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Articles

Modeling for particle size prediction and mechanism of silicon nitride nanoparticle synthesis by chemical vapor deposition

, &
Pages 845-855 | Received 24 Jan 2017, Accepted 06 Mar 2017, Published online: 05 Apr 2017

Figures & data

Figure 1. Physical model for radiation and convection in ultrafine silicon nitride production through CVD. This represents silicon nitride nucleation and the condensation process of cooling by argon. Silicon nitride molecules result from the thermal chemical reaction between silane and ammonia. is the energy dissipated though radiative heat transfer, and is the energy dissipated though convective heat transfer.

Figure 1. Physical model for radiation and convection in ultrafine silicon nitride production through CVD. This represents silicon nitride nucleation and the condensation process of cooling by argon. Silicon nitride molecules result from the thermal chemical reaction between silane and ammonia. is the energy dissipated though radiative heat transfer, and is the energy dissipated though convective heat transfer.

Figure 2. Energy exchanges because of collisions between silicon nitride molecules and argon atoms. Solid spheres in this figure represent silicon nitride molecules, and hollow ones represent argon atoms. Changes in color show how energy is transmitted. Assume , and represents the initial temperature of the silicon nitride vapor, represents the initial temperature of the inert gas.

Figure 2. Energy exchanges because of collisions between silicon nitride molecules and argon atoms. Solid spheres in this figure represent silicon nitride molecules, and hollow ones represent argon atoms. Changes in color show how energy is transmitted. Assume , and represents the initial temperature of the silicon nitride vapor, represents the initial temperature of the inert gas.

Figure 3. Flow chart simulating the modeling of ultrafine silicon nitride powder production by CVD.

Figure 3. Flow chart simulating the modeling of ultrafine silicon nitride powder production by CVD.

Figure 4. Flow diagram of laser-driven CVD experiment; feed gas are silane and ammonia, inert gas is argon.

Figure 4. Flow diagram of laser-driven CVD experiment; feed gas are silane and ammonia, inert gas is argon.

Figure 5. Comparison between calculated results and experimental ones.

Figure 5. Comparison between calculated results and experimental ones.

Figure 6. Diameter of silicon nitride particle and molecule number in the particle as a function of pressure in the condensation room.

Figure 6. Diameter of silicon nitride particle and molecule number in the particle as a function of pressure in the condensation room.

Figure 7. Energy variation of the condensation nucleus under different absolute pressure in the condensation room as a function of the number of molecules in the particle.

Figure 7. Energy variation of the condensation nucleus under different absolute pressure in the condensation room as a function of the number of molecules in the particle.

Figure 8. Mechanisms of ultrafine silicon nitride powder prepared by CVD. (a) The thermochemical reaction process. (b) The nucleation and condensation nuclei growth process, and argon is employed for cooling. (c) The deposition process.

Figure 8. Mechanisms of ultrafine silicon nitride powder prepared by CVD. (a) The thermochemical reaction process. (b) The nucleation and condensation nuclei growth process, and argon is employed for cooling. (c) The deposition process.

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