Nuclear Magnetic Resonance (NMR) of Porous Silicon

1996 ◽  
Vol 452 ◽  
Author(s):  
W. K. Chang ◽  
M. Y. Liao ◽  
K. K. Gleason

AbstractPorous silicon (PS) was characterized by 1H, 19F and 29Si solid-state nuclear magnetic resonance (NMR). On freshly prepared samples, hydrogen contents were between 3 × 1014 and 3 × 1015 per cm2 of PS surface area, while fluorine concentrations were below the detection limit. Cross-polarization (CP) was used to selectively observe the 29Si near the hydrogen passivation. The features of the 29Si NMR spectra are assigned as (O)2(Si)Si-H (-50 ppm), (O)3Si-H (-84 ppm), (Si)3Si-H (-91 ppm), (Si)2Si-H2 (-102 ppm) and (O)4Si (-109 ppm). Changes resulting from low temperature annealing in air and an HF soak were observed by both NMR and infrared spectroscopy. The 29Si NMR line widths for PS fall between those for crystalline silicon and those for amorphous hydrogenated silicon films (a-Si:H), suggesting disorder near the PS surface is intermediate between these extremes. However, comparison of the isotropie chemical shift values shows that the bonding in the disordered regions of PS differs from that found in a-Si:H. In addition, the sharp 29Si NMR resonance observed in the bulk single crystal starting material can not be resolved in the spectra of PS. Thus, well-ordered silicon nanocrystallites in the PS are either several bond-lengths removed from hydrogen or comprise only a small fraction of the PS layer.

1986 ◽  
Vol 60 (5) ◽  
pp. 1839-1841 ◽  
Author(s):  
Shigenobu Hayashi ◽  
Kikuko Hayamizu ◽  
Satoshi Yamasaki ◽  
Akihisa Matsuda ◽  
Kazunobu Tanaka

1997 ◽  
Vol 70 (2) ◽  
pp. 191-193 ◽  
Author(s):  
D. Petit ◽  
J.-N. Chazalviel ◽  
F. Ozanam ◽  
F. Devreux

1986 ◽  
Vol 25 (Part 2, No. 4) ◽  
pp. L313-L315 ◽  
Author(s):  
Shigenobu Hayashi ◽  
Kikuko Hayamizu ◽  
Satoshi Yamasaki ◽  
Akihisa Matsuda ◽  
Kazunobu Tanaka

1996 ◽  
Vol 100 (50) ◽  
pp. 19653-19658 ◽  
Author(s):  
W. K. Chang ◽  
M. Y. Liao ◽  
K. K. Gleason

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.


1991 ◽  
Vol 219 ◽  
Author(s):  
Man Ken Cheung ◽  
Mark A. Petrich

ABSTRACTWe report here the first phase of our attempt to deposit “device-quality” a-Si:H films by glow discharge near room temperature (50 °C). We have found that, at a low rf power density (40 mW/cm2) and high hydrogen/silane ratios (≥ 2), film quality is not uniquely determined by the substrate temperature, Ts. The microstructure of our low hydrogen content films as revealed by infrared (IR) and nuclear magnetic resonance (NMR) spectroscopies is similar to that of “device-quality” films deposited at standard Ts. The next phase of our work is to ascertain whether or not similar IR and NMR characteristics between our low Ts films and the standard Ts films imply also similar opto-electronic properties.


Author(s):  
M.J. Hennessy ◽  
E. Kwok

Much progress in nuclear magnetic resonance microscope has been made in the last few years as a result of improved instrumentation and techniques being made available through basic research in magnetic resonance imaging (MRI) technologies for medicine. Nuclear magnetic resonance (NMR) was first observed in the hydrogen nucleus in water by Bloch, Purcell and Pound over 40 years ago. Today, in medicine, virtually all commercial MRI scans are made of water bound in tissue. This is also true for NMR microscopy, which has focussed mainly on biological applications. The reason water is the favored molecule for NMR is because water is,the most abundant molecule in biology. It is also the most NMR sensitive having the largest nuclear magnetic moment and having reasonable room temperature relaxation times (from 10 ms to 3 sec). The contrast seen in magnetic resonance images is due mostly to distribution of water relaxation times in sample which are extremely sensitive to the local environment.


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