RAMAN SCATTERING IN ANNEAL STABLE AMORPHOUS SILICON

1981 ◽  
Vol 42 (C6) ◽  
pp. C6-54-C6-56 ◽  
Author(s):  
S. T. Kshirsagar ◽  
J. S. Lannin
2013 ◽  
Vol 49 (9) ◽  
pp. 610-612
Author(s):  
K. Tanizawa ◽  
S. Suda ◽  
Y. Sakakibara ◽  
T. Kamei ◽  
R. Takei ◽  
...  

2009 ◽  
Vol 255 (19) ◽  
pp. 8252-8256 ◽  
Author(s):  
Thanh Nga Nguyen ◽  
Van Duy Nguyen ◽  
Sungwook Jung ◽  
Junsin Yi

1989 ◽  
Vol 40 (15) ◽  
pp. 10420-10424 ◽  
Author(s):  
M. C. Lee ◽  
C. R. Huang ◽  
Y. S. Chang ◽  
Y. F. Chao

2012 ◽  
Vol 2012 ◽  
pp. 1-5 ◽  
Author(s):  
M. A. Ferrara ◽  
I. Rendina ◽  
S. N. Basu ◽  
L. Dal Negro ◽  
L. Sirleto

The observation of stimulated Raman scattering in amorphous silicon nanoparticles embedded in Si-rich nitride/silicon superlattice structures (SRN/Si-SLs) is reported. Using a 1427 nm continuous-wavelength pump laser, an amplification of Stokes signal up to 0.9 dB/cm at 1540.6 nm and a significant reduction in threshold power of about 40% with respect to silicon are experimentally demonstrated. Our results indicate that amorphous silicon nanoparticles are a great promise for Si-based Raman lasers.


1993 ◽  
Vol 48 (9) ◽  
pp. 6024-6032 ◽  
Author(s):  
A. Zwick ◽  
R. Carles

1993 ◽  
Vol 321 ◽  
Author(s):  
Nagarajan Sridhar ◽  
D. D. L. Chung ◽  
W. A. Anderson ◽  
W. Y. Yu ◽  
L. P. Fu ◽  
...  

ABSTRACTWe observed the processes of hydrogen evolution and crystallization in hydrogenated Amorphous silicon 0.5–7 μm thick films (deposited by dc glow discharge on Molybdenum) by differential scanning calorimetry (DSC), Raman scattering and thermogravimetric analysis (TGA). Investigation was made as a function of doping, deposition temperature and film thickness. For all the films, an endothermic DSC peak was observed at 694 °C (onset). That this peak was at least partly due to hydrogen evolution was shown by TGA, which showed weight loss beginning at 694 °C, and by evolved gas analysis, which showed hydrogen evolution at 694 °C. This temperature (658–704 °C) increased with increasing heating rate (5–30 °C/min). Doping reduced this temperature from 694 to 625 °C for boron doping and to 675 °C for phosphorous doping. Hydrogen evolution kinetics and FTIR results suggest that the silicon-hydrogen bonding in the intrinsic film was a mixture of SiH and S1H2, and was predominantly SiH in the phosphorous doped films and SiH2 in the boron doped films. Crystallization was independent of silicon-hydrogen bonding in the as-deposited Amorphous silicon film. It was bulk (not interface) induced. No exothermic DSC peak accompanied the crystallization. The film deposition temperature had little effect on the DSC result, but crystallization was enhanced by a higher deposition temperature.


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