Radial atomic hydrogen flux measurements to the TEXTOR liner

1987 ◽  
Vol 145-147 ◽  
pp. 201-205 ◽  
Author(s):  
W.T. Shmayda ◽  
J. Winter ◽  
F. Waelbroeck ◽  
P. Wienhold
Vacuum ◽  
2016 ◽  
Vol 129 ◽  
pp. 178-182 ◽  
Author(s):  
A. Kuzmin ◽  
H. Zushi ◽  
I. Takagi ◽  
S.K. Sharma ◽  
Y. Hirooka ◽  
...  

2003 ◽  
Vol 29 (11) ◽  
pp. 897-900 ◽  
Author(s):  
V. A. Kagadei ◽  
E. V. Nefyodtsev ◽  
D. I. Proskurovsky ◽  
S. V. Romanenko

1994 ◽  
Vol 9 (6) ◽  
pp. 1546-1551 ◽  
Author(s):  
Darin S. Olson ◽  
Michael A. Kelly ◽  
Sanjiv Kapoor ◽  
Stig B. Hagstrom

We describe a growth mechanism of CVD diamond films consisting of a series of surface reactions. It is derived from experimental observations of a sequential deposition process in which incident carbon flux and atomic hydrogen flux were independently varied. In this sequential process, film growth rate increased with atomic hydrogen exposure, and a saturation in the utilization of carbon was observed. These features are consistent with a surface growth process consisting of the following steps: (i) the carburization of the diamond surface, (ii) the deposition of highly disordered carbon on top of this surface, (iii) the etching of disordered carbon by atomic hydrogen, (iv) the conversion of the carburized diamond surface to diamond at growth sites by atomic hydrogen, and (v) the carburization of newly grown diamond surface. The nature of the growth sites on the diamond surface has not been determined experimentally, and the existence of the carburized surface layer has not been demonstrated experimentally. The surface growth mechanism is the only one consistent with the growth observed in conventional diamond reactors and the sequential reactor, while precluding the necessity of gas phase precursors.


1990 ◽  
Vol 5 (11) ◽  
pp. 2326-2333 ◽  
Author(s):  
M. A. Cappelli ◽  
T. G. Owano ◽  
C. H. Kruger

A study of diamond synthesis in an atmospheric pressure inductively coupled argon-hydrogen-methane plasma is presented. The plasma generated has an active area of 20 cm2 and a free stream temperature of approximately 5000 K. Deposition experiments lasting 1 h in duration have been performed in both stagnation flow and flat plate parallel flow geometries. The diamond film deposited in both configurations are nonuniform yet fairly reproducible. The variation in the growth rates at various regions of the substrate is attributed to the variation in the surface atomic hydrogen flux. Growth rates are as high as 50 μm/h, in regions of the substrate where the atomic hydrogen flux is expected to be large. Little or no growth is observed in regions where the atomic hydrogen is expected to recombine within the thermal boundary layer before arriving at the surface. Individual particles are analyzed by micro-Raman spectroscopy. Large (50 μm) size well-faceted particles show little evidence of non-diamond carbon content and are found to be under a state of compression, displaying shifts in the principal phonon mode as great as 3 cm−1.


2008 ◽  
Vol 51 (1) ◽  
pp. 142-146 ◽  
Author(s):  
V. A. Kagadei ◽  
E. V. Nefedtsev ◽  
D. I. Proskurovskii ◽  
S. V. Romanenko ◽  
V. V. Chupin

Sign in / Sign up

Export Citation Format

Share Document