scholarly journals Plasma-enhanced chemical vapor deposition of amorphous Si on graphene

2016 ◽  
Vol 108 (19) ◽  
pp. 193105 ◽  
Author(s):  
G. Lupina ◽  
C. Strobel ◽  
J. Dabrowski ◽  
G. Lippert ◽  
J. Kitzmann ◽  
...  
2010 ◽  
Vol 107 (4) ◽  
pp. 043503 ◽  
Author(s):  
I. Crupi ◽  
S. Mirabella ◽  
D. D’Angelo ◽  
S. Gibilisco ◽  
A. Grasso ◽  
...  

2006 ◽  
Vol 510-511 ◽  
pp. 954-957
Author(s):  
Myung Beom Park ◽  
Jae Hyun Shim ◽  
Nam Hee Cho

Hydrogenated amorphous Si (a-Si:H) films were prepared by plasma enhanced chemical vapor deposition (PECVD) techniques, and the effect of nano-structure on the photoluminescence (PL) phenomena of the films was investigated. The films, which were prepared at R.T., contain both amorphous and crystalline phases of 1 ~ 3 nm size nano-crystallites with {100} orientation preference while the films prepared at 500°C are composed of about 6 nm and 150 nm size crystallites. The former exhibit a strong PL intensity near blue light region, while the latter exhibiting little PL phenomena; also, the optical band gap of the former was calculated at 4.2 eV.


2008 ◽  
Vol 8 (5) ◽  
pp. 2540-2543 ◽  
Author(s):  
S. M. Kang ◽  
S. G. Yoon ◽  
S.-W. Kim ◽  
D. H. Yoon

Amorphous Si (a-Si) quantum dots (QDs) embedded in a silicon nitride film were prepared by a plasma-enhanced chemical vapor deposition (PECVD) technique using gaseous mixtures of silane, hydrogen and nitrogen. We observed that the Si QDs had an amorphous structure from the Raman spectroscopy measurement. The Fourier transform infrared (FTIR) spectra showed that the relative transmittance of the SiH bands decreased, but that of the NH bands increased, with increasing nitrogen flow rate. During the deposition of SiNx, the number of dangling bonds of silicon acting as nucleation sites increased. As the hydrogen flow rate increased the growth rate decreased, due to the reduction in the hydrogen partial pressure. The hydrogen and nitrogen gas flow rates were found to be important parameters for determining the size of the a-Si QDs. In addition, we observed that the PL peak shifted toward a higher energy with increasing hydrogen and nitrogen gas flow rates, which was attributed to the increase in the quantum confinement effect in the a-Si QDs.


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