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Lecture handout including QS - Department of Materials Science ...

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BH12 Course B: <strong>Materials</strong> for Devices BH12<br />

A sample <strong>of</strong> nematic LC will not necessarily have a single, uniform director across its whole volume,<br />

but instead may be broken down into smaller, differently oriented regions, or domains.<br />

Where differently oriented domains meet there is<br />

a ‘glitch’, called a disclination. Observation <strong>of</strong> a<br />

LC sample between crossed polars typically<br />

shows a schlieren texture: bright regions <strong>of</strong><br />

nematic LC with uniform director, separated by<br />

dark boundary regions where the director is<br />

aligned with the polarizer or analyzer (or is<br />

parallel to the light path), and hence the sample is<br />

in extinction.<br />

Further types <strong>of</strong> Liquid Crystals<br />

There are several different classes <strong>of</strong> LC, based upon their overall tendency for molecular alignment.<br />

Smectic: molecules organise into layers<br />

⇒ orientational order, some positional order<br />

Chiral nematic: helical twist<br />

Smectic A<br />

D parallel to<br />

layer normal<br />

Smectic C<br />

↑<br />

D<br />

D<br />

D<br />

The molecules in a Chiral Nematic (also called cholesteric) have their long axes (and hence director)<br />

in a plane (in the above, this is shown as the horizontal); the director rotates along the axis perpendicular<br />

to this plane, tracing out a helix. For polarized light propagating along this axis, the plane <strong>of</strong><br />

polarization rotates with D. The pitch is the distance along the axis taken for a complete 360° rotation<br />

<strong>of</strong> the director. It can vary over a very wide range, e.g. ~100 nm - 100 µm, depending upon the LC<br />

molecules involved, the degree <strong>of</strong> polymerization, and the concentration in solution.

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