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Introduction to Nanotechnology

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6.2. NANOSTRUCTURED CRYSTALS 159<br />

repulsions the lattice structure is face-centered cubic. Increasing the range of the<br />

repulsion, or lowering the concentration, allows the formation of the slightly less<br />

compact body-centered structure. Figure 6.28 shows the phase diagram of a system<br />

of soft spherical particles. The excluded volume is the volume that is inaccessible <strong>to</strong><br />

one particle because of the presence of the other particles. By adjusting the fraction<br />

of particles, a structural phase transition between the face-centered and body-<br />

centered structures can be induced. The particles can also be modified <strong>to</strong> have<br />

attractive potentials. For the case of charged particles in aqueous solutions, this can<br />

be accomplished by adding an electrolyte <strong>to</strong> the solution. When this is done, abrupt<br />

aggregation occurs.<br />

6.2.6. Pho<strong>to</strong>nic Crystals<br />

A pho<strong>to</strong>nic crystal consists of a lattice of dielectric particles with separations on the<br />

order of the wavelength of visible light. Such crystals have interesting optical<br />

properties. Before discussing these properties, we will say a few words about the<br />

reflection of waves of electrons in ordinary metallic crystal lattices.<br />

The wavefunction of an electron in a metal can be written in the free-electron<br />

approximation as<br />

0.002 0.004 0.006 0.008 0.01<br />

VOLUME FRACTION<br />

(6.12)<br />

Figure 6.28. Phase diagram for soft spherical particles in suspension showing the fluid state,<br />

the body-centered cubic (BCC) and face-centered cubic (FCC) phases. The vertical axis<br />

(ordinate) represents the volume that is inaccessible <strong>to</strong> one particle because the presence of<br />

the others. The excluded volume has been scaled <strong>to</strong> the cube of the Debye screening length,<br />

which characterizes the range of the interaction. [Adapted from A. P. Gast and W. B. Russel,<br />

Phys. Today (Dec. 1998.)]

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