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Byeong-Joo Lee www.postech.ac.kr/~calphad
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Byeong-Joo Lee www.postech.ac.kr/~calphad Scope CVD 1.Too much changeable results depending on the condition 2.Beyond Scientific Explanation for long time 3.Process development has been mostly empirical Approach (by Nong Moon Hwang, KRISS/SNU) 1.How to define the driving force of CVD 2.Low pressure synthesis of Diamond 3.Charged Cluster Model in CVD References ▶ N.M. Hwang et al., Diamond and Related Materials, 1 (1992) 191-194.; 3 (1993) 163-167. ▶ N.M. Hwang et al., J. Crystal Growth 135 (1994) 165-171; 143 (1994) 103-109; 160 (1996) 87-97; 160 (1996) 98-103; 162 (1996) 55-68.
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Byeong-Joo Lee www.postech.ac.kr/~calphad ※ Example: Deposition of Silicon SiH 4 + 2Cl 2 = Si + 4HCl Driving force of CVD Deposition - from N.M. Hwang, SNU
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Byeong-Joo Lee www.postech.ac.kr/~calphad Diamond formation with simultaneous graphite etching in low pressure synthesis of diamond in low pressure synthesis of diamond Thermodynamic Paradox
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Byeong-Joo Lee www.postech.ac.kr/~calphad CVD Diamond - N.M. Hwang et al., J. Crystal Growth 162, 55 (1996) Diamond deposited on silicon substrate Soot deposited on the iron substrate
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Byeong-Joo Lee www.postech.ac.kr/~calphad CVD Si - N.M. Hwang et al., J. Crystal Growth 218, 27 (2000)
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Byeong-Joo Lee www.postech.ac.kr/~calphad CVD Si Nanowire - N.M. Hwang et al., J. Crystal Growth 218, 33 (2000)
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Byeong-Joo Lee www.postech.ac.kr/~calphad The nucleation ratio is very sensitive to the variation of the surface energy ranging from 10 10 to 10 -6 with σ dia = 3.7 and 4.1 J/m 2 at 1200K and σ gra = 3.1 J/m 2 → There must be some factor that modifies the surface energy of diamond → Creation of the Charged Cluster Model Nucleation of clusters in gas phase - Diamond/Graphite
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