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Introduction to Nanotechnology

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162 BULK NANOSTRUCTURED MATERIALS<br />

0<br />

Z 0.4 ~ T PHOTONIC M BAND GAP:<br />

3<br />

$ 0.3 1 -<br />

Figure 6.31. A part of the dispersion relationship of a pho<strong>to</strong>nic crystal mode, Th., of a pho<strong>to</strong>nic<br />

crystal made of a square lattice of alumina rods. The ordinate scale is the frequency f multiplied<br />

by the lattice parameter a divided by the speed of light c. [Adapted from J. D. Joannopoulos,<br />

Nature 386, 143 (1 997).]<br />

power is intense below this band gap, and in analogy with the terms conduction band<br />

and valence band, this region is called the dielectric band. Above the forbidden gap<br />

the light power is low, and the region there is referred <strong>to</strong> as the “air band.”<br />

Now let us consider what would happen if a line defect were introduced in<strong>to</strong> the<br />

lattice by removing a row of rods. The region where the rods have been removed<br />

would act like a wave guide, and there would now be an allowed frequency in the<br />

band gap, as shown in Fig. 6.32. This is analogous <strong>to</strong> p and n doping of<br />

0.5<br />

c-<br />

1 1 1 1 1 1 1 1 1 1 1 I l l , I I I l l , , I<br />

0 0.1 0.2 0.3 0.4 0.5<br />

WAVEVECTOR (Ka/2n)<br />

Figure 6.32. Effect of removing one row of rods from a square lattice of a pho<strong>to</strong>nic crystal, which<br />

introduces a level (guided mode) in the forbidden gap. The ordinate scale is the frequency f<br />

multiplied by the lattice parameter a divided by the speed of light c. [Adapted from<br />

J. D. Joannopoulos, Nature 386, 143 (1997).]

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