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Diamond Detectors for Ionizing Radiation - HEPHY

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CHAPTER 3. MATERIAL PROPERTIES 12<br />

oxygen gas. When the gas mixture is ionized, carbon based radicals are reduced and<br />

settle on a substrate, usually silicon or molybdenum, and link together with -type bonds,<br />

<strong>for</strong>ming a diamond lattice. Successful diamond deposition is restricted to a well dened<br />

area within the C-H-O ternary diagram shown in g. 3.2. Outside this area, either nondiamond<br />

carbon or nothing at all is grown.<br />

Figure 3.2: The C-H-O ternary diagram. CVD <strong>Diamond</strong> growth is restricted to the white area<br />

in the center [7].<br />

The properties of the diamond grown in this process depend on the gas mixture,<br />

temperature and pressure. Although this is an easy principle, the growth process is<br />

extremely dicult to control in order to grow material suitable <strong>for</strong> detector application;<br />

the parameters are not constant throughout the process. The growth speed is typically<br />

about 1 mh ,1 . There are several types of CVD reactors, which dier in the way the gas<br />

is ionized; e.g., this is done by microwaves or by a heating wire. After the growth process,<br />

the substrate is etched from the diamond lm, which is then cut and cleaned.<br />

Initially, there is a large number of small crystal seeds on the substrate, each oriented<br />

individually. As deposition continues, the grains grow together, <strong>for</strong>ming columnar singlecrystals<br />

with grain boundaries between. On the substrate side the lateral grain size is very<br />

small (in the order of micrometers), while the size continuously increases in the growth

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