Clifford algebra

This article is about (orthogonal) Clifford algebra. For symplectic Clifford algebra, see Weyl algebra.

In mathematics, Clifford algebras are a type of associative algebra. As K-algebras, they generalize the real numbers, complex numbers, quaternions and several other hypercomplex number systems. The theory of Clifford algebras is intimately connected with the theory of quadratic forms and orthogonal transformations. Clifford algebras have important applications in a variety of fields including geometry, theoretical physics and digital image processing. They are named after the English geometer William Kingdon Clifford.

The most familiar Clifford algebra, or orthogonal Clifford algebra, is also referred to as Riemannian Clifford algebra.

Introduction and basic properties

A Clifford algebra is a unital associative algebra that contains and is generated by a vector space V over a field K, where V is equipped with a quadratic form Q. The Clifford algebra Cℓ(V, Q) is the "freest" algebra generated by V subject to the condition

$v^{2}=Q(v)1\ {\text{ for all }}v\in V,$

where the product on the left is that of the algebra, and the 1 is its multiplicative identity.

One common way of writing this is to say that the free algebra generated by V may be written as the tensor algebra $\oplus _{n\geq 0}V\otimes \cdots \otimes V$, that is, the sum of n copies of V for all n, and so a Clifford algebra would be the quotient of this tensor algebra by the two-sided ideal generated by elements the form $v\otimes v-Q(v)1$ for all elements $v\in V$. The product induced by the tensor product in the quotient algebra is written using juxtaposition (e.g. uv). Its associativity follows from the associativity of the tensor product.

The definition of a Clifford algebra endows the algebra with more structure than a "bare" K-algebra: specifically it has a distinguished subspace V. Such a subspace cannot in general be uniquely determined given only a K-algebra isomorphic to the Clifford algebra.

If the characteristic of the ground field K is not 2, then one can rewrite this fundamental identity in the form

$uv+vu=2\langle u,v\rangle 1\ {\text{ for all }}u,v\in V,$

where

$\langle u,v\rangle ={\frac {1}{2}}\left(Q(u+v)-Q(u)-Q(v)\right)$

is the symmetric bilinear form associated with Q, via the polarization identity. The idea of being the "freest" or "most general" algebra subject to this identity can be formally expressed through the notion of a universal property, as done below.

Quadratic forms and Clifford algebras in characteristic 2 form an exceptional case. In particular, if char(K) = 2 it is not true that a quadratic form determines a symmetric bilinear form, or that every quadratic form admits an orthogonal basis. Many of the statements in this article include the condition that the characteristic is not 2, and are false if this condition is removed.

As a quantization of the exterior algebra

Clifford algebras are closely related to exterior algebras. In fact, if Q = 0 then the Clifford algebra Cℓ(V, Q) is just the exterior algebra Λ(V). For nonzero Q there exists a canonical linear isomorphism between Λ(V) and Cℓ(V, Q) whenever the ground field K does not have characteristic two. That is, they are naturally isomorphic as vector spaces, but with different multiplications (in the case of characteristic two, they are still isomorphic as vector spaces, just not naturally). Clifford multiplication together with the distinguished subspace is strictly richer than the exterior product since it makes use of the extra information provided by Q.

A different way of saying this is that, if one takes the Clifford algebra to be a filtered algebra, then the associated graded algebra is the exterior algebra.

More precisely, Clifford algebras may be thought of as quantizations (cf. Quantum group) of the exterior algebra, in the same way that the Weyl algebra is a quantization of the symmetric algebra.

Weyl algebras and Clifford algebras admit a further structure of a *-algebra, and can be unified as even and odd terms of a superalgebra, as discussed in CCR and CAR algebras.

Universal property and construction

Let V be a vector space over a field K, and let Q: V → K be a quadratic form on V. In most cases of interest the field K is either the field of real numbers R, or the field of complex numbers C, or a finite field.

A Clifford algebra Cℓ(V, Q) is a unital associative algebra over K together with a linear map i : V → Cℓ(V, Q) satisfying i(v)² = Q(v)1 for all v ∈ V, defined by the following universal property: given any associative algebra A over K and any linear map j : V → A such that

j(v)² = Q(v)1_A for all v ∈ V

(where 1_A denotes the multiplicative identity of A), there is a unique algebra homomorphism f : Cℓ(V, Q) → A such that the following diagram commutes (i.e. such that f ∘ i = j):

The quadratic form Q (in characteristic not 2) may be replaced by a symmetric bilinear form $\langle {\cdot },{\cdot }\rangle$, in which case the requirement on j is

$j(v)j(w)+j(w)j(v)=2\langle v,w\rangle 1_{A}\quad {\text{ for all }}v,w\in V\ .$

A Clifford algebra as described above always exists and can be constructed as follows: start with the most general algebra that contains V, namely the tensor algebra T(V), and then enforce the fundamental identity by taking a suitable quotient. In our case we want to take the two-sided ideal I_Q in T(V) generated by all elements of the form

$v\otimes v-Q(v)1$ for all $v\in V$

and define Cℓ(V, Q) as the quotient algebra

Cℓ(V, Q) = T(V)/I_Q.

The ring product inherited by this quotient is sometimes referred to as the Clifford product to differentiate it from the exterior product and the scalar product.

It is then straightforward to show that Cℓ(V, Q) contains V and satisfies the above universal property, so that Cℓ is unique up to a unique isomorphism; thus one speaks of "the" Clifford algebra Cℓ(V, Q). It also follows from this construction that i is injective. One usually drops the i and considers V as a linear subspace of Cℓ(V, Q).

The universal characterization of the Clifford algebra shows that the construction of Cℓ(V, Q) is functorial in nature. Namely, Cℓ can be considered as a functor from the category of vector spaces with quadratic forms (whose morphisms are linear maps preserving the quadratic form) to the category of associative algebras. The universal property guarantees that linear maps between vector spaces (preserving the quadratic form) extend uniquely to algebra homomorphisms between the associated Clifford algebras.

Basis and dimension

If the dimension of V over K is n and {e₁, ..., e_n} is an orthogonal basis of (V, Q), then Cℓ(V, Q) is free over K with a basis

$\{e_{i_{1}}e_{i_{2}}\cdots e_{i_{k}}\mid 1\leq i_{1}<i_{2}<\cdots <i_{k}\leq n{\mbox{ and }}0\leq k\leq n\}$.

The empty product (k = 0) is defined as the multiplicative identity element. For each value of k there are n choose k basis elements, so the total dimension of the Clifford algebra is

$\dim C\ell (V,Q)=\sum _{k=0}^{n}{\begin{pmatrix}n\\k\end{pmatrix}}=2^{n}.$

Since V comes equipped with a quadratic form, there is a set of privileged bases for V: the orthogonal ones. An orthogonal basis is one such that

$\langle e_{i},e_{j}\rangle =0$ for $i\neq j$, and $\langle e_{i},e_{i}\rangle =Q(e_{i}).$

where $\langle \cdot ,\cdot \rangle$ is the symmetric bilinear form associated to Q. The fundamental Clifford identity implies that for an orthogonal basis

$e_{i}e_{j}=-e_{j}e_{i}$ for $i\neq j$, and $e_{i}^{2}=Q(e_{i})\,$

This makes manipulation of orthogonal basis vectors quite simple. Given a product $e_{i_{1}}e_{i_{2}}\cdots e_{i_{k}}$ of distinct orthogonal basis vectors of V, one can put them into standard order while including an overall sign determined by the number of pairwise swaps needed to do so (i.e. the signature of the ordering permutation).

Examples: real and complex Clifford algebras

The most important Clifford algebras are those over real and complex vector spaces equipped with nondegenerate quadratic forms.

Each of the algebras Cℓ_p,q(R) and Cℓ_n(C) is isomorphic to A or A ⊕ A, where A is a full matrix ring with entries from R, C, or H. For a complete classification of these algebras see classification of Clifford algebras.

Real numbers

Main article: Geometric algebra

The geometric interpretation of real Clifford algebras is known as geometric algebra.

Every nondegenerate quadratic form on a finite-dimensional real vector space is equivalent to the standard diagonal form:

$Q(v)=v_{1}^{2}+\cdots +v_{p}^{2}-v_{p+1}^{2}-\cdots -v_{p+q}^{2}$

where n = p + q is the dimension of the vector space. The pair of integers (p, q) is called the signature of the quadratic form. The real vector space with this quadratic form is often denoted R^p,q. The Clifford algebra on R^p,q is denoted Cℓ_p,q(R). The symbol Cℓ_n(R) means either Cℓ_n,0(R) or Cℓ_0,n(R) depending on whether the author prefers positive definite or negative definite spaces.

A standard basis {e_i} for R^p,q consists of n = p + q mutually orthogonal vectors, p of which square to +1 and q of which square to −1. The algebra Cℓ_p,q(R) will therefore have p vectors that square to +1 and q vectors that square to −1.

Note that Cℓ_0,0(R) is naturally isomorphic to R since there are no nonzero vectors. Cℓ_0,1(R) is a two-dimensional algebra generated by a single vector e₁ that squares to −1, and therefore is isomorphic as an algebra (but not as a superalgebra) to C, the field of complex numbers. The algebra Cℓ_0,2(R) is a four-dimensional algebra spanned by {1, e₁, e₂, e₁e₂}. The latter three elements square to −1 and all anticommute, and so the algebra is isomorphic to the quaternions H. Cℓ_0,3(R) is an 8-dimensional algebra isomorphic to the direct sum H ⊕ H called split-biquaternions.

Complex numbers

One can also study Clifford algebras on complex vector spaces. Every nondegenerate quadratic form on a complex vector space is equivalent to the standard diagonal form

$Q(z)=z_{1}^{2}+z_{2}^{2}+\cdots +z_{n}^{2}$

where n = dim V, up to isomorphism so there is only one nondegenerate Clifford algebra for each dimension n. We will denote the Clifford algebra on Cⁿ with the standard quadratic form by Cℓ_n(C).

The first few cases are not hard to compute. One finds that

Cℓ₀(C) ≅ C, the complex numbers

Cℓ₁(C) ≅ C ⊕ C, the bicomplex numbers

Cℓ₂(C) ≅ M(2, C), the biquaternions

where M(n, C) denotes the algebra of n × n matrices over C.

Examples: constructing quaternions and dual quaternions

Quaternions

In this section, Hamilton's quaternions are constructed as the even sub algebra of the Clifford algebra Cℓ_0,3(R).

Let the vector space V be real three dimensional space R³, and the quadratic form Q be derived from the usual Euclidean metric. Then, for v, w in R³ we have the quadratic form, or scalar product,

$\mathbf {v} \cdot \mathbf {w} =v_{1}w_{1}+v_{2}w_{2}+v_{3}w_{3}.$

Now introduce the Clifford product of vectors v and w given by

$\mathbf {v} \mathbf {w} +\mathbf {w} \mathbf {v} =-2(\mathbf {v} \cdot \mathbf {w} ).$

This formulation uses the negative sign so the correspondence with quaternions is easily shown.

Denote a set of orthogonal unit vectors of R³ as e₁, e₂, and e₃, then the Clifford product yields the relations

$\mathbf {e} _{2}\mathbf {e} _{3}=-\mathbf {e} _{3}\mathbf {e} _{2},\,\,\,\mathbf {e} _{3}\mathbf {e} _{1}=-\mathbf {e} _{1}\mathbf {e} _{3},\,\,\,\mathbf {e} _{1}\mathbf {e} _{2}=-\mathbf {e} _{2}\mathbf {e} _{1},$

and

$\mathbf {e} _{1}^{2}=\mathbf {e} _{2}^{2}=\mathbf {e} _{3}^{2}=-1.$

The general element of the Clifford algebra Cℓ_0,3(R) is given by

$A=a_{0}+a_{1}\mathbf {e} _{1}+a_{2}\mathbf {e} _{2}+a_{3}\mathbf {e} _{3}+a_{4}\mathbf {e} _{2}\mathbf {e} _{3}+a_{5}\mathbf {e} _{3}\mathbf {e} _{1}+a_{6}\mathbf {e} _{1}\mathbf {e} _{2}+a_{7}\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}.$

The linear combination of the even grade elements of Cℓ_0,3(R) defines the even sub algebra Cℓ⁰_0,3(R) with the general element

$Q=q_{0}+q_{1}\mathbf {e} _{2}\mathbf {e} _{3}+q_{2}\mathbf {e} _{3}\mathbf {e} _{1}+q_{3}\mathbf {e} _{1}\mathbf {e} _{2}.$

The basis elements can be identified with the quaternion basis elements i, j, k as

$i=\mathbf {e} _{2}\mathbf {e} _{3},j=\mathbf {e} _{3}\mathbf {e} _{1},k=\mathbf {e} _{1}\mathbf {e} _{2},$

which shows that the even sub algebra Cℓ⁰_0,3(R) is Hamilton's real quaternion algebra.

To see this, compute

$i^{2}=(\mathbf {e} _{2}\mathbf {e} _{3})^{2}=\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{2}\mathbf {e} _{3}=-\mathbf {e} _{2}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{3}=-1,$

and

$ij=\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{3}\mathbf {e} _{1}=-\mathbf {e} _{2}\mathbf {e} _{1}=\mathbf {e} _{1}\mathbf {e} _{2}=k.$

Finally,

$ijk=\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{3}\mathbf {e} _{1}\mathbf {e} _{1}\mathbf {e} _{2}=-1.$

Dual quaternions

In this section, dual quaternions are constructed as the even Clifford algebra of real four dimensional space with a degenerate quadratic form.

Let the vector space V be real four dimensional space R⁴, and let the quadratic form Q be a degenerate form derived from the Euclidean metric on R³. For v, w in R⁴ introduce the degenerate bilinear form

$d(\mathbf {v} ,\mathbf {w} )=v_{1}w_{1}+v_{2}w_{2}+v_{3}w_{3}.$

This degenerate scalar product projects distance measurements in R⁴ onto the R³ hyperplane.

The Clifford product of vectors v and w is given by

$\mathbf {v} \mathbf {w} +\mathbf {w} \mathbf {v} =-2\,d(\mathbf {v} ,\mathbf {w} ).$

Note the negative sign is introduced to simplify the correspondence with quaternions.

Denote a set of orthogonal unit vectors of R⁴ as e₁, e₂, e₃ and e₄, then the Clifford product yields the relations

$\mathbf {e} _{m}\mathbf {e} _{n}=-\mathbf {e} _{n}\mathbf {e} _{m},\,\,\,m\neq n,$

and

$\mathbf {e} _{1}^{2}=\mathbf {e} _{2}^{2}=\mathbf {e} _{3}^{2}=-1,\,\,\mathbf {e} _{4}^{2}=0.$

The general element of the Clifford algebra Cℓ(R⁴, d) has 16 components. The linear combination of the even graded elements defines the even sub algebra Cℓ⁰(R⁴, d) with the general element

$H=h_{0}+h_{1}\mathbf {e} _{2}\mathbf {e} _{3}+h_{2}\mathbf {e} _{3}\mathbf {e} _{1}+h_{3}\mathbf {e} _{1}\mathbf {e} _{2}+h_{4}\mathbf {e} _{4}\mathbf {e} _{1}+h_{5}\mathbf {e} _{4}\mathbf {e} _{2}+h_{6}\mathbf {e} _{4}\mathbf {e} _{3}+h_{7}\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4}.$

The basis elements can be identified with the quaternion basis elements i, j, k and the dual unit ε as

$i=\mathbf {e} _{2}\mathbf {e} _{3},j=\mathbf {e} _{3}\mathbf {e} _{1},k=\mathbf {e} _{1}\mathbf {e} _{2},\,\,\varepsilon =\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4}.$

This provides the correspondence of Cℓ⁰_0,3,1(R) with dual quaternion algebra.

To see this, compute

$\varepsilon ^{2}=(\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4})^{2}=\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4}\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4}=-\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}(\mathbf {e} _{4}\mathbf {e} _{4})\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}=0,$

and

$\varepsilon i=(\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4})\mathbf {e} _{2}\mathbf {e} _{3}=\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4}\mathbf {e} _{2}\mathbf {e} _{3}=\mathbf {e} _{2}\mathbf {e} _{3}(\mathbf {e} _{1}\mathbf {e} _{2}\mathbf {e} _{3}\mathbf {e} _{4})=i\varepsilon .$

The exchanges of e₁ and e₄ alternate signs an even number of times, and show the dual unit ε commutes with the quaternion basis elements i, j, and k.

Examples: in small dimension

Let K be any field of characteristic not 2.

Rank 1

If Q has diagonalization ⟨a⟩, that is there is a non-zero vector x such that Q(x) = a, then Cℓ(V, Q) is a K-algebra generated by an element x satisfying x² = a, so it is the étale quadratic algebra K[X] / (X² − a).

In particular, if a = 0 (that is, Q is the zero quadratic form) then Cℓ(V, Q) is the dual numbers algebra over K.

If a is a non-zero square in K, then Cℓ(V, Q) ≃ K ⊕ K.

Otherwise, Cℓ(V, Q) is the quadratic field extension K(√a) of K.

Rank 2

If Q has diagonalization ⟨a,b⟩ with non-zero a and b (which always exists if Q is non-degenerated), then Cℓ(V, Q) is a K-algebra generated by elements x and y satisfying x² = a, y² = b and xy = −yx.

Thus Cℓ(V, Q) is the (generalized) quaternion algebra (a, b)_K. We retrieve the real case when a = b = −1, since H = (−1, −1)_R.

As a special case, if some x in V satisfies Q(x) = 1, then Cℓ(V, Q) = M₂(K).

Properties

Relation to the exterior algebra

Given a vector space V one can construct the exterior algebra Λ(V), whose definition is independent of any quadratic form on V. It turns out that if K does not have characteristic 2 then there is a natural isomorphism between Λ(V) and Cℓ(V, Q) considered as vector spaces (and there exists an isomorphism in characteristic two, which may not be natural). This is an algebra isomorphism if and only if Q = 0. One can thus consider the Clifford algebra Cℓ(V, Q) as an enrichment (or more precisely, a quantization, cf. the Introduction) of the exterior algebra on V with a multiplication that depends on Q (one can still define the exterior product independent of Q).

The easiest way to establish the isomorphism is to choose an orthogonal basis {e_i} for V and extend it to a basis for Cℓ(V, Q) as described above. The map Cℓ(V, Q) → Λ(V) is determined by

$e_{i_{1}}e_{i_{2}}\cdots e_{i_{k}}\mapsto e_{i_{1}}\wedge e_{i_{2}}\wedge \cdots \wedge e_{i_{k}}.$

Note that this only works if the basis {e_i} is orthogonal. One can show that this map is independent of the choice of orthogonal basis and so gives a natural isomorphism.

If the characteristic of K is 0, one can also establish the isomorphism by antisymmetrizing. Define functions f_k: V × ... × V → Cℓ(V, Q) by

$f_{k}(v_{1},\cdots ,v_{k})={\frac {1}{k!}}\sum _{\sigma \in S_{k}}{\rm {sgn}}(\sigma )\,v_{\sigma (1)}\cdots v_{\sigma (k)}$

where the sum is taken over the symmetric group on k elements. Since f_k is alternating it induces a unique linear map Λ^k(V) → Cℓ(V, Q). The direct sum of these maps gives a linear map between Λ(V) and Cℓ(V, Q). This map can be shown to be a linear isomorphism, and it is natural.

A more sophisticated way to view the relationship is to construct a filtration on Cℓ(V, Q). Recall that the tensor algebra T(V) has a natural filtration: F⁰ ⊂ F¹ ⊂ F² ⊂ ..., where F^k contains sums of tensors with order ≤ k. Projecting this down to the Clifford algebra gives a filtration on Cℓ(V, Q). The associated graded algebra

$Gr_{F}C\ell (V,Q)=\bigoplus _{k}F^{k}/F^{k-1}$

is naturally isomorphic to the exterior algebra Λ(V). Since the associated graded algebra of a filtered algebra is always isomorphic to the filtered algebra as filtered vector spaces (by choosing complements of F^k in F^k+1 for all k), this provides an isomorphism (although not a natural one) in any characteristic, even two.

Grading

In the following, assume that the characteristic is not 2.

Clifford algebras are Z₂-graded algebras (also known as superalgebras). Indeed, the linear map on V defined by v ↦ −v (reflection through the origin) preserves the quadratic form Q and so by the universal property of Clifford algebras extends to an algebra automorphism

α: Cℓ(V, Q) → Cℓ(V, Q).

Since α is an involution (i.e. it squares to the identity) one can decompose Cℓ(V, Q) into positive and negative eigenspaces of α

$C\ell (V,Q)=C\ell ^{0}(V,Q)\oplus C\ell ^{1}(V,Q)$

where Cℓⁱ(V, Q) = {x ∈ Cℓ(V, Q) | α(x) = (−1)ⁱx}. Since α is an automorphism it follows that

$C\ell ^{\,i}(V,Q)C\ell ^{\,j}(V,Q)=C\ell ^{\,i+j}(V,Q)$

where the superscripts are read modulo 2. This gives Cℓ(V, Q) the structure of a Z₂-graded algebra. The subspace Cℓ⁰(V, Q) forms a subalgebra of Cℓ(V, Q), called the even subalgebra. The subspace Cℓ¹(V, Q) is called the odd part of Cℓ(V, Q) (it is not a subalgebra). This Z₂-grading plays an important role in the analysis and application of Clifford algebras. The automorphism α is called the main involution or grade involution. Elements that are pure in this Z₂-grading are simply said to be even or odd.

Remark. In characteristic not 2 the underlying vector space of Cℓ(V, Q) inherits an N-grading and a Z-grading from the canonical isomorphism with the underlying vector space of the exterior algebra Λ(V). It is important to note, however, that this is a vector space grading only. That is, Clifford multiplication does not respect the N-grading or Z-grading, only the Z₂-grading: for instance if Q(v) ≠ 0, then v ∈ Cℓ¹(V, Q), but v² ∈ Cℓ⁰(V, Q), not in Cℓ²(V, Q). Happily, the gradings are related in the natural way: Z₂ ≅ N/2N ≅ Z/2Z. Further, the Clifford algebra is Z-filtered: Cℓ^≤i(V, Q) ⋅ Cℓ^≤j(V, Q) ⊂ Cℓ^≤i+j(V, Q). The degree of a Clifford number usually refers to the degree in the N-grading.

The even subalgebra Cℓ⁰(V, Q) of a Clifford algebra is itself isomorphic to a Clifford algebra. If V is the orthogonal direct sum of a vector a of nonzero norm Q(a) and a subspace U, then Cℓ⁰(V, Q) is isomorphic to Cℓ(U, −Q(a)Q), where −Q(a)Q is the form Q restricted to U and multiplied by −Q(a). In particular over the reals this implies that

$C\ell _{p,q}^{0}(\mathbf {R} )\cong C\ell _{p,q-1}(\mathbf {R} )$ for q > 0, and

$C\ell _{p,q}^{0}(\mathbf {R} )\cong C\ell _{q,p-1}(\mathbf {R} )$ for p > 0.

In the negative-definite case this gives an inclusion Cℓ_0,n−1(R) ⊂ Cℓ_0,n(R), which extends the sequence

R ⊂ C ⊂ H ⊂ H ⊕ H ⊂ ...;

Likewise, in the complex case, one can show that the even subalgebra of Cℓ_n(C) is isomorphic to Cℓ_n−1(C).

Antiautomorphisms

In addition to the automorphism α, there are two antiautomorphisms which play an important role in the analysis of Clifford algebras. Recall that the tensor algebra T(V) comes with an antiautomorphism that reverses the order in all products:

$v_{1}\otimes v_{2}\otimes \cdots \otimes v_{k}\mapsto v_{k}\otimes \cdots \otimes v_{2}\otimes v_{1}.$

Since the ideal I_Q is invariant under this reversal, this operation descends to an antiautomorphism of Cℓ(V, Q) called the transpose or reversal operation, denoted by x^t. The transpose is an antiautomorphism: (xy)^t = y^t x^t. The transpose operation makes no use of the Z₂-grading so we define a second antiautomorphism by composing α and the transpose. We call this operation Clifford conjugation denoted ${\bar {x}}$

${\bar {x}}=\alpha (x^{\mathrm {t} })=\alpha (x)^{\mathrm {t} }.$

Of the two antiautomorphisms, the transpose is the more fundamental.

Note that all of these operations are involutions. One can show that they act as ±1 on elements which are pure in the Z-grading. In fact, all three operations depend only on the degree modulo 4. That is, if x is pure with degree k then

$\alpha (x)=\pm x\qquad x^{\mathrm {t} }=\pm x\qquad {\bar {x}}=\pm x$

where the signs are given by the following table:

k mod 4	0	1	2	3
$\alpha (x)\,$	+	−	+	−	(−1)k
$x^{\mathrm {t} }\,$	+	+	−	−	(−1)k(k−1)/2
${\bar {x}}$	+	−	−	+	(−1)k(k+1)/2

Clifford scalar product

When the characteristic is not 2, the quadratic form Q on V can be extended to a quadratic form on all of Cℓ(V, Q) (which we also denoted by Q). A basis independent definition of one such extension is

$Q(x)=\langle x^{\mathrm {t} }x\rangle$

where ⟨a⟩ denotes the scalar part of a (the grade 0 part in the Z-grading). One can show that

$Q(v_{1}v_{2}\cdots v_{k})=Q(v_{1})Q(v_{2})\cdots Q(v_{k})$

where the v_i are elements of V – this identity is not true for arbitrary elements of Cℓ(V, Q).

The associated symmetric bilinear form on Cℓ(V, Q) is given by

$\langle x,y\rangle =\langle x^{\mathrm {t} }y\rangle .$

One can check that this reduces to the original bilinear form when restricted to V. The bilinear form on all of Cℓ(V, Q) is nondegenerate if and only if it is nondegenerate on V.

It is not hard to verify that the transpose is the adjoint of left/right Clifford multiplication with respect to this inner product. That is,

$\langle ax,y\rangle =\langle x,a^{\mathrm {t} }y\rangle ,$

and

$\langle xa,y\rangle =\langle x,ya^{\mathrm {t} }\rangle .$

Structure of Clifford algebras

In this section we assume that the vector space V is finite dimensional and that the bilinear form of Q is non-singular. A central simple algebra over K is a matrix algebra over a (finite dimensional) division algebra with center K. For example, the central simple algebras over the reals are matrix algebras over either the reals or the quaternions.

• If V has even dimension then Cℓ(V, Q) is a central simple algebra over K.
• If V has even dimension then Cℓ⁰(V, Q) is a central simple algebra over a quadratic extension of K or a sum of two isomorphic central simple algebras over K.
• If V has odd dimension then Cℓ(V, Q) is a central simple algebra over a quadratic extension of K or a sum of two isomorphic central simple algebras over K.
• If V has odd dimension then Cℓ⁰(V, Q) is a central simple algebra over K.

The structure of Clifford algebras can be worked out explicitly using the following result. Suppose that U has even dimension and a non-singular bilinear form with discriminant d, and suppose that V is another vector space with a quadratic form. The Clifford algebra of U + V is isomorphic to the tensor product of the Clifford algebras of U and (−1)^dim(U)/2dV, which is the space V with its quadratic form multiplied by (−1)^dim(U)/2d. Over the reals, this implies in particular that

$C\ell _{p+2,q}(\mathbf {R} )=M_{2}(\mathbf {R} )\otimes C\ell _{q,p}(\mathbf {R} )$

$C\ell _{p+1,q+1}(\mathbf {R} )=M_{2}(\mathbf {R} )\otimes C\ell _{p,q}(\mathbf {R} )$

$C\ell _{p,q+2}(\mathbf {R} )=\mathbf {H} \otimes C\ell _{q,p}(\mathbf {R} ).$

These formulas can be used to find the structure of all real Clifford algebras and all complex Clifford algebras; see the classification of Clifford algebras.

Notably, the Morita equivalence class of a Clifford algebra (its representation theory: the equivalence class of the category of modules over it) depends only on the signature (p − q) mod 8. This is an algebraic form of Bott periodicity.

Clifford group

The class of Clifford groups was discovered by Rudolf Lipschitz.

In this section we assume that V is finite dimensional and the quadratic form Q is nondegenerate.

An action on the elements of a Clifford algebra by the group of its invertible elements may be defined in terms of a twisted conjugation: twisted conjugation by x maps y ↦ x y α(x)⁻¹, where α is the main involution defined above.

The Clifford group Γ is defined to be the set of invertible elements x that stabilize vectors under this action, meaning that for all v in V we have:

$xv\alpha (x)^{-1}\in V.$

This formula also defines an action of the Clifford group on the vector space V that preserves the norm Q, and so gives a homomorphism from the Clifford group to the orthogonal group. The Clifford group contains all elements r of V of nonzero norm, and these act on V by the corresponding reflections that take v to v − 2⟨v,r⟩r/Q(r) (In characteristic 2 these are called orthogonal transvections rather than reflections.)

The Clifford group Γ is the disjoint union of two subsets Γ⁰ and Γ¹, where Γⁱ is the subset of elements of degree i. The subset Γ⁰ is a subgroup of index 2 in Γ.

If V is a finite dimensional real vector space with positive definite (or negative definite) quadratic form then the Clifford group maps onto the orthogonal group of V with respect to the form (by the Cartan–Dieudonné theorem) and the kernel consists of the nonzero elements of the field K. This leads to exact sequences

$1\rightarrow K^{*}\rightarrow \Gamma \rightarrow {\mbox{O}}_{V}(K)\rightarrow 1,\,$

$1\rightarrow K^{*}\rightarrow \Gamma ^{0}\rightarrow {\mbox{SO}}_{V}(K)\rightarrow 1.\,$

Over other fields or with indefinite forms, the map is not in general onto, and the failure is captured by the spinor norm.

Spinor norm

Further information: Spinor norm § Galois cohomology and orthogonal groups

In arbitrary characteristic, the spinor norm Q is defined on the Clifford group by

$Q(x)=x^{\mathrm {t} }x.$

It is a homomorphism from the Clifford group to the group K^× of non-zero elements of K. It coincides with the quadratic form Q of V when V is identified with a subspace of the Clifford algebra. Several authors define the spinor norm slightly differently, so that it differs from the one here by a factor of −1, 2, or −2 on Γ¹. The difference is not very important in characteristic other than 2.

The nonzero elements of K have spinor norm in the group (K^×)² of squares of nonzero elements of the field K. So when V is finite dimensional and non-singular we get an induced map from the orthogonal group of V to the group K^×/(K^×)², also called the spinor norm. The spinor norm of the reflection about r^⊥, for any vector r, has image Q(r) in K^×/(K^×)², and this property uniquely defines it on the orthogonal group. This gives exact sequences:

$1\to \{\pm 1\}\to {\mbox{Pin}}_{V}(K)\to {\mbox{O}}_{V}(K)\to K^{\times }/(K^{\times })^{2},$

$1\to \{\pm 1\}\to {\mbox{Spin}}_{V}(K)\to {\mbox{SO}}_{V}(K)\to K^{\times }/(K^{\times })^{2}.$

Note that in characteristic 2 the group {±1} has just one element.

From the point of view of Galois cohomology of algebraic groups, the spinor norm is a connecting homomorphism on cohomology. Writing μ₂ for the algebraic group of square roots of 1 (over a field of characteristic not 2 it is roughly the same as a two-element group with trivial Galois action), the short exact sequence

$1\to \mu _{2}\rightarrow {\mbox{Pin}}_{V}\rightarrow {\mbox{O}}_{V}\rightarrow 1$

yields a long exact sequence on cohomology, which begins

$1\to H^{0}(\mu _{2};K)\to H^{0}({\mbox{Pin}}_{V};K)\to H^{0}({\mbox{O}}_{V};K)\to H^{1}(\mu _{2};K).$

The 0th Galois cohomology group of an algebraic group with coefficients in K is just the group of K-valued points: H⁰(G; K) = G(K), and H¹(μ₂; K) ≅ K^×/(K^×)², which recovers the previous sequence

$1\to \{\pm 1\}\to {\mbox{Pin}}_{V}(K)\to {\mbox{O}}_{V}(K)\to K^{\times }/(K^{\times })^{2},$

where the spinor norm is the connecting homomorphism H⁰(O_V; K) → H¹(μ₂; K).

Spin and Pin groups

Further information: Spin group, Pin group, and Spinor

In this section we assume that V is finite dimensional and its bilinear form is non-singular. (If K has characteristic 2 this implies that the dimension of V is even.)

The Pin group Pin_V(K) is the subgroup of the Clifford group Γ of elements of spinor norm ±1, and similarly the Spin group Spin_V(K) is the subgroup of elements of Dickson invariant 0 in Pin_V(K). When the characteristic is not 2, these are the elements of determinant 1. The Spin group usually has index 2 in the Pin group.

Recall from the previous section that there is a homomorphism from the Clifford group onto the orthogonal group. We define the special orthogonal group to be the image of Γ⁰. If K does not have characteristic 2 this is just the group of elements of the orthogonal group of determinant 1. If K does have characteristic 2, then all elements of the orthogonal group have determinant 1, and the special orthogonal group is the set of elements of Dickson invariant 0.

There is a homomorphism from the Pin group to the orthogonal group. The image consists of the elements of spinor norm 1 ∈ K^×/(K^×)². The kernel consists of the elements +1 and −1, and has order 2 unless K has characteristic 2. Similarly there is a homomorphism from the Spin group to the special orthogonal group of V.

In the common case when V is a positive or negative definite space over the reals, the spin group maps onto the special orthogonal group, and is simply connected when V has dimension at least 3. Further the kernel of this homomorphism consists of 1 and −1. So in this case the spin group, Spin(n), is a double cover of SO(n). Please note, however, that the simple connectedness of the spin group is not true in general: if V is R^p,q for p and q both at least 2 then the spin group is not simply connected. In this case the algebraic group Spin_p,q is simply connected as an algebraic group, even though its group of real valued points Spin_p,q(R) is not simply connected. This is a rather subtle point, which completely confused the authors of at least one standard book about spin groups.

Spinors

Clifford algebras Cℓ_p,q(C), with p + q = 2n even, are matrix algebras which have a complex representation of dimension 2ⁿ. By restricting to the group Pin_p,q(R) we get a complex representation of the Pin group of the same dimension, called the spin representation. If we restrict this to the spin group Spin_p,q(R) then it splits as the sum of two half spin representations (or Weyl representations) of dimension 2ⁿ⁻¹.

If p + q = 2n + 1 is odd then the Clifford algebra Cℓ_p,q(C) is a sum of two matrix algebras, each of which has a representation of dimension 2ⁿ, and these are also both representations of the Pin group Pin_p,q(R). On restriction to the spin group Spin_p,q(R) these become isomorphic, so the spin group has a complex spinor representation of dimension 2ⁿ.

More generally, spinor groups and pin groups over any field have similar representations whose exact structure depends on the structure of the corresponding Clifford algebras: whenever a Clifford algebra has a factor that is a matrix algebra over some division algebra, we get a corresponding representation of the pin and spin groups over that division algebra. For examples over the reals see the article on spinors.

Real spinors

Further information: spinor

To describe the real spin representations, one must know how the spin group sits inside its Clifford algebra. The Pin group, Pin_p,q is the set of invertible elements in Cℓ_p,q that can be written as a product of unit vectors:

${\mbox{Pin}}_{p,q}=\{v_{1}v_{2}\dots v_{r}|\,\,\forall i\,\|v_{i}\|=\pm 1\}.$

Comparing with the above concrete realizations of the Clifford algebras, the Pin group corresponds to the products of arbitrarily many reflections: it is a cover of the full orthogonal group O(p, q). The Spin group consists of those elements of Pin_{p, q} which are products of an even number of unit vectors. Thus by the Cartan-Dieudonné theorem Spin is a cover of the group of proper rotations SO(p, q).

Let α : Cℓ → Cℓ be the automorphism which is given by the mapping v ↦ −v acting on pure vectors. Then in particular, Spin_p,q is the subgroup of Pin_p,q whose elements are fixed by α. Let

$C\ell _{p,q}^{0}=\{x\in C\ell _{p,q}|\,\alpha (x)=x\}.$

(These are precisely the elements of even degree in Cℓ_p,q.) Then the spin group lies within Cℓ⁰_p,q.

The irreducible representations of Cℓ_p,q restrict to give representations of the pin group. Conversely, since the pin group is generated by unit vectors, all of its irreducible representation are induced in this manner. Thus the two representations coincide. For the same reasons, the irreducible representations of the spin coincide with the irreducible representations of Cℓ⁰_p,q

To classify the pin representations, one need only appeal to the classification of Clifford algebras. To find the spin representations (which are representations of the even subalgebra), one can first make use of either of the isomorphisms (see above)

Cℓ⁰_p,q ≈ Cℓ_p,q−1, for q > 0

Cℓ⁰_p,q ≈ Cℓ_q,p−1, for p > 0

and realize a spin representation in signature (p, q) as a pin representation in either signature (p, q − 1) or (q, p − 1).

Applications

Differential geometry

One of the principal applications of the exterior algebra is in differential geometry where it is used to define the bundle of differential forms on a smooth manifold. In the case of a (pseudo-)Riemannian manifold, the tangent spaces come equipped with a natural quadratic form induced by the metric. Thus, one can define a Clifford bundle in analogy with the exterior bundle. This has a number of important applications in Riemannian geometry. Perhaps more importantly is the link to a spin manifold, its associated spinor bundle and spin^c manifolds.

Physics

Clifford algebras have numerous important applications in physics. Physicists usually consider a Clifford algebra to be an algebra with a basis generated by the matrices γ₀, ..., γ₃ called Dirac matrices which have the property that

$\gamma _{i}\gamma _{j}+\gamma _{j}\gamma _{i}=2\eta _{ij}\,$

where η is the matrix of a quadratic form of signature (1, 3) (or (3, 1) corresponding to the two equivalent choices of metric signature). These are exactly the defining relations for the Clifford algebra Cℓ_1,3(R) up to an unimportant factor of 2, whose complexification is Cℓ_1,3(R)_C which, by the classification of Clifford algebras, is isomorphic to the algebra of 4 × 4 complex matrices Cℓ₄(C) ≈ M₄(C). However, it is best to retain the notation Cℓ_1,3(R)_C, since any transformation that takes the bilinear form to the canonical form is not a Lorentz transformation of the underlying spacetime.

The Clifford algebra of spacetime used in physics thus has more structure than Cℓ₄(C). It has in addition a set of preferred transformations – Lorentz transformations. Whether complexification is necessary to begin with depends in part on conventions used and in part on how much one wants to incorporate straightforwardly, but complexification is most often necessary in quantum mechanics where the spin representation of the Lie algebra so(1, 3) sitting inside the Clifford algebra conventionally requires a complex Clifford algebra. For reference, the spin Lie algebra is given by

$\sigma ^{\mu \nu }=-{\frac {i}{4}}[\gamma ^{\mu },\gamma ^{\nu }],$

$[\sigma ^{\mu \nu },\sigma ^{\rho \tau }]=i(\eta ^{\tau \mu }\sigma ^{\rho \nu }+\eta ^{\nu \tau }\sigma ^{\mu \rho }-\eta ^{\rho \mu }\sigma ^{\tau \nu }-\eta ^{\nu \rho }\sigma ^{\mu \tau }).$

This is in the (3, 1) convention, hence fits in Cℓ_3,1(R)_C.

The Dirac matrices were first written down by Paul Dirac when he was trying to write a relativistic first-order wave equation for the electron, and give an explicit isomorphism from the Clifford algebra to the algebra of complex matrices. The result was used to define the Dirac equation and introduce the Dirac operator. The entire Clifford algebra shows up in quantum field theory in the form of Dirac field bilinears.

The use of Clifford algebras to describe quantum theory has been advanced among others by Mario Schönberg, by David Hestenes in terms of geometric calculus, by David Bohm and Basil Hiley and co-workers in form of a hierarchy of Clifford algebras, and by Elio Conte et al.

Computer vision

Recently, Clifford algebras have been applied in the problem of action recognition and classification in computer vision. Rodriguez et al. propose a Clifford embedding to generalize traditional MACH filters to video (3D spatiotemporal volume), and vector-valued data such as optical flow. Vector-valued data is analyzed using the Clifford Fourier Transform. Based on these vectors action filters are synthesized in the Clifford Fourier domain and recognition of actions is performed using Clifford Correlation. The authors demonstrate the effectiveness of the Clifford embedding by recognizing actions typically performed in classic feature films and sports broadcast television.

See also

• Algebra of physical space, APS
• Cayley–Dickson construction
• Classification of Clifford algebras
• Clifford analysis
• Clifford module
• Complex spin structure
• Dirac operator
• Exterior algebra
• Gamma matrices
• Generalized Clifford algebra
• Geometric algebra
• Higher-dimensional gamma matrices
• Hypercomplex number
• Octonion
• Paravector
• Quaternion
• Spin group
• Spin structure
• Spinor
• Spinor bundle

References

• Bourbaki, Nicolas (1988), Algebra, Berlin, New York: Springer-Verlag, ISBN 978-3-540-19373-9, section IX.9.
• Carnahan, S. Borcherds Seminar Notes, Uncut. Week 5, "Spinors and Clifford Algebras".
• Garling, D. J. H. (2011), Clifford algebras. An introduction, London Mathematical Society Student Texts, vol. 78, Cambridge: Cambridge University Press, ISBN 978-1-107-09638-7, Zbl 1235.15025
• Lam, Tsit-Yuen (2005), Introduction to Quadratic Forms over Fields, Graduate Studies in Mathematics, vol. 67, American Mathematical Society, ISBN 0-8218-1095-2, MR 2104929, Zbl 1068.11023
• Lawson, H. Blaine; Michelsohn, Marie-Louise (1989), Spin Geometry, Princeton, NJ: Princeton University Press, ISBN 978-0-691-08542-5. An advanced textbook on Clifford algebras and their applications to differential geometry.
• Lounesto, Pertti (2001), Clifford algebras and spinors, Cambridge: Cambridge University Press, ISBN 978-0-521-00551-7
• Porteous, Ian R. (1995), Clifford algebras and the classical groups, Cambridge: Cambridge University Press, ISBN 978-0-521-55177-9
• Jagannathan, R., On generalized Clifford algebras and their physical applications, arXiv:1005.4300
• Sylvester, J. J., (1882), Johns Hopkins University Circulars I: 241-242; ibid II (1883) 46; ibid III (1884) 7-9. Summarized in The Collected Mathematics Papers of James Joseph Sylvester (Cambridge University Press, 1909) v III .online and further.
• Weinberg, S. (2002), The Quantum Theory of Fields, vol. 1, Cambridge University Press, ISBN 0-521-55001-7

Further reading

• Knus, Max-Albert (1991), Quadratic and Hermitian forms over rings, Grundlehren der Mathematischen Wissenschaften, vol. 294, Berlin: Springer-Verlag, doi:10.1007/978-3-642-75401-2, ISBN 3-540-52117-8, MR 1096299, Zbl 0756.11008

External links

• "Clifford algebra", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
• Planetmath entry on Clifford algebras
• A history of Clifford algebras (unverified)
• John Baez on Clifford algebras
• Clifford Algebra: A Visual Introduction