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Introduction to Nanotechnology

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154 BULK NANOSTRUCTURED MATERIALS<br />

Figure 6.22. The icosohedral structure of a boron cluster containing 12 a<strong>to</strong>ms. This cluster is<br />

the basic unit of a number of boron lattices.<br />

6.2.3. Arrays of Nanoparticles in Zeolites<br />

Another approach that has enabled the formation of latticelike structures of nano-<br />

particles is <strong>to</strong> incorporate them in<strong>to</strong> zeolites. Zeolites such as the cubic mineral,<br />

faujasite, (Na2,Ca)(A12Si4)OI2. 8H20, are porous materials in which the pores have<br />

a regular arrangement in space. The pores are large enough <strong>to</strong> accommodate small<br />

clusters. The clusters are stabilized in the pores by weak van der Waals interactions<br />

between the cluster and the zeolite. Figure 6.24 shows a schematic of a cluster<br />

assembly in a zeolite. The pores are filled by injection of the guest material in the<br />

molten state. It is possible <strong>to</strong> make lower-dimensional nanostructured solids by this<br />

approach using a zeolite material such as mordenite, which has the structure<br />

illustrated in Fig. 6.25. The mordenite has long parallel channels running through<br />

it with a diameter of 0.6nm. Selenium can be incorporated in<strong>to</strong> these channels,<br />

forming chains of single a<strong>to</strong>ms. A trigonal crystal of selenium also has parallel<br />

chains, but the chains are sufficiently close <strong>to</strong>gether so that there is an interaction<br />

between them. In the mordenite this interaction is reduced significantly, and the<br />

electronic structure is different from that of a selenium crystal. This causes the<br />

optical absorption spectra of the selenium crystal and the selenium in mordenite <strong>to</strong><br />

differ in the manner shown in Fig. 6.26.

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