, N. A. Kotov, S. O'Brien, C. B. Murray, Nature439, 55 (2006) [CrossRef].
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10.1126/science.1125800
The author is in the Department of Chemical and Biomolecular Engineering, North Carolina State University, Raleigh, NC 27695-7905, USA. E-mail: odvelev{at}unity.ncsu.edu
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REPORTS
Alexander M. Kalsin, Marcin Fialkowski, Maciej Paszewski, Stoyan K. Smoukov, Kyle J. M. Bishop, and Bartosz A. Grzybowski (21 April 2006) Science312 (5772), 420.
[DOI: 10.1126/science.1125124] |Abstract »|Full Text »|PDF »|Supporting Online Material »
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