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handbook of carbon, graphite, diamond and fullerenes

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CVD Diamond 329<br />

It should be noted that beryllia is being phased out because <strong>of</strong> the<br />

acute health problems associated with its use.<br />

Heat sinks in the form <strong>of</strong> thin slices prepared from single-crystal<br />

natural <strong>diamond</strong> are already used commercially but are limited in size to<br />

approximately 3x3x1 mm. These single-crystal <strong>diamond</strong>s are gradually<br />

being replaced by CVD <strong>diamond</strong> which is now available in shapes up to 15<br />

cm in diameter.t 30 !! 31 ! CVD-<strong>diamond</strong> heat sinks may be at the threshold <strong>of</strong><br />

large-scale commercialization <strong>and</strong> could be the most promising application<br />

<strong>of</strong> the material. 139 !<br />

5.6 Optical Applications<br />

A CVO <strong>diamond</strong> coating is yet to be produced with the optical clarity<br />

<strong>of</strong> single-crystal <strong>diamond</strong> <strong>and</strong>, for that reason, CVD <strong>diamond</strong> has found<br />

little application so far in optics. Typically CVD <strong>diamond</strong> coatings are<br />

translucent. Some are nearly white, some have a black tingeJ 54 '<br />

The rough surface <strong>of</strong> CVD <strong>diamond</strong> is also a drawback since an<br />

optically smooth coating is an essential requirement for most optical<br />

applications. The surface can be smoothed to some degree by increasing<br />

the nucleation density <strong>and</strong> by deposition strongly textured coatings<br />

where the surface consists <strong>of</strong> flat {100} faces more or less parallel to the<br />

substrate.1 55 ]<br />

Diamond for IR Windows. A new optical-brazing process bonds a<br />

thin layer <strong>of</strong> CVD <strong>diamond</strong> on a zinc sutfide or zinc selenide IR window.<br />

This thin layer is obtained by depositing <strong>diamond</strong> on a silicon substrate <strong>and</strong><br />

dissolving the silicon. The <strong>diamond</strong> layer is then brazed to the IR window<br />

with the smooth interface surface on the outside. The brazing material is<br />

an index-matching chalcogenide glassJ 56 ' This process is a possible<br />

solution to the optical-roughness problem mentioned above. The process<br />

is shown schematically in Fig. 13.9. In such an application, <strong>diamond</strong> would<br />

compete directly with <strong>diamond</strong>-like <strong>carbon</strong> (DLC) (see Ch. 14, Sec. 5.2).<br />

Advances in deposition techniques have now made possible the<br />

fabrication <strong>of</strong> free-st<strong>and</strong>ing shapes such as the 7.6 cm (3") diameter<br />

hemispherical dome for IR-window applications shown in Fig. 13.10 which<br />

may eventually replace the present IR materials.

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