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  • 1
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Review of Scientific Instruments 72 (2001), S. 4331-4336 
    ISSN: 1089-7623
    Source: AIP Digital Archive
    Topics: Physics , Electrical Engineering, Measurement and Control Technology
    Notes: The use of synchrotron radiation (SR) as a far- and mid-infrared source in the measurement of photoacoustic Fourier transform infrared spectra of solids is demonstrated for the first time in this work. Initial experiments were performed at beamline U10A at the National Synchrotron Light Source, Brookhaven National Laboratory. For synchrotron photoacoustic spectroscopy to be feasible, it must yield results superior to those obtained with a conventional thermal (Globar®) source; accordingly, SR and Globar® photoacoustic spectra recorded under similar conditions were compared in detail. The intensities of SR far-infrared photoacoustic spectra were found to be consistently greater than the corresponding Globar® spectra. At shorter wavelengths, SR always underfills the effective aperture (or, alternately, sample size); SR is a superior source in a spectral region that is a function of this aperture. The high wave number limit of this region exhibits a power-law dependence on aperture size. This investigation also showed that the entire mid-infrared photoacoustic spectrum is more intense using SR and apertures smaller than approximately 0.5 mm. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 4779-4789 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: In keeping with current theoretical activity concerning the OH and OD stretching bands of the carboxylic acids, we report the Raman spectra of gaseous formic acid-OD and formic acid-d1 for the first time. We emphasize the OH and OD stretching bands, which can be studied cleanly in these isotopomers but not in normal or perdeuterated formic acid. The spectra of the dimers and monomers below 2000 cm−1 are assigned, and current knowledge of the vibrations of the molecules is summarized. The Raman spectra allow the estimation of the energies of the Bu combination levels that may be in Fermi resonance with the infrared active Bu, OH or OD stretching fundamental, as well as those of the Ag overtone and combination levels that may interact with the Raman-active stretching fundamental. We conclude that the sharp features on the Raman OH and OD stretching bands are due to overtone and combination transitions, that the stretching modes cause the underlying broad scattering, namely three broad bands, centered at 2430, 2270, and 2080 cm−1 for (HCOOD)2 and at 3240, 3074, and 2880 cm−1 for (DCOOH)2. We further conclude that the higher and lower frequency broad bands are due to sum and difference transitions with the hydrogen bond modes, which lie between 60 and 240 cm−1. The infrared OD and OH stretching bands of (HCOOD)2 and (DCOOH)2 are consistent with this interpretation. The Raman OD stretching band of HCOOD ⋅ HCOOH coincides with that of (HCOOD)2 apart from the overtone and combination transitions. The centers of Raman intensity, corrected for instrument, wave number, and temperature dependencies, of the OD stretching bands of (HCOOD)2 and HCOOH ⋅ HCOOD are 2300 ±5 and 2305 ±10 cm−1, respectively, and that of the OH stretching band of (DCOOH)2 is 3035±10 cm−1. This data and the near coincidence of the infrared and Raman bands of (HCOOD)2 show that the vibrational coupling of the two OD bonds in the dimer is not unusually large. Comparison of the infrared and Raman OH stretching bands indicates a larger coupling between OH oscillators. These results agree with earlier result for acetic acid.
    Type of Medium: Electronic Resource
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