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TauCeti.LinearAlgebra.CliffordAlgebra.VolumeElement.Complex

The normalized complex volume element of an oriented Euclidean space #

Let V be an oriented real inner product space of dimension n and Q a quadratic form on V. For the geometric convention Q v = -‖v‖², so that c(v) c(w) + c(w) c(v) = -2 ⟪v, w⟫, the normalized complex volume element is

Γ = i ^ ⌊(n + 1) / 2⌋ c(e₁) ⋯ c(eₙ)

in the complexified Clifford algebra Cℓ(ℂ ⊗ V, Q_ℂ), for any positively oriented orthonormal basis e. It is defined without a frame, as i ^ ⌊(n + 1) / 2⌋ times the image of the real volume element CliffordAlgebra.volumeElement Q o, so the frame formula CliffordAlgebra.complexVolume_eq is its independence under orientation-preserving orthonormal changes of frame, and reversing the orientation changes its sign.

In even dimension n = 2ℓ this is Γ = i ^ ℓ c(e₁) ⋯ c(e₂ₗ), the chirality operator: it anticommutes with every vector, so its ±1 eigenspaces in a Clifford module are exchanged by Clifford multiplication, and conjugation by Γ is the grade involution. In odd dimension n = 2ℓ + 1 it is ω_ℂ = i ^ (ℓ + 1) c(e₁) ⋯ c(eₙ), a central element whose ±1 eigenspaces separate the two irreducible Clifford modules. The power of i is chosen so that Γ squares to 1 and is fixed by the conjugate-linear Clifford involution CliffordAlgebra.conjStar, so that it acts as a self-adjoint involution in every *-representation. The complex-linear Clifford conjugation star instead multiplies it by (-1) ^ ⌊(n + 1) / 2⌋. In rank zero, Γ is 1 for the positive orientation and -1 for the negative one.

Main definitions #

Main results #

Only the statements involving Γ² assume Q v = -‖v‖²; the others hold for every Q.

References #

The normalized complex volume element Γ = i ^ ⌊(n + 1) / 2⌋ c(e₁) ⋯ c(eₙ) of the complexified Clifford algebra of an oriented real inner product space of dimension n, for any positively oriented orthonormal basis e that is orthogonal for Q (CliffordAlgebra.complexVolume_eq). It is fixed by CliffordAlgebra.conjStar; in even dimension it anticommutes with every vector, and in odd dimension it is central. For Q v = -‖v‖² it squares to 1, so in even dimension it is the chirality operator.

Instances For

    The real volume element is (-i) ^ ⌊(n + 1) / 2⌋ Γ in the complexified Clifford algebra; in dimension two it is -i Γ.

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    Reversing the orientation negates the normalized complex volume element.

    Frame independence of Γ: Γ = i ^ ⌊(n + 1) / 2⌋ c(e₁) ⋯ c(eₙ) for every positively oriented orthonormal basis e that is orthogonal for Q, for instance for Q v = -‖v‖² (OrthonormalBasis.isOrthoᵢ_associated).

    Γ as a product of adjacent pairs: in dimension 2ℓ, Γ = i ^ ℓ (c(e₁) c(e₂)) ⋯ (c(e₂ℓ₋₁) c(e₂ℓ)) for every positively oriented orthonormal basis e that is orthogonal for Q.

    ω_ℂ as a product of adjacent pairs and a last vector: in dimension 2ℓ + 1, ω_ℂ = i ^ (ℓ + 1) (c(e₁) c(e₂)) ⋯ (c(e₂ℓ₋₁) c(e₂ℓ)) c(e₂ℓ₊₁) for every positively oriented orthonormal basis e that is orthogonal for Q.

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    The normalized complex volume element in rank zero: for the positive orientation of a zero-dimensional space, Γ = 1. By CliffordAlgebra.complexVolume_neg_orientation, the negative orientation gives Γ = -1.

    Naturality of Γ: the complexification of an isometric equivalence e of the quadratic forms that also preserves the norms carries Γ for o to Γ for the transported orientation. In particular an orientation-preserving isometry of V fixing Q fixes Γ, while an orientation-reversing one negates it (CliffordAlgebra.complexVolume_neg_orientation).

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    The grade involution multiplies Γ by (-1) ^ n.

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    Reversal multiplies Γ by (-1) ^ ⌊n / 2⌋.

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    Complex-linear Clifford conjugation multiplies Γ by (-1) ^ ⌊(n + 1) / 2⌋; in dimension 2ℓ this is star Γ = (-1) ^ ℓ Γ.

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    Complex conjugation of the coefficients multiplies Γ by (-1) ^ ⌊(n + 1) / 2⌋.

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    Γ is self-adjoint: it is fixed by the conjugate-linear Clifford involution CliffordAlgebra.conjStar, so it acts self-adjointly in every *-representation.

    In even dimension Γ anticommutes with every vector: Γ c(w) = -c(w) Γ.

    In even dimension Γ intertwines the grade involution: Γ x = involute x Γ.

    In even dimension Γ anticommutes with every odd element.

    Γ commutes with every even element, in every dimension: in even dimension Γ intertwines the grade involution, and in odd dimension Γ is central.

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    Γ is an involution: Γ² = 1.

    Γ acts as an involution on every module: Γ • Γ • ψ = ψ.

    In even dimension, conjugation by Γ is the grade involution: Γ x Γ = involute x.