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handbook of carbon, graphite, diamond and fullerenes

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266 Carbon, Graphite, Diamond, <strong>and</strong> Fullerenes<br />

Effect <strong>of</strong> Impurities <strong>and</strong> Structural Defects. As seen above,<br />

<strong>diamond</strong> would be the ideal transparent material if it were totally free <strong>of</strong><br />

impurities, particularly nitrogen, <strong>and</strong> had a perfect structure. Howeverthese<br />

conditions are never completely achieved, <strong>and</strong> impurities <strong>and</strong> crystal-lattice<br />

defects <strong>and</strong> other obstacles to the free movement <strong>of</strong> photons affect its<br />

transmittance. These obstacles add a number <strong>of</strong> absorption b<strong>and</strong>s to the<br />

two mentioned above, particularly in the IR region as shown in Table 11.4.<br />

In spite <strong>of</strong> this, <strong>diamond</strong> remains the best optical material.<br />

Lattice vacancies (missing atoms) may considerably alter the valence<br />

bonds <strong>and</strong> cause electrons to be exited by a much smaller amount <strong>of</strong> energy<br />

(such as produced by a photon <strong>of</strong> red light) that would normally be required<br />

in a perfect lattice. A <strong>diamond</strong> containing such lattice vacancies appears<br />

blue since the red components <strong>of</strong> light (the one with less photon energy) are<br />

absorbed. A minimum <strong>of</strong> one vacancy per 10 5 atoms is necessary for the<br />

blue color to be noticeable.! 11 )<br />

Table 11.4. Optical Absorption <strong>of</strong> Diamond by Type<br />

Type Optical absorption b<strong>and</strong>s<br />

la IR: 6-13 microns<br />

UV:

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