Variability in the Raman Spectrum of Unpolished Growth and Fracture Surfaces of Pyrite Due to Laser Heating and Crystal Orientation

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.

1991 ◽  
Vol 179-181 ◽  
pp. 214-217 ◽  
Author(s):  
K. Niwase ◽  
K. Nakamura ◽  
I. Tanaka ◽  
Y. Miyamoto ◽  
T. Tanabe

1990 ◽  
Vol 201 ◽  
Author(s):  
Irving P. Herman ◽  
Hua Tang ◽  
Patrick P. Leong

AbstractOptical probing of laser-assisted chemical reactions on surfaces in real time can help explain and control these processes. Raman microprobe spectroscopy and micro laser induced fluorescence are the two optical probes employed here to investigate several examples of localized laser surface reactions. Raman microprobe analysis is used to monitor in real time the CuCl and CuCl2 products on the surface during local laser etching of copper films by Cl2 and the concomitant loss of the Cu2O passivation layer. It is also used to follow the production of Cu2O during the laser oxidation of Cu. Polarization Raman analysis is utilized to identify and analyze partially molten silicon during laser heating in vacuum and during the etching of silicon by chlorine. Laser induced fluorescence is used as a real time microprobe of desorbed products during local laser-assisted etching of Si and Al surfaces.


2008 ◽  
Vol 373 (1-3) ◽  
pp. 119-122 ◽  
Author(s):  
T. Hirai ◽  
J. Compan ◽  
K. Niwase ◽  
J. Linke

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

1998 ◽  
Vol 52 (3) ◽  
pp. 339-342 ◽  
Author(s):  
Katsuhiro Ajito

A combined Raman microprobe and laser trapping system using near-infrared (NIR) laser light was developed for the investigation of single organic microdroplets. The NIR laser light is noninvasive and reduces fluorescence interference in the Raman spectrum for organic molecules. The focused laser beam used for the laser trapping of a microdroplet serves simultaneously as the laser microprobe for Raman measurement. With this system, the focused laser spot is about 1 μm in diameter, which is small enough for the laser trapping of a single toluene microdroplet in water. The system also makes it possible to visualize a focused laser spot together with a laser-trapped microdroplet by using holographic notch filters. The Raman spectrum for a single laser-trapped toluene microdroplet can be obtained from below 100 cm−1 to above 3000 cm−1 with a charge-coupled device (CCD) detector. Fluorescence interference in the Raman spectrum is completely removed by using NIR laser light. The signal-to-noise ratio (SNR), defined as the ratio of the peak height to the standard deviation of the baseline noise in the spectrum, exceeded 250 for the 1003 cm−1 band of a toluene microdroplet at 1 s, which is sufficient to allow identification of the molecular species of a microdroplet.


1973 ◽  
Vol 6 (6) ◽  
pp. 347-352 ◽  
Author(s):  
Armen Galustian

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 ◽  

Sign in / Sign up

Export Citation Format

Share Document