E. Libowitzky et Gr. Rossman, PRINCIPLES OF QUANTITATIVE ABSORBENCY MEASUREMENTS IN ANISOTROPIC CRYSTALS, Physics and chemistry of minerals, 23(6), 1996, pp. 319-327
The accurate measurement of absorbance (A=-log T; T=I/I-0) in anisotro
pic materials like crystals is highly important for the determination
of the concentration and orientation of the oscillator (absorber) unde
r investigation. The absorbance in isotropic material is linearly depe
ndent on the concentration of the absorber and on the thickness of the
sample (A=epsilon . c . t). Measurement of absorbance in anisotropic
media is more complicated, but it can be obtained from polarized spect
ra (i) on three random, but orthogonal sections of a crystal, or (ii)
preferably on two orthogonal sections oriented parallel to each of two
axes of the indicatrix ellipsoid. To compare among different crystal
classes (including cubic symmetry) it is useful to convert measured ab
sorbance values to one common basis (the total absorbance A,,,), where
in all absorbers are corrected as if they were aligned parallel to the
E-vector of the incident light. The total absorption coefficient (a(t
ot)=A(tot)/t) is calculated by (i) a(tot)=Sigma(i=1)(3)(a(max,i)+a(min
,i))/2, or by (ii) a(tot)=a(x)+a(y)+a(z). Only in special. circumstanc
es will unpolarized measurements of absorbance provide data useful for
quantitative studies of anisotropic material. The theoretical approac
h is confirmed by measurements on calcite and topaz. The orientation o
f the absorber with respect to the axes of the indicatrix ellipsoid is
calculated according to A(x)/A(tot)=cos(2) (x angle absorber), and an
alogously for A(y) and A(z). In this way, correct angles are obtained
for all cases of symmetry. The extinction ratio of the polarizer (Pe=I
-crossed/I-parallel) has considerable influence on the measured amplit
ude of absorption bands, especially in cases of strong anisotropic abs
orbance. However, if Pe is known, the true absorbance values can be ca
lculated even with polarizers of low extinction ratio, according to Am
ax=-log [(T-max,T-obs-0.5 . Pe . T-min,T-obs)/(1-0.5 . Pe)], and simil
ar for A(min).