Definition

Let (V,q)(V,q) be a finite-dimensional nondegenerate real or complex quadratic space. A spinor module Δ\Delta is a specified for the corresponding real, complex, or complexified , usually chosen irreducible in the relevant module category. Since the lies in the group of units of the even Clifford algebra, the Clifford action restricts to a representation

ρ:Spin(V,q)GL(Δ),\rho:\operatorname{Spin}(V,q)\longrightarrow\operatorname{GL}(\Delta),

called a spin representation.

Irreducibility and scalar field

The phrase “a spinor module” does not specify a unique module until the scalar field, signature, grading convention, and irreducibility condition have been fixed. Over C\mathbb C, the possibilities are described by the . Over R\mathbb R, the answer depends on the signature modulo 88.

These choices also determine which additional spinor conditions exist. A is complex, a has a specified chirality, and and use compatible real structures. These are distinct definitions rather than interchangeable names for elements of Δ\Delta.

From modules to bundles

Given a on a manifold, a chosen spinor module produces the by the associated-bundle construction. Clifford multiplication then acts fiberwise, and a lifted metric connection yields the corresponding .

References
  1. H. Blaine Lawson Jr. and Marie-Louise Michelsohn, Spin Geometry, Princeton University Press, 1989. DOI record. Relevant: Chapter I, Sections 4–5.
  2. Daniel S. Freed, Five Lectures on Supersymmetry, American Mathematical Society, 1999. Relevant: Lectures 1–2.
  3. Pierre Deligne, “Notes on spinors,” in Quantum Fields and Strings: A Course for Mathematicians, Volume 1, American Mathematical Society, 1999, pp. 99–135. Relevant: signature-dependent real and complex spinors.