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Chemkin 4.1.1<br />

Chapter 4: Materials Problems<br />

4.1.5.3 Project Results<br />

The gas temperatures in Figure 4-15 show that the gas heats up substantially near<br />

the deposition surface, with the hot zone expanding with axial distance, as expected.<br />

The inlet gas temperature is lower than the upper wall temperature, such that the<br />

coolest gas lies in a region near to, but below the top wall. This cooler gas region is<br />

reflected in the trichlorosilane mole fraction contours shown in Figure 4-16. Depletion<br />

as a result of chemical reaction causes the low SiCl 3 H mole fractions near the lower<br />

wall, but thermal diffusion causes the heavier gas to move away from the upper wall.<br />

A simulation run without thermal diffusion gives uniform SiCl 3 H mole fractions in the<br />

upper part of the reactor. Figure 4-17 shows how the deposition rate of solid silicon<br />

varies as a function of axial distance. Initially, the deposition rate is quite high, but it<br />

drops rapidly as the SiCl 3 H near the surface is depleted, indicating that the deposition<br />

process is transport limited in this system. Figure 4-18 shows gas-phase mole<br />

fractions near the lower surface as a function of axial distance. The extent of SiCl 3 H<br />

depletion and HCl formation is notably larger than the formation of the other siliconchlorine<br />

species (SiCl 2 , SiCl 2 H 2 and SiCl 4 ), which indicates that deposition of solid<br />

silicon is the dominant reaction pathway.<br />

Figure 4-15<br />

Trichlorosilane CVD—Gas Temperatures vs. Axial and Radial Distance<br />

© 2007 Reaction Design 132 RD0411-C20-000-001

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