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The split even Clifford algebra in signature (1,1)

Example

For signature (1,1), let E=e+e− with e+2=1, e−2=−1. Then E2=1 and Cl1,10≅R⊕R. The two one-dimensional modules M± defined by E⋅t=±t are inequivalent irreducible real Clifford spinor representations of Spin, obtained by restricting the two unital even-Clifford modules.

Facts & Assumptions

Given: The (1,1) Clifford relations and the real even-algebra module classification of Real Spin modules from the even Clifford algebra.

[F1]

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).

[F2]

A simple module for a split factor R is one-dimensional over R (Real Spin modules from the even Clifford algebra).

[F3]

The ordered even Clifford monomials form a basis of Cl0 (PBW basis and exterior associated graded for a Clifford algebra).

Verification

technique · direct
1.1givenF3algebra

The polarized Clifford relation gives e+e−=−e−e+ and hence E2=−e+2e−2=1. By [F3], 1,E form a basis of Cl1,10. The map a+bE↦(a+b,a−b) preserves products and is bijective, so it identifies this algebra with R⊕R.

2.1F1F2step 1.1algebra∎

The idempotents p±=(1±E)/2 are the two factor identities. Let each factor act on R by its scalar coordinate and the other factor by zero. Each module is one-dimensional and hence irreducible; they are inequivalent because E acts by opposite scalars. By [F1], invariance under full-even Spin is equivalent to invariance under its linear span Cl0, so these are precisely the two split-row Clifford spinor types in this example.

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