July 1997
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5 Reads
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3 Citations
Optics Communications
By expanding Fresnel's formulae in McLaurin's series of the extinction coefficient (k2), expressions for the absorbances in the ATR spectra are obtained. It is shown that in the case of weak absorption the absorbance values are directly proportional to the values of the imaginary part of the dielectric constant (ε''2). Thus, the ATR spectra obtained under conditions of weak absorption are, in effect, dependences of ε''2 on the frequency (nu). It is also shown that the use of the effective thickness concept, introduced by Harrick, leads to an incorrect physical interpretation of the ATR spectra. Namely, they are considered as frequency dependences of the Lambert absorption coefficient (alpha2) that are somewhat distorted due to anomalous dispersion. It is found that there are three reasons which cause differences between ATR and transmission spectra. The relative contribution of each of them is illustrated on the absorption band with a maximum at nu0 = 3400 cm-1, assigned to the stretching vibration of water molecules. The anomalous dispersion influence is also demonstrated on the benzene absorption band with a maximum at nu0 = 1035 cm-1.