Pulsed and continuous wave plasma deposition of amorphous, hydrogenated silicon carbide from SiH4/CH4 plasmas

1999 ◽  
Vol 17 (5) ◽  
pp. 2475-2484 ◽  
Author(s):  
Patrick R. McCurdy ◽  
Jason M. Truitt ◽  
Ellen R. Fisher
1991 ◽  
Vol 219 ◽  
Author(s):  
Hsueh Yi Lu ◽  
Mark A. Petrich

ABSTRACTWe present evidence that an independently applied dc bias voltage has a significant effect on the plasma deposition of amorphous hydrogenated silicon carbide. Deposition rates increase with either positive or negative dc voltages applied to the powered rf electrode. The microstructure of the films (as determined by infrared absorption) can be reduced by increasing the plasma potential (positive dc bias voltages). Negative dc biases, or excessively high positive biases, result in increased amounts of film microstructure. Film carbon content is increased when positive biases are applied, but the optical band gaps decrease suggesting increased amounts of graphitic bonding configurations. Negative biases do not change the carbon content of the films, but do increase both deposition rate and microstructure.


1998 ◽  
Vol 1 (2) ◽  
pp. 81-85
Author(s):  
Clara EE Hanekamp ◽  
Hans JRM Bonnier ◽  
Rolf H Michels ◽  
Kathinka H Peels ◽  
Eric PCM Heijmen ◽  
...  

2003 ◽  
Vol 17 (09) ◽  
pp. 387-392 ◽  
Author(s):  
NIKIFOR RAKOV ◽  
ARSHAD MAHMOOD ◽  
MUFEI XIAO

Amorphous hydrogenated silicon carbide (a-SiC:H) thin films have been prepared by the RF reactive magnetron sputtering technique. The optical properties of the films have been studied by optical spectroscopy with an incoherent light source. The material is commonly regarded as a dielectric. We have discovered however that some films that were prepared under certain deposition conditions and on certain substrates may respond to external light as a metallic thin film, i.e. there are strongly enhanced reflection peaks in the optical spectrum. We have further discovered that some films may have a strong and broadened absorption peak at about 590 nm, which is an apparent photonic bandgap in the visible spectrum. The appearance of the photonic bandgap is very sensitive to two parameters: the substrate and the deposition gas. By changing the two parameters, one shifts the status of the film from with and without the photonic bandgap.


2009 ◽  
Vol 15 (1-3) ◽  
pp. 39-46 ◽  
Author(s):  
Aleksander M. Wrobel ◽  
Agnieszka Walkiewicz-Pietrzykowska ◽  
Marja Ahola ◽  
I. Juhani Vayrynen ◽  
Francisco J. Ferrer-Fernandez ◽  
...  

MRS Advances ◽  
2016 ◽  
Vol 1 (43) ◽  
pp. 2929-2934 ◽  
Author(s):  
J. A. Guerra ◽  
L. M. Montañez ◽  
K. Tucto ◽  
J. Angulo ◽  
J. A. Töfflinger ◽  
...  

ABSTRACTA simple model to describe the fundamental absorption of amorphous hydrogenated silicon carbide thin films based on band fluctuations is presented. It provides a general equation describing both the Urbach and Tauc regions in the absorption spectrum. In principle, our model is applicable to any amorphous material and it allows the determination of the bandgap. Here we focus on the bandgap engineering of amorphous hydrogenated silicon carbide layers. Emphasis is given on the role of hydrogen dilution during the deposition process and post deposition annealing treatments. Using the conventional Urbach and Tauc equations, it was found that an increase/decrease of the Urbach energy produces a shrink/enhancement of the Tauc-gap. On the contrary, the here proposed model provides a bandgap energy which behaves independently of the Urbach energy.


1987 ◽  
Vol 95 ◽  
Author(s):  
Mark A. Petrich ◽  
Jeffrey A. Reimer

AbstractWe present the results of a carbon-13 nuclear magnetic resonance (NMR) study of well-characterized thin films of amorphous hydrogenated silicon carbide. The NMR data detail the distribution of carbon local bonding configurations in films which have carbon-to-silicon ratios less than one. In particular, we show data which clearly identify and quantify non-hydrogenated sp2, or unsaturated, carbon bonding environments.


1994 ◽  
Vol 114-115 (1) ◽  
pp. 255-260 ◽  
Author(s):  
Allison Cook ◽  
Alexander G. Fitzgerald ◽  
Faridah Ibrahim ◽  
John I. B. Wilson ◽  
Philip John

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