Thermodynamic Simulation of Polycrystalline Silicon Chemical Vapor Deposition in Si–Cl–H System


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Resumo

Based on thermodynamic data for related pure substances, the relations of (nCl/nH)Eq and (nCl/nH)o have been plotted in the Si–Cl–H system. The results show that the difference of (nSi/nCl)o and (nSi/nCl)Eq is the driving force for polycrystalline silicon chemical vapor deposition (CVD). SiHCl3 is preferred for polycrystalline silicon deposition to SiCl4. SiH2Cl2 would be even better, but it is not stable as a gas and hence it is less frequently used. Then, thermodynamic simulation of polycrystalline silicon CVD in the Si–H–Cl system has been investigated. The pressure has a negative effect on polycrystalline silicon yield. The optimum temperature is 1400 K, at which the kinetic rate of rate-determining step for the main reaction is large enough. The excess hydrogen is necessary for polycrystalline silicon CVD in the Si–Cl–H system. However, the silicon deposition rate increases then decreases with increasing H2 molar fraction. The optimum H2 molar fraction should be determined by considering thermodynamics and transport phenomena simultaneously. Finally, the optimum conditions have been obtained as 1400 K, about 0.1 MPa, and H2 to SiHCl3 ratio of 15, which are close to the limited reported values in the open literature. Under the optimum conditions, the silicon yield ratio is 34.82% against 20% reported in the open literature.

Sobre autores

Yangmin Zhou

State Key Laboratory of Complex Nonferrous Metal Resources Clean Utilization, Kunming University of Science
and Technology; Faculty of Metallurgical and Energy Engineering, Kunming University of Science and Technology; Kunming Metallurgical Research Institute

Email: hhouyanqing@163.com
República Popular da China, Kunming; Kunming; Kunming

Yanqing Hou

State Key Laboratory of Complex Nonferrous Metal Resources Clean Utilization, Kunming University of Science
and Technology

Autor responsável pela correspondência
Email: hhouyanqing@163.com
República Popular da China, Kunming

Zhifeng Nie

State Key Laboratory of Complex Nonferrous Metal Resources Clean Utilization, Kunming University of Science
and Technology; Faculty of Metallurgical and Energy Engineering, Kunming University of Science and Technology

Email: hhouyanqing@163.com
República Popular da China, Kunming; Kunming

Gang Xie

State Key Laboratory of Complex Nonferrous Metal Resources Clean Utilization, Kunming University of Science
and Technology; Kunming Metallurgical Research Institute

Email: hhouyanqing@163.com
República Popular da China, Kunming; Kunming

Wenhui Ma

State Key Laboratory of Complex Nonferrous Metal Resources Clean Utilization, Kunming University of Science
and Technology; Faculty of Metallurgical and Energy Engineering, Kunming University of Science and Technology

Email: hhouyanqing@163.com
República Popular da China, Kunming; Kunming

Yongnian Dai

State Key Laboratory of Complex Nonferrous Metal Resources Clean Utilization, Kunming University of Science
and Technology; Faculty of Metallurgical and Energy Engineering, Kunming University of Science and Technology

Email: hhouyanqing@163.com
República Popular da China, Kunming; Kunming

Palghat Ramachandran

Department of Energy, Environmental and Chemical Engineering, Washington University in St. Louis

Email: hhouyanqing@163.com
Estados Unidos da América, MO

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