Abstract
The primary requirement for transport of radiation through a material media is to have estimates for the absorption coefficients at the appropriate wavelengths. For many applications, the appropriate wavelengths are determined by the temperature of the material in question. In many other cases where the source of radiation is not characterized by the local temperature, one needs a versatile source of radiation continuously covering a wavelength interval appropriate for the problem at hand.
© 1988 Optical Society of America
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