The spins in a ferromagnet define a vector field. Their simplest line singularities are therefore disclinations of unit strength, and their point singularities are of the types analysed by Poincaré. A nematic liquid crystal is normally unpolarised. As a result, a vector placed along the nematic axis at a point may be carried continuously through « good » liquid crystal and return inverted. The simplest line singularities are therefore disclinations of half unit strength. A double circuit restores the vector to its original orientation. The director field thus has the character of the wave function of a spinor. The extension of this idea to three dimensions allows a preliminary description of the point singularities of nematic structures.
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F. R. N. Nabarro (1972) studied this question.
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