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Real and complex Clifford algebra classification with explicit signature
Statement
Let , let be the residue of modulo in , and use with signature ordered . For every nondegenerate real form of signature , the real Clifford algebra is
| parity of | ||
|---|---|---|
| even | ||
| odd | ||
| even | ||
| odd | ||
| even | ||
| odd | ||
| even | ||
| odd |
Only signatures with are considered; in the feasible rows the displayed exponents are nonnegative. For a nondegenerate complex quadratic form on dimension , its Clifford algebra is
These matrix-algebra classifications require nondegeneracy; no such classification is asserted for degenerate forms.
Facts & Assumptions
Given: A finite-dimensional nondegenerate real or complex symmetric bilinear form, with associated quadratic form , and the Clifford convention .
Every finite-dimensional real symmetric form is congruent to exactly one (Sylvester's law of inertia: every real symmetric form is congruent to , and is unique).
The real pure-signature table, signature recurrences, and pure eightfold periodicity are proved in Real Clifford signature recurrences and eightfold periodicity.
The coefficient identities include , , , and (Tensor identities for the real division algebras).
Every complex scalar has a square root (Every complex number has a square root, by an explicit Cartesian formula).
A linear isometry of quadratic spaces induces a Clifford algebra homomorphism by the universal property (Universal property of the Clifford algebra).
The Clifford algebra of an -dimensional space has dimension , with the ordered square-free monomial basis (PBW basis and exterior associated graded for a Clifford algebra).
The plus- Clifford algebra is the quotient of the tensor algebra by the relations (Universal Clifford algebra of a quadratic space).
is a field containing the embedded real field, and has characteristic zero, so has characteristic zero ( is a field, every element is uniquely , and every nonzero element has inverse , The reals form a totally ordered field).
A real-bilinear map from two real vector spaces induces a unique linear map from their tensor product (Universal property of the tensor product for balanced maps into abelian groups).
The flip of ordinary tensor factors sends to (Symmetry and associativity isomorphisms for tensor products over a commutative ring).
Tensoring with a fixed module commutes with direct sums (Tensor products commute with arbitrary direct sums).
is a tensor unit: (The regular module is a tensor unit: and ).
Proof
By [F1], a nondegenerate real form of signature has an orthogonal basis with squares and squares . In the quotient convention [F7], the linear isometry from this standard form to the given form induces a Clifford homomorphism by [F5]; applying [F5] to the inverse isometry gives its inverse, since both composites fix every canonical generator. Thus it suffices to classify the standard .
Let . Repeatedly applying the first recurrence in [F2] removes one positive and one negative generator at a time, giving when , and when . If the remaining pure dimension is with , [F2] replaces its -part by a factor .
Let be a nondegenerate symmetric complex bilinear form on a positive-dimensional complex vector space. Some vector has : otherwise polarization, valid because is invertible by [F8], would give , contradicting nondegeneracy. By [F4], rescale so that . Then every decomposes as with the second term in , so and . The restriction to is nondegenerate, since a vector in its radical is orthogonal to both and , hence to all of . Induction therefore gives an orthogonal basis with every square , so all nondegenerate complex forms of dimension are isometric to the standard one.
If , the PBW basis from [F6] consists only of the unit, so the scalar map is an isomorphism: it is nonzero and hence injective, and both sides have complex dimension one.
For , the pure positive column in [F2] supplies, for residues , coefficient types , , , , , , , , with matrix-size exponents respectively , , , , , , , . Since , these are exactly the exponents in the table of the Statement. For , apply the negative pure column of [F2] with and ; its eight residue rows give respectively residues and matrix-size exponents , , , , , , , . Substituting again gives precisely the displayed real table, including the split rows.
Suppose . The real generator map into the complex Clifford algebra satisfies the same squares, so [F5] extends it to a real-algebra homomorphism . The real-bilinear map induces by [F9] a linear map , . It is multiplicative because complex scalars are central in the target: . Its image contains the complex scalars and all complex Clifford generators, so it is surjective; both sides have complex dimension by [F6], making it an isomorphism. For a real matrix factor, [F3] gives . The coefficient algebra changes as follows: by the tensor-unit map [F12], which preserves products; and by [F3]; and by the flip [F10], which is multiplicative since it sends to . The direct-sum isomorphism [F11] preserves componentwise products, so split rows remain two factors. Thus real residue rows remain single -matrix factors of the same size; rows replace each by , doubling the matrix size; rows remain split into two factors, with the matrix size doubled; and rows split because . Substituting the real table sizes in [F2] gives one factor for even and two factors for odd . Together with step 1.3, this classifies every nondegenerate complex form.
Depends on
- Real, complex, and quaternion coefficient algebras and matrix notation
- Universal Clifford algebra of a quadratic space
- Universal property of the Clifford algebra
- Real Clifford signature recurrences and eightfold periodicity
- Tensor identities for the real division algebras
- PBW basis and exterior associated graded for a Clifford algebra
- Sylvester's law of inertia: every real symmetric form is congruent to $\operatorname{diag}(I_p,-I_q,0_r)$, and $(p,q,r)$ is unique
- Every complex number has a square root, by an explicit Cartesian formula
- $\mathbb C=\mathbb R[x]/(x^2+1)$ is a field, every element is uniquely $a+bi$, and every nonzero element has inverse $(a-bi)/(a^2+b^2)$
- The reals form a totally ordered field
- Universal property of the tensor product for balanced maps into abelian groups
- Symmetry and associativity isomorphisms for tensor products over a commutative ring
- Tensor products commute with arbitrary direct sums
- The regular module is a tensor unit: $R\otimes_RN\cong N$ and $M\otimes_RR\cong M$
Used by
- The twisted Spin Dirac index is the integral of A-hat times ch(E) Corollary
- Even-dimensional spinor bundles, chirality, and the spin connection Definition
- Fourier modes give index zero for the periodic flat even torus Example
- Low-signature real Clifford algebras as C, H, and matrix algebras Example
- Positive Clifford mass differences give the actual KO classes Lemma
- Real Clifford block-rotation index bounds Lemma
- Restriction matrices for negative-square graded real Clifford modules Lemma
- Spinor and geometric Clifford bundles and connections are well defined Lemma
- Ungraded real and quaternionic spinor Morita evaluation Lemma
- Antiunitary AZ symmetry classes give Clifford extension problems Theorem
- Atiyah–Singer index formula for a closed even-dimensional geometric Clifford module Theorem
- Complex spinor modules and complete reducibility for Euclidean Spin Theorem
- Irreducible graded Clifford modules and real, complex, and quaternionic types Theorem
- Real Clifford–Thom isomorphism Theorem
- Real Spin modules from the even Clifford algebra Theorem
Dependency tree · two levels
59 results within two dependency steps of this one, each drawn at its shortest distance from it. An arrow runs from a result to what uses it, so the chart reads left to right and ends at this result, which carries a heavier outline. Every node is a link to that result. Click elsewhere on the chart to enlarge it.
Sources
- Jean Gallier, Clifford Algebras, Clifford Groups, and a Generalization of the Quaternions: The Pin and Spin Groups, §1.6 (standard reference, not scraped)
- M. F. Atiyah, R. Bott, and A. Shapiro, Clifford Modules, Part I, §4, Table 1 (standard reference, not scraped)
- Konstantin Wernli, Lecture Notes on Spin Geometry, §§1.4.1–1.4.2, Tables 1.1 and Corollary 1.4.10 (standard reference, not scraped)