Laser Raman microprobe analysis of the modified surface of He+-irradiated graphite

1991 ◽  
Vol 179-181 ◽  
pp. 214-217 ◽  
Author(s):  
K. Niwase ◽  
K. Nakamura ◽  
I. Tanaka ◽  
Y. Miyamoto ◽  
T. Tanabe
2008 ◽  
Vol 373 (1-3) ◽  
pp. 119-122 ◽  
Author(s):  
T. Hirai ◽  
J. Compan ◽  
K. Niwase ◽  
J. Linke

2017 ◽  
Vol 72 (1) ◽  
pp. 37-47 ◽  
Author(s):  
Roger N. Bryant ◽  
Jill D. Pasteris ◽  
David A. Fike

Two probable causes of variability in the Raman spectrum of unpolished pyrite are well recognized, in principle, but not always in practice, namely: (1) downshifting of band positions due to laser heating; and (2) variations in the ratios of band intensities due to crystallographic orientation of the sample with respect to the laser’s dominant polarization plane. The aims of this paper are to determine whether these variations can be used to acquire additional information about pyrites. Here, using laser Raman microprobe analysis of natural, unpolished pyrite samples, we investigate the magnitude of downshifting of band positions associated with laser heating of different sizes of pyrite grains. We demonstrate that the magnitude of this effect can be large (up to ∼10 cm−1), negatively proportional to grain size, of greater magnitude than the effect typically attributable to natural intersample differences in trace element (TE) solid solution, and of similar magnitude among bands. Through Raman analysis of naturally occurring faces on pyrite samples at various angles of rotation, we also demonstrate that the three most common faces on pyrite can be distinguished by the ratio of the intensities of the dominant bands. We conclude that for unpolished samples, laser Raman microprobe analysis is most effective as a means of identifying pyrite, and the presence of solid solution therein, when laser power is low enough to avoid substantial heating. Once pyrite has been identified, higher laser powers can be used to produce spectra whose ratios of band intensities indicate the face or crystallographic plane being irradiated.


1984 ◽  
Vol 107 (2) ◽  
pp. 193-202 ◽  
Author(s):  
Nicole Guilhaumou ◽  
Bruce Velde ◽  
Claire Beny

1990 ◽  
Vol 54 (3) ◽  
pp. 535-543 ◽  
Author(s):  
I-Ming Chou ◽  
Jill Dill Pasteris ◽  
Jeffery C Seitz

Author(s):  
Barry E. Scheetz ◽  
William B. White ◽  
F. Adar
Keyword(s):  
Fly Ash ◽  

1990 ◽  
Vol 103 (1-4) ◽  
pp. 54-60 ◽  
Author(s):  
J. Jimenez ◽  
M.A. González ◽  
B. Martín ◽  
B. Calvo

1995 ◽  
Vol 396 ◽  
Author(s):  
A. L. Evelyn ◽  
D. Ila ◽  
J. Fisher ◽  
D. B. Poker

AbstractThe electronic and nuclear stopping effects produced by MeV ion bombardment in polyvinylidine chloride (PVDC) and polyethylene (PE) are separated by stacking thin films of the polymers. The resulting multi-layer laminates of each polymer were bombarded with 3.5 MeV alpha particles. The energy of the incident ions was selected, using TRIM, such that the first layers experienced most of the effects of the electronic energy deposited and the last layers received most of the effects of the nuclear stopping power. The changes in the conductance and the chemical structure of each layer were measured by direct resistivity measurements and Raman microprobe analysis.


1985 ◽  
Vol 51 ◽  
Author(s):  
P. M. Fauchet

ABSTRACTWe study the composition, stress and structure variations across periodic surface undulations produced by pulsed laser illumination of semiconductors, by explosive crystallization of amorphous films, and by laser-assisted CVD. These variations are mapped out with a one micron spatial resolution using a Raman microprobe. Similarities and differences between the three cases are pointed out. These results are also compared to those obtained by deliberately exposing the sample to interfering beams.


1982 ◽  
Vol 36 (1) ◽  
pp. 30-37 ◽  
Author(s):  
E. Payen ◽  
M. C. Dhamelincourt ◽  
P. Dhamelincourt ◽  
J. Grimblot ◽  
J. P. Bonnelle

Heating cells used in optical microscopy are adapted to a laser Raman microprobe to an under air study of the solid phase transformation of cobalt and nickel molybdates in which the molybdenum atoms are in tetrahedral oxygen environment ([a] phase) or in octahedral environment ([b] phase). In each case, the Co or Ni environment is octahedral. In the second part of this paper, a newly designed controlled-atmosphere and temperature cell is described. It permits the study of several problems particularly those related to the reactivity of Co or Ni-Mo-γ-Al2O3 hydrodesulfurization catalysts. Results on (1) sulfidation of the oxide precursor form catalysts by a H2-H2S mixture, (2) interaction with a model sulfided molecule: thiophene, and (3) pyridine chemisorption are reported.


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