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Figure 3
Reorientation of a sample about the κ or φ axis of an inverse-κ system. The sample's initial position is defined in motor coordinate space by [{{\bi t}_{{\psi _1}}}]. The sample is rotated about [{\bf{d}}_\Psi ^0], where [\Psi \in \left\{ {{\rm K},\Phi } \right\}], by [{\psi _2} - {\psi _1}] (1). Subsequent translation to the motor position coordinates [{{\bi t}_{{\psi _2}}}] restores the sample to the centre without further changing its orientation (2).

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