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 #
CliffordAlgebra.complexVolume Q o: the normalized complex volume elementΓofCliffordAlgebra (Q.baseChange ℂ).
Main results #
CliffordAlgebra.complexVolume_eq:Γ = i ^ ⌊(n + 1) / 2⌋ c(e₁) ⋯ c(eₙ)for every positively oriented orthonormal basisethat is orthogonal forQ, andCliffordAlgebra.complexVolume_eq_prod_pairs: in dimension2ℓit groups asΓ = i ^ ℓ (c(e₁) c(e₂)) ⋯ (c(e₂ℓ₋₁) c(e₂ℓ)), whileCliffordAlgebra.complexVolume_eq_prod_pairs_mul: in dimension2ℓ + 1it groups asω_ℂ = i ^ (ℓ + 1) (c(e₁) c(e₂)) ⋯ (c(e₂ℓ₋₁) c(e₂ℓ)) c(e₂ℓ₊₁).CliffordAlgebra.ofBaseChangeAux_volumeElement: conversely, the real volume element is(-i) ^ ⌊(n + 1) / 2⌋ Γ.CliffordAlgebra.complexVolume_neg_orientation: reversing the orientation negatesΓ, andCliffordAlgebra.complexVolume_positiveOrientation: in rank zero,Γ = 1.CliffordAlgebra.map_complexVolume: the complexification of an isometry of quadratic forms that also preserves the norms carriesΓtoΓfor the transported orientation.CliffordAlgebra.complexVolume_mul_self:Γ² = 1forQ v = -‖v‖².CliffordAlgebra.complexVolume_smul_complexVolume_smul,CliffordAlgebra.lsmul_complexVolume_involutive:Γacts as an involution on every module.CliffordAlgebra.conjStar_complexVolume:Γis fixed by the conjugate-linear Clifford involution, whileCliffordAlgebra.star_complexVolumecomputes the complex-linear Clifford conjugationstar Γ = (-1) ^ ⌊(n + 1) / 2⌋ Γ; in dimension2ℓthis is(-1) ^ ℓ Γ.CliffordAlgebra.complexVolume_mul_eq_involute_mul: in even dimension,Γ x = involute x Γ; henceΓanticommutes with odd elements (CliffordAlgebra.complexVolume_mul_of_mem_odd), in particular with vectors (CliffordAlgebra.complexVolume_mul_ι_of_even). ForQ v = -‖v‖², conjugation byΓis the grade involution (CliffordAlgebra.complexVolume_mul_mul_complexVolume).CliffordAlgebra.complexVolume_mem_center: in odd dimension,Γis central.CliffordAlgebra.commute_complexVolume_of_mem_even: in every dimension,Γcommutes with even elements.
Only the statements involving Γ² assume Q v = -‖v‖²; the others hold for every Q.
References #
- H. B. Lawson and M.-L. Michelsohn, Spin Geometry (1989), Chapter I, §5.
- L. Nicolaescu, Lectures on the Geometry of Manifolds, the chapter on Clifford modules.
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
Unfolding lemma for CliffordAlgebra.complexVolume.
The real volume element is (-i) ^ ⌊(n + 1) / 2⌋ Γ in the complexified Clifford algebra; in
dimension two it is -i Γ.
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.
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).
The grade involution multiplies Γ by (-1) ^ n.
Reversal multiplies Γ by (-1) ^ ⌊n / 2⌋.
Complex-linear Clifford conjugation multiplies Γ by (-1) ^ ⌊(n + 1) / 2⌋; in dimension
2ℓ this is star Γ = (-1) ^ ℓ Γ.
Complex conjugation of the coefficients multiplies Γ by (-1) ^ ⌊(n + 1) / 2⌋.
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.
In odd dimension Γ commutes with every vector.
In odd dimension Γ is central.
Γ commutes with every even element, in every dimension: in even dimension Γ intertwines the
grade involution, and in odd dimension Γ is central.
Γ is an involution: Γ² = 1.
Γ acts as an involution on every module: Γ • Γ • ψ = ψ.
Multiplication by Γ is an involution of every module.
In even dimension, conjugation by Γ is the grade involution: Γ x Γ = involute x.