Definition

Let

Δ=Δ+Δ\Delta=\Delta^+\oplus\Delta^-

be an even-dimensional complex spinor module, and let JJ be a that preserves each half-spin module:

J(Δ±)Δ±.J(\Delta^\pm)\subseteq\Delta^\pm.

A Majorana–Weyl spinor of positive or negative chirality is a spinor ψΔ±\psi\in\Delta^\pm such that

Jψ=ψ.J\psi=\psi.

It is therefore simultaneously a and a Majorana spinor.

The definition is available only when the dimension and signature admit a real structure compatible with the chiral decomposition. The existence of a Majorana condition and the existence of Weyl spinors separately do not imply that the two conditions are compatible.

References
  1. Pierre Deligne, “Notes on spinors,” in Quantum Fields and Strings: A Course for Mathematicians, Volume 1, American Mathematical Society, 1999, pp. 99–135.
  2. Daniel S. Freed, Five Lectures on Supersymmetry, American Mathematical Society, 1999. Relevant: Lectures 1–2.