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Prospects of Colloidal Nanocrystals for Electronic - Computer Science

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396 Chemical Reviews, 2010, Vol. 110, No. 1 Talapin et al.<br />

lasing 16 applications. The confinement regime can depend<br />

on the diameter <strong>of</strong> the core and thickness <strong>of</strong> the shell. For<br />

example, ZnSe/CdSe core-shell nanoparticles can exhibit<br />

either type-I or type-II behavior, depending on CdSe shell<br />

thickness. 165,169 If core and shell materials have a difference<br />

in lattice parameters (i.e., lattice mismatch) larger than a few<br />

percent, the addition <strong>of</strong> an intermediate “wetting” layer helps<br />

to relax the interfacial strain and prevent accumulation <strong>of</strong><br />

structural defects at the interface. 11,170<br />

The seeded growth can be used to fabricate a large variety<br />

<strong>of</strong> core-shell structures, including some very unusual<br />

material combinations such as Co/CdSe, 160 FePt/CdSe, 172<br />

PtFe/CdS 172 magnetic core-semiconductor shell, or Au/PbS<br />

plasmonic core-semiconductor shell 24 (Figure 6c). Depending<br />

on the interfacial energy, lattice matching, and the<br />

reaction conditions, multicomponent nanostructures can range<br />

from uni<strong>for</strong>mly covered core-shells to dumbbells (Figure<br />

6d) and even highly anisotropic heterostructures like tetrapods<br />

shown in Figure 6b.<br />

The use <strong>of</strong> seeds other than spherical nanoparticle, such<br />

as nanorods and tetrapods, may result in highly anisotropic<br />

structures where the new phase is selectively deposited on<br />

the tips <strong>of</strong> nanorods or tetrapod arms. Thus, PbSe/CdSe/<br />

PbSe, 173 CdTe/CdSe/CdTe, 35 and metal-semiconductor-metal<br />

Au/CdSe/Au heterostructures 38 (Figure 6e) were synthesized<br />

from CdSe nanorods.<br />

Robinson et al. used partial exchange <strong>of</strong> Cd 2+ ions in CdS<br />

nanorods with Ag + via cation exchange reaction 175 to prepare<br />

beautiful periodic CdS/Ag2S nanoheterostructures (Figure 6f).<br />

This approach is considered as a promising route to create<br />

modulated structures, interesting <strong>for</strong> thermoelectronic applications.<br />

Among other examples <strong>of</strong> multicomponent nanostructures,<br />

Au/PbS, 24 CoPt3/Au dumbbells, 174 PbSe/Aux, 176<br />

gold/iron oxide dumbbells, 177 solid core-shell 178 and<br />

core-hollow shell structures, 32 TiO2/Fe2O3, 179 PtFe/iron<br />

oxide, 180 and ZnO/Ag, 181 and many others have been reported<br />

during the last several years. The recent advances in the<br />

synthesis <strong>of</strong> hybrid structures were reviewed by Cozzoli et<br />

al. 37 and Zeng et al. 36<br />

The toolbox <strong>of</strong> synthetic techniques is quickly expanding,<br />

and many novel structures are reported every year. No doubt,<br />

this progress will further continue, providing scientists and<br />

engineers with novel potential functional building blocks <strong>for</strong><br />

electronics and optoelectronics.<br />

3. Nanocrystal Solids<br />

When considering chemically synthesized nanoparticles<br />

<strong>for</strong> electronic and optoelectronic applications, we should keep<br />

in mind that the actual active element <strong>of</strong> most devices will<br />

be not individual nanoparticles but their macroscopic arrays.<br />

In analogy with conventional solids, the assemblies <strong>of</strong><br />

nanoparticles should conduct charge carriers and per<strong>for</strong>m<br />

other useful actions such as light absorption and carrier<br />

separation in solar cells, light emission in LEDs, etc. The<br />

ability to tailor size, shape, and compositions <strong>of</strong> individual<br />

nanoparticles provides means <strong>for</strong> fine-tuning material properties.<br />

At the same time, the behavior <strong>of</strong> nanoparticle ensembles<br />

depends not only on the properties <strong>of</strong> individual elements,<br />

but on the electronic and optical communication between<br />

the nanoparticles, on the interparticle medium, packing<br />

density, and mutual orientations <strong>of</strong> NCs, etc. All <strong>of</strong> these<br />

issues add new levels <strong>of</strong> complexity to the problem <strong>of</strong><br />

designing electronic materials from nanoparticle building<br />

blocks. At the same time, understanding and utilizing self-<br />

Figure 7. (a) High-resolution cross-section SEM image <strong>of</strong> a dropcast<br />

film assembled from PbSe nanocrystals. Thickness <strong>of</strong> SiO2<br />

layer is 100 nm. Reprinted with permission from ref 23. Copyright<br />

2005 American Association <strong>for</strong> Advancement <strong>of</strong> <strong>Science</strong>. (b) SEM<br />

micrographs <strong>of</strong> a glassy solid prepared from 5.6 nm CdSe<br />

nanoparticles. Reprinted with permission from ref 39. Copyright<br />

2000 Annual Reviews.<br />

assembly <strong>of</strong> nanoparticles can provide routes to multifunctional<br />

materials <strong>of</strong> unprecedented precision, complexity, and<br />

aesthetic beauty. 182<br />

NCs can be brought together in a <strong>for</strong>m <strong>of</strong> an amorphous<br />

(glassy) or ordered periodic structures. Glassy NC solids can<br />

be defined as isotropic materials with only short-range order<br />

among the NCs (Figure 7). Several factors, such as polydispersity<br />

<strong>of</strong> NCs, their poor solubility in a given solvent,<br />

and fast solvent evaporation, favor the <strong>for</strong>mation <strong>of</strong> disordered<br />

structures or assemblies with short-range order (Figure<br />

7). Also, if repulsive <strong>for</strong>ces dominate the particle-particle<br />

interactions and other interactions are weak, there is no<br />

significant energy driving the <strong>for</strong>mation <strong>of</strong> an ordered<br />

lattice. 39<br />

Ordered NC solids (also referred to as “superlattices”) are<br />

anisotropic materials that are characterized by threedimensional<br />

periodicity with or without preferential orientation<br />

<strong>of</strong> individual nanoparticles. 39,183 In the case <strong>of</strong> periodic<br />

assemblies, the positions <strong>of</strong> particles and, as a result, packing<br />

density and chemical composition are uni<strong>for</strong>m throughout<br />

the entire structure. This uni<strong>for</strong>mity makes periodic nanoparticle<br />

arrays (films, 3D crystals) especially attractive <strong>for</strong><br />

practical applications and <strong>for</strong> fundamental studies. However,<br />

there are a number <strong>of</strong> technical challenges in reproducible<br />

preparation <strong>of</strong> large nanoparticle superlattices, such as lack<br />

<strong>of</strong> control over their dimensions and structural defects.

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