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 />
The colour shift <strong>to</strong> a lower order is not always easily identified in minerals with high<br />
birefringence and interference colours <strong>of</strong> the 3 rd or higher order, particularly for the novice. In<br />
such cases, the quartz wedge may be used instead <strong>of</strong> the first-order red plate. By inserting the<br />
quartz wedge, the continuous change <strong>of</strong> the interference colours <strong>to</strong>wards more saturated hues<br />
can be observed while the colours shift <strong>to</strong> lower orders. In minerals with low birefringence<br />
first-order black is reached initially. With further insertion <strong>of</strong> the quartz wedge, the colour<br />
sequence reverts <strong>to</strong> increasing interference colours (e.g., olivine and white mica). At <strong>thin</strong>ningout<br />
crystal plate edges, the colour bands move <strong>to</strong>wards the grain interior as the quartz wedge<br />
is inserted (Fig. 4-44). This effect is particularly evident from the red <strong>to</strong>nes <strong>of</strong> the first, second<br />
and third order. The dark grey colour band <strong>of</strong> the first order at the outermost edge <strong>of</strong> the<br />
mineral migrates in<strong>to</strong> the grain interior and is replaced by colours <strong>of</strong> the first <strong>to</strong> third order, if<br />
the interference colours <strong>of</strong> the mineral lie in the first <strong>to</strong> second order (e.g., olivine, white<br />
mica, pyroxenes).<br />
Interpretation:<br />
In an anisotropic mineral, the n x ' wave advances faster in the crystal plate than the n z ' wave.<br />
Both waves have different wavelengths. After exciting the mineral, both waves have the same<br />
velocity and wavelength, but with an accumulated retardation <strong>of</strong> Γ Min = d * (n z ' – n x ').<br />
With this retardation, the waves enter the crystal plate in the compensa<strong>to</strong>r in which the fast<br />
and slow wave directions are at 90˚ <strong>to</strong> those <strong>of</strong> the mineral. The mineral's n x ' wave now<br />
becomes the slower wave n zComp , the original n z ' wave transforms <strong>to</strong> the faster wave n xComp .<br />
Therefore, the retardation accumulated in the mineral is now reduced by the retardation <strong>of</strong> the<br />
compensa<strong>to</strong>r. There is a decrease <strong>of</strong> interference colours:<br />
Γ Min – Γ Comp = Γ <strong>to</strong>tal .<br />
When inserting the first-order red plate or the quartz wedge, the following is <strong>to</strong> be noted:<br />
1. If the retardation <strong>of</strong> the mineral is larger than that <strong>of</strong> the compensa<strong>to</strong>r, only decreasing<br />
colours <strong>of</strong> a lower order are observed.<br />
2. If the retardation <strong>of</strong> the mineral is the same as that <strong>of</strong> the compensa<strong>to</strong>r, the mineral appears<br />
in first-order black (Γ <strong>to</strong>tal = 0). The retardation <strong>of</strong> the mineral is fully compensated.<br />
Raith, Raase & Reinhardt – February 2012<br />
3. If the retardation <strong>of</strong> the mineral is smaller than that <strong>of</strong> the compensa<strong>to</strong>r, the interference<br />
colour are reduced <strong>to</strong> a value corresponding <strong>to</strong> the difference Γ Comp – Γ Min . When inserting the<br />
quartz wedge, decreasing colours will be observed initially, down <strong>to</strong> first-order black, after<br />
which colours will increase again.<br />
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