The volume element and even part of the split real Clifford plane #
In the matrix model of Cliff(1, 1), the product z = e₁ e₂ of the coordinate generators is
the swap matrix. It satisfies z² = 1, reverse z = -z, and star z = -z. The even Clifford
algebra consists of the elements a + b z, uniquely, represented by the matrices !![a, b; b, a].
These are Clifford algebra computations independent of the Spin group and its hyperbolic parametrization. Both Bott periodicity and the Spin classification use this general layer.
Main definitions and results #
TauCeti.realCliffordOneOneEquivMatrix_e₀_mul_e₁: the coordinate-generator product is the swap matrix.TauCeti.realCliffordOneOneVolume: the volume element, with defining equationTauCeti.realCliffordOneOneVolume_def.TauCeti.mem_even_realCliffordOneOne_iff: the even part consists of the elementsa + b z.TauCeti.algebraMap_add_smul_realCliffordOneOneVolume_inj: these coordinates are unique.
References #
- H. B. Lawson and M.-L. Michelsohn, Spin Geometry (1989), Chapter I, §2.
The two coordinate generators of Cliff(1, 1) multiply to the swap matrix.
The product z = e₁ e₂ of the two coordinate generators of Cliff(1, 1), the generator e₁
squaring to 1 and e₂ to -1.
Instances For
The volume element is the product of the positive and negative coordinate generators.
In the matrix model of Cliff(1, 1), a + b z is the matrix !![a, b; b, a].
Multiplication in the even plane ℝ + ℝ z, where z² = 1.
z is even: the grade involution fixes it.
z lies in the even part of Cliff(1, 1).
The coefficients a and b of a + b z are unique.
The even part of Cliff(1, 1). Every even element is a + b z for some real a, b.
The even part of Cliff(1, 1) consists of the elements a + b z.
The Clifford conjugate of a + b z is a - b z.