Diamond growth in a direct-current low-pressure supersonic plasmajet

1997 ◽  
Vol 6 (2-4) ◽  
pp. 406-410 ◽  
Author(s):  
J. Laimer ◽  
H. Pauser ◽  
H. Störi ◽  
R. Haubner ◽  
B. Lux
1995 ◽  
Vol 10 (11) ◽  
pp. 2685-2688 ◽  
Author(s):  
Qijin Chen ◽  
Zhangda Lin

Diamond film was synthesized on thin Ti wafers (as thin as 40 μm) via hot filament chemical vapor deposition (HFCVD). The hydrogen embrittlement of the titanium substrate and the formation of a thick TiC interlayer were suppressed. A very low pressure (133 Pa) was employed to achieve high-density rapid nucleation and thus to suppress the formation of TiC. Oxygen was added to source gases to lower the growth temperature and therefore to slow down the hydrogenation of the thin Ti substrate. The role of the very low pressure during nucleation is discussed, providing insight into the nucleation mechanism of diamond on a titanium substrate. The as-grown diamond films were characterized by scanning electron microscopy (SEM), Raman spectroscopy, and x-ray analysis.


2013 ◽  
Vol 103 (25) ◽  
pp. 254104 ◽  
Author(s):  
Zhiying Chen ◽  
Lee Chen ◽  
Merritt Funk
Keyword(s):  

Author(s):  
jiamao gao ◽  
Hao Wu ◽  
Shimin Yu ◽  
Zhipeng Chen ◽  
Zhijiang Wang ◽  
...  

1997 ◽  
Vol 12 (12) ◽  
pp. 3250-3253 ◽  
Author(s):  
Ji-Tao Wang ◽  
Yong-Zhong Wan ◽  
David Wei Zhang ◽  
Zhi-Jie Liu ◽  
Zhong-Qiang Huang

Three-dimensional temperature (T)–pressure (P)–composition (X) phase diagrams of binary carbon-hydrogen (C–H) and carbon-oxygen (C–O) systems for activated low pressure diamond growth have been calculated. Based on an approximation of linear combination between C–H and C–O systems, a projective ternary carbonhydrogen-oxygen (C–H–O) phase diagram has also been obtained. There is always a diamond growth region in each of these phase diagrams. Once a supply of external activating energy stops, the diamond growth region will not exist. Nearly all of the reliable experimental data reported in the literature drop into the possible diamond growth region of the calculated projective ternary C–H–O phase diagram under the conditions of 0.01–100 kPa and above 700 K.


1995 ◽  
Vol 10 (8) ◽  
pp. 1993-2010 ◽  
Author(s):  
David S. Dandy ◽  
Michael E. Coltrin

A simplified model of a direct current arcjet-assisted diamond chemical vapor deposition reactor is presented. The model is based upon detailed theoretical analysis of the transport and chemical processes occurring during diamond deposition, and is formulated to yield closed-form solutions for diamond growth rate, defect density, and heat flux to the substrate. In a direct current arcjet reactor there is a natural division of the physical system into four characteristic domains: plasma torch, free stream, boundary layer, and surface, leading to the development of simplified thermodynamic, transport, and chemical kinetic models for each of the four regions. The models for these four regions are linked to form a single unified model. For a relatively wide range of reactor operating conditions, this simplified model yields results that are in good quantitative agreement with stagnation flow models containing detailed multicomponent transport and chemical kinetics. However, in contrast to the detailed reactor models, the model presented here executes in near real-time on a computer of modest size, and can therefore be readily incorporated into process control models or global dynamic loop simulations.


2020 ◽  
Vol 35 (7) ◽  
pp. 1450-1457
Author(s):  
Gagan Paudel ◽  
Sergey Khromov ◽  
Martin Kasik ◽  
Hans Jørgen Roven ◽  
Marisa Di Sabatino

It is likely that observation of roughness at crater bottom upon GDMS sputtering is due to differential sputtering of grains.


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