Abstract
Paralleling the evolution of Fourier Transform Infrared Spectroscopy during the 1960’s and 1970’s there have been rapid developments in the area of Raman spectroscopy. The laser serves only in a secondary role for FT-IR spectroscopy, but as a source for excitation it has greatly revolutionized conventional Raman spectroscopy and led to the advent of new techniques including coherent anti-Stokes Raman scattering (CARS), Raman gain, inverse or hyper- Raman spectroscopy. Both FT-IR and Raman techniques have also benefited from the improvements in optoelectronic and data processing systems. While a moving mirror with high mechanical precision and a high quality beam splitter are basic to an FT-IR instrument, a double monochromator with precision gratings, which may be holographic, and a laser as light source are intrinsic to a Raman spectrometer. Improved detector systems (pyroelectric bolometers, such as triglycine sulfate, TGS, for FT-IR or photon counting for Raman), not available a decade ago now serve vital functions. Utilization of an on-line mini-computer is all but essential for practical FT-IR spectroscopy in order to facilitate the data handling and computation; it can also serve as a valuable accessory for the signal averaging and manipulation of Raman data.
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Kiefer, W., Laane, J. (1980). Comparison of FT-IR and Raman Spectroscopy. In: Durig, J.R. (eds) Analytical Applications of FT-IR to Molecular and Biological Systems. NATO Advanced Study Institutes Series, vol 57. Springer, Dordrecht. https://doi.org/10.1007/978-94-009-9070-8_26
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DOI: https://doi.org/10.1007/978-94-009-9070-8_26
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