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handbook of carbon, graphite, diamond and fullerenes

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CVD Diamond 319<br />

(see Ch. 2, Sec. 2.1). The deposition <strong>of</strong> 12 C <strong>diamond</strong> is accomplished by<br />

the decomposition in a microwave plasma <strong>of</strong> methane in which the <strong>carbon</strong><br />

atom is 99.97% 12 C. The resulting polycrystalline deposit is crushed,<br />

processed to a single crystal with molten iron <strong>and</strong> aluminum at high<br />

temperature <strong>and</strong> pressure, <strong>and</strong> recovered by leaching out the metalsl 37 ^ 38 ]<br />

(SeeCh. 12, Sec. 3.0).<br />

In <strong>diamond</strong>, thermal conductivity occurs by aflow <strong>of</strong> phonons (see Ch.<br />

11, Sec. 5.2). These phonons are scattered by imperfections such as<br />

isotopic imperfections <strong>and</strong> the scattering varies as the fourth power <strong>of</strong> the<br />

phonon frequency. Thus, the exclusion <strong>of</strong> 13 C should result in a significant<br />

increase in thermal conductivity. This increase was confirmed experimentally<br />

as 12 C <strong>diamond</strong> is reported to have a 50% higher thermal conductivity<br />

than natural <strong>diamond</strong>.I 37 " 38 ' It is also reported to be harder than natural<br />

<strong>diamond</strong> by a few percent as determined by the relation between hardness<br />

<strong>and</strong> the elastic coefficients (see Ch. 11, Sec. 10.2).<br />

3.8 Nucleation <strong>and</strong> Structure<br />

CVD <strong>diamond</strong> is a polycrystalline material with grain size ranging from<br />

a few nanometers to a few micrometers. The polycrystallinity results from<br />

the formation <strong>of</strong> separate nuclei on the deposition surface. As deposition<br />

proceeds, these nuclei eventually coalesce to form acontinuousfilm. Some<br />

grow in size while other are crowded out <strong>and</strong> the average crystal size <strong>of</strong>ten<br />

becomes larger as thickness increases. Some degree <strong>of</strong> crystal orientation<br />

(texture) can be achieved. A cross-section <strong>of</strong> a coating is shown in Fig. 13.7.<br />

As mentioned in Ch. 11, the most prevalent crystal surfaces in CVD<br />

<strong>diamond</strong> are the (111) octahedral <strong>and</strong> the (100) cubic. Cubo-octahedral<br />

crystals combining both <strong>of</strong> these surfaces are also common. Twinning<br />

occurs frequently at the (111) surface. The 6H structure may also be<br />

present.<br />

3.9 Substrate Preparation <strong>and</strong> Adhesion<br />

The nature <strong>of</strong> the substrate <strong>and</strong> its predeposition treatment play a<br />

major role in determining the surface nucleation rate but not necessarily the<br />

rate <strong>of</strong> subsequent growth (after the immediate surface layer is deposited)<br />

.t 13 !! 39 ! The most widely used substrate is still silicon, but other materials<br />

perform successfully such as the refractory metals (W, Ta, Mo), carbides

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