guide to thin section microscopy - Mineralogical Society of America
guide to thin section microscopy - Mineralogical Society of America
guide to thin section microscopy - Mineralogical Society of America
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Guide <strong>to</strong> Thin Section Microscopy<br />
Extinction<br />
Figure 4-45 B. Prismatic apatite showing negative sign <strong>of</strong> elongation. In apatite, the fast<br />
wave vibrates parallel <strong>to</strong> the slow wave <strong>of</strong> the first-order red plate, and the slow wave in<br />
apatite parallel <strong>to</strong> the fast wave <strong>of</strong> the first-order red plate. Hence, retardation is reduced and<br />
subtraction results (Γ res = Γ Red1 + Γ Ap = 476 nm; first-order orange-yellow).<br />
If the extinction direction deviates significantly from the long axis <strong>of</strong> the crystal <strong>section</strong>, it is<br />
convention <strong>to</strong> use the extinction position that forms an angle smaller than 45˚ with the long<br />
axis, and <strong>to</strong> rotate it in<strong>to</strong> the diagonal position before the first-order red plate or lambda/4<br />
plate is inserted for determining the sign <strong>of</strong> elongation. However, if extinction angles are<br />
close <strong>to</strong> 40-50˚, the use <strong>of</strong> l(+) and l(-) becomes impractical.<br />
Determination <strong>of</strong> the optic sign <strong>of</strong> optically uniaxial minerals<br />
Optically uniaxial minerals that are elongate in c direction (e.g., quartz, apatite, <strong>to</strong>urmaline)<br />
and are present in <strong>thin</strong> <strong>section</strong> in a cut that is roughly parallel <strong>to</strong> that long axis, will have the<br />
E-wave (n e ) vibrating parallel <strong>to</strong> c and the O-wave (n o ) orthogonal <strong>to</strong> c. If the habit <strong>of</strong><br />
optically uniaxial minerals is platy (e.g., melilite), the same applies, but the O-wave now<br />
vibrates parallel <strong>to</strong> the elongate <strong>section</strong>.<br />
Raith, Raase & Reinhardt – February 2012<br />
For both crystal habits, the optic sign can be determined easily by compensation, that is,<br />
whether n e > n o (= optically uniaxial positive) or n e < n o (= optically uniaxial negative) (Fig.<br />
4-46). The long axis <strong>of</strong> the crystal <strong>section</strong> is rotated in<strong>to</strong> diagonal position (NE-SW<br />
orientation), and the first-order red plate or lambda/4 plate is inserted. For crystals elongate in<br />
c, n e is now parallel <strong>to</strong> n zComp and n o is parallel <strong>to</strong> n xComp . For platy minerals, the relation is<br />
reverse as c is perpendicular <strong>to</strong> the long dimension <strong>of</strong> the crystal <strong>section</strong>s. The retardation<br />
between the waves which are created in the optically uniaxial mineral (Γ Min ) and in the<br />
compensa<strong>to</strong>r plate will be increased through addition or decreased through subtraction,<br />
depending on optical sign. Correspondingly, the crystal <strong>section</strong> shows higher or lower<br />
interference colours if the compensa<strong>to</strong>r is inserted.<br />
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