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The split even Clifford algebra in signature (1,1)
Example
For signature , let with , . Then and . The two one-dimensional modules defined by are inequivalent irreducible real Clifford spinor representations of Spin, obtained by restricting the two unital even-Clifford modules.
Facts & Assumptions
Given: The Clifford relations and the real even-algebra module classification of Real Spin modules from the even Clifford algebra.
Full-even Spin consists of even normalized products, and its linear span is the even Clifford algebra (Normalized Pin products and Clifford norm, Real Spin modules from the even Clifford algebra).
A simple module for a split factor is one-dimensional over (Real Spin modules from the even Clifford algebra).
The ordered even Clifford monomials form a basis of (PBW basis and exterior associated graded for a Clifford algebra).
Verification
The polarized Clifford relation gives and hence . By [F3], form a basis of . The map preserves products and is bijective, so it identifies this algebra with .
The idempotents are the two factor identities. Let each factor act on by its scalar coordinate and the other factor by zero. Each module is one-dimensional and hence irreducible; they are inequivalent because acts by opposite scalars. By [F1], invariance under full-even Spin is equivalent to invariance under its linear span , so these are precisely the two split-row Clifford spinor types in this example.
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Sources
- M. F. Atiyah, R. Bott, and A. Shapiro, Clifford Modules, Part I (standard reference, not scraped)
- Konstantin Wernli, Lecture Notes on Spin Geometry, §1.5.4, pp. 32–33 (standard reference, not scraped)