Amorphous Silicon Deposition Diagnostics Using Coherent Anti-Stokes Raman Spectroscopy

1987 ◽  
Vol 95 ◽  
Author(s):  
Y. H. Shing ◽  
J. W. Perry ◽  
D. R. Coulter ◽  
G. Radhakrishnan

AbstractIn situ process diagnostics using coherent anti-Stokes Raman spectroscopy (CARS) have been performed under state-of-the-art a-Si:H film deposition conditions in a reactor designed for a-Si:H solar cell fabrication. The silane plasma of device-quality a-Si:H film depositions was monitored by measuring the silane ν1 band CARS spectrum to determine the depletion induced by the RF glow discharge. The silane depletion is linearly dependent on the RF power in the region of 4 to 12 W with a slope of O.5%/mWcm−2. The depletion is also dependent on the SiH4 flow rate starting with a 50% depletion at a low flow rate of 5.6 sccm and asymptotically approaching an 8% depletion at a high flow rate of 80 sccm. The a-Si:H film deposition rate is systematically measured as a function of the flow rate and the RF power. Linear correlations between the silane depletion and the film deposition rate are observed. The results are discussed in terms of primary electron impact dissociations of silane and the residence time of SiH4 molecule in the glow discharge region.

2011 ◽  
Vol 63 (6) ◽  
pp. 433-439 ◽  
Author(s):  
Mohammad Asaduzzaman Chowdhury ◽  
Dewan Muhammad Nuruzzaman ◽  
Khaled Khalil ◽  
Mohammad Lutfar Rahaman

Author(s):  
Mohammad A. Chowdhury ◽  
Dewan M. Nuruzzaman ◽  
Mohammad L. Rahaman

Solid thin films have been deposited on carbon steel substrates in a chemical vapor deposition (CVD) reactor where natural gas, mostly methane (CH4), was used as a precursor gas. The effect of gas flow rate on the thin film deposition rate has been investigated experimentally. The effect of gap between activation heater and substrate on the deposition rate has also been observed. To do so, a hot filament thermal chemical vapor deposition unit is used. The flow rate of natural gas varies from 0.5 to 2 l/min at normal temperature and pressure (NTP) and the gap between activation heater and substrate varies from 4 to 6.5 mm. Results show that the deposition rate on carbon steel increases with the increase of gas flow rate. It is also seen that deposition rate increases with the decrease of gap between activation heater and substrate within the observed range. These results are analyzed by dimensional analysis to correlate the deposition rate with gas flow rate, surface roughness and film thickness. In addition, friction coefficient and wear rate of carbon steel sliding against SS 304 under different normal loads are also investigated before and after deposition. The obtained results reveal that in general, the values of friction coefficient and wear rate are lower after deposition than that of before deposition.


2013 ◽  
Vol 114 (4) ◽  
pp. 1295-1301
Author(s):  
Thomas Reichenbacher ◽  
Simon Schuetz ◽  
Ilja Stasewitsch ◽  
Stephan Fabig

Shinku ◽  
1991 ◽  
Vol 34 (4) ◽  
pp. 427-431
Author(s):  
Mitsuo. SHIMOZUMA ◽  
Jin. MURAKAMI ◽  
Gen. TOCHITANI ◽  
Takashi. TSUJI ◽  
Hiroaki. TAGASHIRA

2012 ◽  
Vol 576 ◽  
pp. 594-597 ◽  
Author(s):  
Mohammad Asaduzzaman Chowdhury ◽  
Dewan Muhammad Nuruzzaman

A hot filament thermal chemical vapor deposition (CVD) reactor was used to deposit solid thin films on stainless steel 316 (SS 316) substrates at different flow rates of natural gas. The variation of thin film deposition rate with the variation of gas flow rate has been investigated experimentally. During experiment, the effect of gap between activation heater and substrate on the deposition rate has also been observed. Results show that deposition rate on SS 316 increases with the increase in gas flow rate. It is also observed that deposition rate increases with the decrease in gap between activation heater and substrate within the observed range. In addition, friction coefficient and wear rate of SS 316 sliding against SS 304 under different normal loads are also investigated before and after deposition. The experimental results reveal that improved friction coefficient and wear rate are obtained after deposition as compared to that of before deposition.


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