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guide to thin section microscopy - Mineralogical Society of America

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Guide <strong>to</strong> Thin Section Microscopy<br />

Double refraction<br />

4.2.3.1 Observation without analyzer (plane-polarized light mode)<br />

In plane-polarized light, anisotropic minerals can only be distinguished from isotropic<br />

minerals if characteristic grain shapes are observed (e.g., elongate or platy habit), if the grains<br />

display relief changes such as chagrin contrast as the stage is turned (only in minerals with<br />

large differences in n z ' and n x '), or if the absorption colour changes with changing orientation<br />

(pleochroism).<br />

The birefringence (∆n) <strong>of</strong> minerals is commonly not large enough <strong>to</strong> create distinct chagrin<br />

effects, with the exception <strong>of</strong> carbonates. Fig. 4-22 shows the striking change <strong>of</strong> chagrin in<br />

calcite and dolomite due <strong>to</strong> their extreme birefringence (∆n = 0.172 Cal resp. 0.177 Dol ).<br />

Figure 4-22. Change <strong>of</strong> chagrin in calcite and dolomite during a 360˚ rotation <strong>of</strong> the stage.<br />

Crystal <strong>section</strong>s are oriented parallel <strong>to</strong> the c axis. Shown are the four positions where the vibration<br />

directions <strong>of</strong> the two waves in the crystal coincide exactly with the polarizer directions. In these<br />

positions, only the E-W vibrating wave is passing through the crystal. The large difference between the<br />

refractive indices <strong>of</strong> the O- and E-waves causes the change in chagrin (∆n = 0.172 Cal resp. 0.177 Dol ).<br />

The majority <strong>of</strong> minerals show no or very little pleochroism. Exceptions include <strong>to</strong>urmaline,<br />

members <strong>of</strong> the amphibole group, Fe-Ti-rich biotites as well as less common minerals such as<br />

piemontite, sapphirine, dumortierite, yoderite and lazulite (Fig. 4-10).<br />

Raith, Raase & Reinhardt – February 2012<br />

Pleochroic minerals <strong>of</strong> tetragonal, hexagonal and trigonal symmetry show two characteristic<br />

absorption colours parallel <strong>to</strong> the vibration directions <strong>of</strong> the E- and O-waves (dichroism).<br />

Crystal <strong>section</strong>s normal <strong>to</strong> the crystallographic c-axis (= optic axis) only show the absorption<br />

colour <strong>of</strong> the O-wave as the stage is rotated. Crystal <strong>section</strong>s parallel <strong>to</strong> the c-axis show an<br />

alternation between the absorption colour <strong>of</strong> the E-wave (E-W orientation <strong>of</strong> c) and the O-<br />

wave (N-S orientation <strong>of</strong> c) every 90˚ during stage rotation (Ch. 4.2.1, Figs. 4-11,12).<br />

Pleochroic minerals <strong>of</strong> orthorhombic, monoclinic and triclinic symmetry show three<br />

characteristic absorption colours parallel <strong>to</strong> the principal indicatrix axes X, Y and Z<br />

(trichroism). Crystal <strong>section</strong>s normal <strong>to</strong> one <strong>of</strong> the two optic axes show the absorption colour<br />

<strong>of</strong> the Y vibration direction as the stage is rotated. An identification <strong>of</strong> the absorption colours<br />

in the X, Y and Z directions requires specific crystal <strong>section</strong>s (Ch. 4.2.1, Figs. 4-14−17).<br />

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