scholarly journals Skeletal Range FT-IR Transmission Spectra of Submicron Commercial High Purity .ALPHA.-Al2O3 Powders Produced by Different Methods.

2000 ◽  
Vol 108 (1253) ◽  
pp. 1-5 ◽  
Author(s):  
Purwadi RAHARJO ◽  
Chanel ISHIZAKI ◽  
Kozo ISHIZAKI
1986 ◽  
Vol 40 (4) ◽  
pp. 427-434 ◽  
Author(s):  
John E. Bertie ◽  
R. Norman Jones ◽  
Victor Behnam

This paper completes the report of our FT-IR measurements of transmission spectra of organic liquids. These measurements were undertaken in order to estimate the photometric accuracy of our FT-IR spectrometer for transmission spectra by comparing the results with those measured previously [Applied Spectroscopy 34, 657 (1980)] by a calibrated dispersive spectrometer. We have studied 97 bands of chlorobenzene, toluene, and dichloromethane, in 500-μm cells and 54 bands of benzene, chlorobenzene, toluene, cyclopentane, and dichloromethane, in cells 11 to 53 μm thick. The average value of the imaginary refractive index at the band peak, kmax, is reported for each band and compared with the calibrated value. When averaged over the 184 bands that are reported in this work and our earlier paper [Applied Spectroscopy 39, 401 (1985)], our measurements agree with the calibrated values to about 3% of kmax, and have a 90% confidence limit of about 0.7 to 1% of kmax, The calibrated values themselves have an estimated error of about 6%, so to obtain better knowledge of the accuracy of our measurements we need better standards and we need measurements to be made on other FT-IR instruments. We plan to publish simplified procedures that will encourage others to make such measurements. Our 90% confidence limit includes effects due to the use of different cells, daily realignment of the fixed mirror of the interferometer, realignment of the optics of the detector and sample compartments, change of beamsplitter, and a day-to-day variation of uncertain origin, in addition to the error sources that always contribute to typical analytical precision. Our data do not show these additional error sources to be systematic, so it is appropriate to include their effect in the evaluation of the confidence limit. We believe the main source of error to be the effect of the infrared cell on the path of the light beam through the instrument. The day-to-day variation of uncertain origin is thought to be due to very small changes in the beam path through the instrument, which in turn cause the effect of the infrared cell on the beam to vary.


2012 ◽  
Vol 576 ◽  
pp. 619-622 ◽  
Author(s):  
Akbar Kaderi ◽  
Shahrul Razi Meskon ◽  
Hanafi Ani Mohd ◽  
Raihan Othman

Little information has been known on the initial – stage oxidation if there is water vapor involved. Cr samples of 10 mm × 10 mm × 1 mm were isothermally oxidized in dry and wet environment respectively for 86.4 ks. Compact and even surface of Cr2O3 was formed on samples oxidized in dry environment. However, the ability to form compact and even Cr2O3 was retarded in wet environment. XRD analysis on all samples shows that Cr2O3 can be formed in dry and wet environment. The IR transmission spectra for samples oxidized in dry environment, were consisting of more intense peak while samples oxidized in wet environment has more relaxed peak. Moreover the peak of samples oxidized in dry tends to be narrower, while samples oxidized in wet tend to have broader peak.


Author(s):  
Angelika Reklat ◽  
Waltraud Bessau ◽  
Anka Kohl

1989 ◽  
Vol 43 (3) ◽  
pp. 481-483 ◽  
Author(s):  
David D. Saperstein

The FT-IR transmission spectrum of 30 Å of a polyperfluoroethylene oxide lubricant on amorphous carbon is shown to be proportional to the transmission spectrum of a 0.4-μm film, and thus, there appears to be little or no interaction of the lubricant with amorphous carbon. These transmission spectra are dramatically different from the spectrum of the lubricant on a carbon-overcoated thin-film disk recorded at grazing incidence. The alteration of the grazing incidence reflection spectrum is due to polarization changes of the light when a strong absorber is measured near a reflecting surface.


1994 ◽  
Vol 66 (23) ◽  
pp. 4354-4358 ◽  
Author(s):  
Yoshimasa. Ogawara ◽  
Albert. Bruneau ◽  
Takako. Kimura

2011 ◽  
Vol 194-196 ◽  
pp. 594-597
Author(s):  
Ke Tang ◽  
Xin Hong ◽  
Jin Gang Qi

FAU-type(NaY) zeolites nanocrystals have been synthesized through crystallization of gel in mesoporous system of carbon nanotubes(CNTS) with a internal diameter of 20~30 nm. Investigation by using X-ray diffraction (XRD), Fourier transform infrared (FT-IR), transmission electron microscope (TEM) shows that the nanocrystals possess the typical nanosized zeolites structural characteristics which is different from those of microsized zeolites.


2014 ◽  
Vol 34 (7) ◽  
pp. 611-616 ◽  
Author(s):  
Shijie Cheng ◽  
Jun Xu ◽  
Yumin Wu

Abstract Oxidized starch-graft-poly(styrene-butyl acrylate) [OS-g-P(St-BA)] latex was synthesized by the graft copolymerization of OS with St and n-butyl acrylate (BA) via emulsion polymerization. The graft copolymers were characterized by Fourier transform infrared (FT-IR), transmission electronic microscopy (TEM), dynamic light scattering, thermogravimetry (TG), and differential scanning calorimetry (DSC). The effects of the amount of OS, monomers, and initiator on graft copolymerization were investigated. Under the optimal conditions, the percentage of graft (PG), grafting efficiency (GE), and ζ potential could reach 256.5%, 41.7%, and -30.1 mV, respectively. The results indicated that the OS grafted onto particles greatly enhanced the colloidal stability of latex. The thermal stability properties of OS-g-P(St-BA) were also improved by the addition of OS. The OS-g-P(St-BA) latex may be used to partly replace the conventional synthetic latex for paper coating.


1995 ◽  
Vol 49 (6) ◽  
pp. 819-824 ◽  
Author(s):  
Jun Shen ◽  
Andreas Mandelis ◽  
Andreas Othonos ◽  
Joseph Vanniasinkam

The recently developed photothermal technique of quadrature photopyroelectric spectroscopy (Q-PPES) has been applied to measurements of amorphous Si thin films deposited on crystalline Si substrates. Direct, meaningful comparisons have been made between purely optical transmission in-phase (IP-PPES) spectra, and purely thermal-wave sub-gap spectra with the use of a novel noncontacting PPES instrument to record lock-in in-phase and quadrature spectra, respectively. FT-IR transmission spectra have also been obtained for a comparison with this IP-PPES optical method. The results of the present work showed that the FT-IR method performs the worst in terms of spectral resolution of thin films and sub-bandgap defect/impurity absorptions inherent in the Si wafer substrate. The optical IP-PPES channel, however, albeit more sensitive than the FT-IR technique, fails to resolve spectra from surface films thinner than 2100 Å, but is sensitive to sub-bandgap absorptions. The thermal-wave Q-PPES channel is capable of resolving thin-film spectra well below 500 Å thick and exhibits strong signal levels from the crystalline Si sub-bandgap absorptions. Depending on the surface thin-film orientation toward, or away from, the direction of the incident radiation, the estimated minimum mean film thickness resolvable spectroscopically by Q-PPES is either 40 Å or 100 Å, respectively.


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