<math>\begin{align}   & \left\{ \begin{align}   & m{\alpha }'\tau \hbar \varepsilon \mu \alpha \mathbf{T}ic\varsigma  \\   & \text{      }\And  \\   & \text{  }\mathsf{\mathcal{P}}\pi y\sigma \mathbf{I}\subset \mathbf{S} \\  \end{align} \right\} \\   & \text{    }Wikia \\  \end{align}</math>


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A Twistor is a pair of two-component Spinors - one transforming in the fundamental representation of SL(2,C), the other in the conjugate representation - which corresponds (via a "twistor correspondence") to a null line in Minkowski space. The space of such objects is called Twistor Space, and provides an important alternative description of many mathematical objects used in physics.

SupertwistorsEdit this section

A supertwistor is a twistor with some Grassmann Variables added. The space of supertwistors with \mathcal{N} Grassmann components is denoted CP^{3|\mathcal{N}}. (e.g. see section 6.4 of [1])

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