Porous Silicon by Galvanostatic Electrochemical Anodisation of Epitaxial Silicon, Polycrystalline Silicon and Silicon on Insulator Layers

Author(s):  
M. Ivanda ◽  
M. Balarin ◽  
O. Gamulin ◽  
V. Đerek ◽  
D. Ristić ◽  
...  
1989 ◽  
Vol 148 ◽  
Author(s):  
L.T.P. Allen ◽  
P.M. Zavracky ◽  
D.P. Vu ◽  
M.W. Batty ◽  
W.R. Henderson ◽  
...  

ABSTRACTIsolated silicon epitaxy (ISE) is a proven method of producing single crystalline silicon-on-insulator (SOI) material with excellent electrical properties. The presence of the remaining isolated dislocation trails in the epitaxial silicon has led to this investigation of the crystallinity throughout the ISE SOI layer and across the isolated dislocations. The structural perfection of these layers has been examined by defect etching, Nomarski optical microscopy, electron channeling patterns, and with more sensitivity using double crystal synchrotron X-ray diffraction and topography. Defect etching reveals the dislocation density within the layers of production ISE SOI material to be ~5×l0 5 /cm2. Electron channeling pattern techniques have reached the resolution limit of angular orientation resolution for the isolated silicon layer. Finally, synchrotron studies have shown that orientation homogeneity across 5" wafers are preserved to 0.006° and the variation in orientation across the defect trails to be, in general, less than 10 arcsec (0.003°), indicating single crystalline ISE SOI production material.


1990 ◽  
Vol 41-42 ◽  
pp. 604-613 ◽  
Author(s):  
G. Bomchil ◽  
A. Halimaoui ◽  
R. Herino

1992 ◽  
Vol 283 ◽  
Author(s):  
R. E. Hummel ◽  
S.-S. Chang ◽  
M. Ludwig ◽  
A. Morrone

ABSTRACTPorous silicon which has been prepared by a “dry” technique, that is, by spark erosion, yields similar photoluminescence spectra as anodically etched porous silicon which has been prepared in aqueous solutions. Fourier transform infrared spectra reveal that the dominant features in spark eroded silicon are the Si-O-Si stretching mode and the Si-O-Si bending mode. No infrared vibrational modes characteristic for siloxene have been found in spark eroded Si. Results from X-ray and electron diffraction studies suggest that spark eroded Si involves minute polycrystalline silicon particles which are imbedded in an amorphous matrix.


1983 ◽  
Vol 29 ◽  
Author(s):  
J. M. Gee ◽  
P. J. Hargis ◽  
M. J. Carr ◽  
D. R. Tallant ◽  
R. W. Light

ABSTRACTIn this paper we report a new method of silicon deposition using the interaction between the radiation from a pulsed-ultraviolet excimer laser and the plasma species produced in a glow discharge in silane (SiH4). Examination of the deposited film by laser Raman spectroscopy and by transmission electron microscopy revealed that the morphology ranged from polycrystalline silicon at laser fluences of 0.13–0.17 J/cm2 to epitaxial silicon at fluences of 0.4–0.6 J/cm2 . Growth rates of 100 nm/min for polycrystalline silicon and 30 nm/min for monocrystalline silicon were achieved.


1987 ◽  
Vol 105 ◽  
Author(s):  
Kyung-Ho Park ◽  
T. Sasaki ◽  
S. Matsuoka ◽  
M. Yoshida ◽  
M. Nakano

AbstractInterfaces between two kind of substrate, a bulk silicon wafer and a laser-recrystallized Silicon-On-Insulator (SOI), and its thermally grown oxide have been studied. High resolution transmission electron microscopy (HRTEM) of cross sectional specimen shows that the roughness at the interface is atomically flat and nearly uniform for the bulk single crystal silicon and silicon oxide, while being nonuniform and rough as much as 20 nm height for the recrystallized silicon and silicon oxide interface. Consideration of interface between recrystallized silicon and silicon oxide, and the oxide surface above, the observed roughness at the interface is due to original grain boundaries of polycrystalline silicon which was used as the material for the laser recrystallized silicon formation. It is also discussed HRTEM of the interface between polycrystalline silicon and silicon oxide.


1987 ◽  
Vol 51 (5) ◽  
pp. 343-345 ◽  
Author(s):  
J. Narayan ◽  
S. Y. Kim ◽  
K. Vedam ◽  
R. Manukonda

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