Namespaces
Variants
Actions

Difference between revisions of "Clifford algebra"

From Encyclopedia of Mathematics
Jump to: navigation, search
(Importing text file)
 
m (link)
 
(2 intermediate revisions by one other user not shown)
Line 1: Line 1:
A finite-dimensional associative algebra over a commutative ring; it was first investigated by W. Clifford in 1876. Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224601.png" /> be a commutative ring with an identity, let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224602.png" /> be a free <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224603.png" />-module and let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224604.png" /> be a quadratic form on <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224605.png" />. By the Clifford algebra of the quadratic form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224606.png" /> (or of the pair <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224607.png" />) one means the quotient algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224608.png" /> of the tensor algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c0224609.png" /> of the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246010.png" />-module <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246011.png" /> by the two-sided ideal generated by the elements of the form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246012.png" />, where <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246013.png" />. Elements of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246014.png" /> are identified with their corresponding cosets in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246015.png" />. For any <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246016.png" /> one has <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246017.png" />, where <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246018.png" /> is the symmetric bilinear form associated with <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246019.png" />.
+
{{MSC|15A66}}
 +
{{TEX|done}}
  
For the case of the null quadratic form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246020.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246021.png" /> is the same as the [[Exterior algebra|exterior algebra]] <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246022.png" /> of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246023.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246024.png" />, the field of real numbers, and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246025.png" /> is a non-degenerate quadratic form on the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246026.png" />-dimensional vector space <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246027.png" /> over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246028.png" />, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246029.png" /> is the algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246030.png" /> of alternions, where <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246031.png" /> is the number of positive squares in the canonical form of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246032.png" /> (cf. [[Alternion|Alternion]]).
+
The ''Clifford algebra'' of a [[quadratic form]] is
 +
a finite-dimensional associative algebra over a commutative ring; it was first investigated by W. Clifford in 1876. Let $K$ be a commutative ring with an identity, let $E$ be a free $K$-module and let $Q$ be a quadratic form on $E$. By the Clifford algebra of the quadratic form $Q$ (or of the pair $(E,Q)$) one means the quotient algebra $C(Q)$ of the tensor algebra $T(E)$ of the $K$-module $E$ by the two-sided ideal generated by the elements of the form $x\otimes x-Q(x)\cdot 1$, where $x\in E$. Elements of $E$ are identified with their corresponding cosets in $C(Q)$. For any $x,y\in E$ one has $xy+yx=\Phi(x,y)$, where $\Phi(E\times E)\to K$ is the symmetric bilinear form associated with $Q$.
  
Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246033.png" /> be a basis of the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246034.png" />-module <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246035.png" />. Then the elements <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246036.png" /> <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246037.png" /> form a basis of the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246038.png" />-module <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246039.png" />. In particular, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246040.png" /> is a free <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246041.png" />-module of rank <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246042.png" />. If in addition the <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246043.png" /> are orthogonal with respect to <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246044.png" />, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246045.png" /> can be presented as a <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246046.png" />-algebra with generators <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246047.png" /> and relations <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246048.png" /> <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246049.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246050.png" />. The submodule of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246051.png" /> generated by products of an even number of elements of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246052.png" /> forms a subalgebra of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246053.png" />, denoted by <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246054.png" />.
+
For the case of the null quadratic form $Q$, $C(Q)$ is the same as the
 +
[[Exterior algebra|exterior algebra]] $\Lambda(E)$ of $E$. If $K=\R$, the field of real numbers, and $Q$ is a non-degenerate quadratic form on the $n$-dimensional vector space $E$ over $\R$, then $C(G)$ is the algebra ${}^lA_{n+1}$ of alternions, where $l$ is the number of positive squares in the canonical form of $Q$ (cf.
 +
[[Alternion|Alternion]]).
  
Suppose that <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246055.png" /> is a field and that the quadratic form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246056.png" /> is non-degenerate. For even <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246057.png" />, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246058.png" /> is a [[Central simple algebra|central simple algebra]] over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246059.png" /> of dimension <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246060.png" />, the subalgebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246061.png" /> is separable, and its centre <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246062.png" /> has dimension 2 over <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246063.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246064.png" /> is algebraically closed, then when <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246065.png" /> is even <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246066.png" /> is a matrix algebra and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246067.png" /> is a product of two matrix algebras. (If, on the other hand, <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246068.png" /> is odd, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246069.png" /> is a matrix algebra and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246070.png" /> is a product of two matrix algebras.)
+
Let $e_1,\dots,e_n$ be a basis of the $K$-module $E$. Then the
 +
elements $1, e_{i_1}\cdots e_{i_k}\; (i_1<\cdots < i_k)$ form a basis
 +
of the $K$-module $C(Q)$. In particular, $C(Q)$ is a free $K$-module
 +
of rank $2^n$. If in addition the $e_1,\dots,e_n$ are orthogonal with
 +
respect to $Q$, then $C(Q)$ can be presented as a $K$-algebra with
 +
generators $1,e_1,\dots,e_n$ and relations $e_i e_j = -e_je_i\; (i\ne j)$
 +
and $e_i^2 = Q(e_i)$. The submodule of $C(Q)$ generated by products of an even number of elements of $E$ forms a subalgebra of $C(Q)$, denoted by $C^+(Q)$.
  
The invertible elements <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246071.png" /> of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246072.png" /> (or of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246073.png" />) for which <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246074.png" /> form the Clifford group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246075.png" /> (or the special Clifford group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246076.png" />) of the quadratic form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246077.png" />. The restriction of the transformation
+
Suppose that $K$ is a field and that the quadratic form $Q$ is non-degenerate. For even $n$, $C(Q)$ is a
 +
[[Central simple algebra|central simple algebra]] over $K$ of dimension $2^n$, the subalgebra $C^+(Q)$ is separable, and its centre $Z$ has dimension 2 over $K$. If $K$ is algebraically closed, then when $n$ is even $C(Q)$ is a matrix algebra and $C^+(Q)$ is a product of two matrix algebras. (If, on the other hand, $n$ is odd, then $C^+(Q)$ is a matrix algebra and $C(Q)$ is a product of two matrix algebras.)
  
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246078.png" /></td> </tr></table>
+
The invertible elements $s$ of $C(Q)$ (or of $C^+(Q)$) for which $sEs^{-1} = E$ form the Clifford group $G(Q)$ (or the special Clifford group $G^+(Q)$) of the quadratic form $Q$. The restriction of the transformation
  
to the subspace <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246079.png" /> defines a homomorphism <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246080.png" />, where <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246081.png" /> is the [[Orthogonal group|orthogonal group]] of the quadratic form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246082.png" />. The kernel <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246083.png" /> consists of the invertible elements of the algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246084.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246085.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246086.png" /> is even, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246087.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246088.png" /> is a subgroup of index 2 in <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246089.png" />, which in the case when <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246090.png" /> is not of characteristic 2, is the same as the special orthogonal group <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246091.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246092.png" /> is odd, then
+
$$x\mapsto sxs^{-1}\quad (x\in G(Q))$$
 +
to the subspace $E$ defines a homomorphism $\def\phi{\varphi}\phi : G(Q)\to \def\O{ {\rm O}}\O(Q)$, where $\O(Q)$ is the
 +
[[Orthogonal group|orthogonal group]] of the quadratic form $Q$. The
 +
kernel $\def\Ker{ {\rm Ker}\;}\Ker \phi$ consists of the invertible elements of the algebra $Z$ and $(\Ker \phi)\cap G^+(Q) = k^*$. If $n$ is even, then $\phi(G(Q))=\O(G)$ and $\phi(G^+(Q))=\O^+(G)$ is a subgroup of index 2 in $\O(Q)$, which in the case when $K$ is not of characteristic 2, is the same as the special orthogonal group $\def\SO{ {\rm SO}}\SO(Q)$. If $n$ is odd, then
  
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246093.png" /></td> </tr></table>
+
$$\phi(G(Q)) = \phi(G^+(Q)) = \SO(Q).$$
 +
Let $\beta : C(Q) \to C(Q)$ be the [[anti-automorphism]] of $C(Q)$ induced by the anti-automorphism
  
Let <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246094.png" /> be the anti-automorphism of <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246095.png" /> induced by the anti-automorphism
+
$$x_1\otimes\cdots \otimes x_n \mapsto x_n\otimes\cdots \otimes x_1$$
 +
of the tensor algebra $T(E)$. The group
  
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246096.png" /></td> </tr></table>
+
$$\def\Spin{ {\rm Spin}}\Spin(Q) = \{s\in G^+(Q) : \beta(s) = s^{-1} \}$$
 +
is called the spinor group of the quadratic form $Q$ (or of the Clifford algebra $C(Q)$).
  
of the tensor algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246097.png" />. The group
+
The homomorphism $\phi: \Spin(Q) \to \O^+(Q) $ has kernel $\{\pm1\}$. If $K=\C$ or $K=\R$ and $Q$ is positive definite, then ${\rm Im}\;\phi : \O^+(Q) = \SO(Q)$ and $\Spin(Q)$ coincides with the classical
 +
[[Spinor group|spinor group]].
  
<table class="eq" style="width:100%;"> <tr><td valign="top" style="width:94%;text-align:center;"><img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246098.png" /></td> </tr></table>
+
====Comments====
 
+
The algebra $C^+(Q)$ generated by products of an even number of elements of the free $K$-module $E$ is also called the even Clifford algebra of the quadratic form $Q$. See also the articles
is called the spinor group of the quadratic form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c02246099.png" /> (or of the Clifford algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460100.png" />).
+
[[Exterior algebra|Exterior algebra]] (or Grassmann algebra), and
 
+
[[Cartan method of exterior forms|Cartan method of exterior forms]] for more details in the case $Q=0$.
The homomorphism <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460101.png" /> has kernel <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460102.png" />. If <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460103.png" /> or <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460104.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460105.png" /> is positive definite, then <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460106.png" /> and <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460107.png" /> coincides with the classical [[Spinor group|spinor group]].
 
  
====References====
 
<table><TR><TD valign="top">[1]</TD> <TD valign="top">  N. Bourbaki,  "Elements of mathematics" , Addison-Wesley  (1966–1977)  (Translated from French)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top">  J.A. Dieudonné,  "La géométrie des groups classiques" , Springer  (1955)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top">  A.A. Kirillov,  "Elements of the theory of representations" , Springer  (1976)  (Translated from Russian)</TD></TR><TR><TD valign="top">[4]</TD> <TD valign="top">  E. Cartan,  "Leçons sur la théorie des spineurs" , Hermann  (1938)</TD></TR></table>
 
  
 
 
====Comments====
 
The algebra <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460108.png" /> generated by products of an even number of elements of the free <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460109.png" />-module <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460110.png" /> is also called the even Clifford algebra of the quadratic form <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460111.png" />. See also the articles [[Exterior algebra|Exterior algebra]] (or Grassmann algebra), and [[Cartan method of exterior forms|Cartan method of exterior forms]] for more details in the case <img align="absmiddle" border="0" src="https://www.encyclopediaofmath.org/legacyimages/c/c022/c022460/c022460112.png" />.
 
  
 
====References====
 
====References====
<table><TR><TD valign="top">[a1]</TD> <TD valign="top"> C. Chevalley,   "The algebraic theory of spinors" , Columbia Univ. Press  (1954)</TD></TR><TR><TD valign="top">[a2]</TD> <TD valign="top">  O.T. O'Meara,   "Introduction to quadratic forms" , Springer  (1973)</TD></TR><TR><TD valign="top">[a3]</TD> <TD valign="top"C. Chevalley,   "The construction and study of certain important algebras" , Math. Soc. Japan (1955) pp. Chapt. III</TD></TR></table>
+
{|
 +
|-
 +
|valign="top"|{{Ref|Bo}}||valign="top"| N. Bourbaki, Éléments de mathématique. Première partie: Les structures fondamentales de l'analyse. Livre II: Algèbre. Chapitre 9: Formes sesquilinéaires et formes quadratiques.  Addison-Wesley (1966–1977) {{MR|0107661}} {{ZBL|0102.25503}}
 +
|-
 +
|valign="top"|{{Ref|Ca}}||valign="top"| E. Cartan, "Leçons sur la théorie des spineurs", Hermann (1938) {{MR|}} {{ZBL|0022.17101}} {{ZBL|0019.36301}} {{ZBL|64.1382.04}}
 +
|-
 +
|valign="top"|{{Ref|Ch}}||valign="top"| C. Chevalley, "The algebraic theory of spinors", Columbia Univ. Press (1954) {{MR|0060497}} {{ZBL|0057.25901}}
 +
|-
 +
|valign="top"|{{Ref|Ch2}}||valign="top"| C. Chevalley, "The construction and study of certain important algebras", Math. Soc. Japan (1955) pp. Chapt. III {{MR|0072867}} {{ZBL|}}
 +
|-
 +
|valign="top"|{{Ref|Ki}}||valign="top"| A.A. Kirillov, "Elements of the theory of representations", Springer (1976) (Translated from Russian) {{MR|0412321}} {{ZBL|0342.22001}}
 +
|-
 +
|valign="top"|{{Ref|OM}}||valign="top"| O.T. O'Meara, "Introduction to quadratic forms", Springer (1973) {{MR|}} {{ZBL|0259.10018}}
 +
|-
 +
|}

Latest revision as of 17:17, 9 October 2016

2020 Mathematics Subject Classification: Primary: 15A66 [MSN][ZBL]

The Clifford algebra of a quadratic form is a finite-dimensional associative algebra over a commutative ring; it was first investigated by W. Clifford in 1876. Let $K$ be a commutative ring with an identity, let $E$ be a free $K$-module and let $Q$ be a quadratic form on $E$. By the Clifford algebra of the quadratic form $Q$ (or of the pair $(E,Q)$) one means the quotient algebra $C(Q)$ of the tensor algebra $T(E)$ of the $K$-module $E$ by the two-sided ideal generated by the elements of the form $x\otimes x-Q(x)\cdot 1$, where $x\in E$. Elements of $E$ are identified with their corresponding cosets in $C(Q)$. For any $x,y\in E$ one has $xy+yx=\Phi(x,y)$, where $\Phi(E\times E)\to K$ is the symmetric bilinear form associated with $Q$.

For the case of the null quadratic form $Q$, $C(Q)$ is the same as the exterior algebra $\Lambda(E)$ of $E$. If $K=\R$, the field of real numbers, and $Q$ is a non-degenerate quadratic form on the $n$-dimensional vector space $E$ over $\R$, then $C(G)$ is the algebra ${}^lA_{n+1}$ of alternions, where $l$ is the number of positive squares in the canonical form of $Q$ (cf. Alternion).

Let $e_1,\dots,e_n$ be a basis of the $K$-module $E$. Then the elements $1, e_{i_1}\cdots e_{i_k}\; (i_1<\cdots < i_k)$ form a basis of the $K$-module $C(Q)$. In particular, $C(Q)$ is a free $K$-module of rank $2^n$. If in addition the $e_1,\dots,e_n$ are orthogonal with respect to $Q$, then $C(Q)$ can be presented as a $K$-algebra with generators $1,e_1,\dots,e_n$ and relations $e_i e_j = -e_je_i\; (i\ne j)$ and $e_i^2 = Q(e_i)$. The submodule of $C(Q)$ generated by products of an even number of elements of $E$ forms a subalgebra of $C(Q)$, denoted by $C^+(Q)$.

Suppose that $K$ is a field and that the quadratic form $Q$ is non-degenerate. For even $n$, $C(Q)$ is a central simple algebra over $K$ of dimension $2^n$, the subalgebra $C^+(Q)$ is separable, and its centre $Z$ has dimension 2 over $K$. If $K$ is algebraically closed, then when $n$ is even $C(Q)$ is a matrix algebra and $C^+(Q)$ is a product of two matrix algebras. (If, on the other hand, $n$ is odd, then $C^+(Q)$ is a matrix algebra and $C(Q)$ is a product of two matrix algebras.)

The invertible elements $s$ of $C(Q)$ (or of $C^+(Q)$) for which $sEs^{-1} = E$ form the Clifford group $G(Q)$ (or the special Clifford group $G^+(Q)$) of the quadratic form $Q$. The restriction of the transformation

$$x\mapsto sxs^{-1}\quad (x\in G(Q))$$ to the subspace $E$ defines a homomorphism $\def\phi{\varphi}\phi : G(Q)\to \def\O{ {\rm O}}\O(Q)$, where $\O(Q)$ is the orthogonal group of the quadratic form $Q$. The kernel $\def\Ker{ {\rm Ker}\;}\Ker \phi$ consists of the invertible elements of the algebra $Z$ and $(\Ker \phi)\cap G^+(Q) = k^*$. If $n$ is even, then $\phi(G(Q))=\O(G)$ and $\phi(G^+(Q))=\O^+(G)$ is a subgroup of index 2 in $\O(Q)$, which in the case when $K$ is not of characteristic 2, is the same as the special orthogonal group $\def\SO{ {\rm SO}}\SO(Q)$. If $n$ is odd, then

$$\phi(G(Q)) = \phi(G^+(Q)) = \SO(Q).$$ Let $\beta : C(Q) \to C(Q)$ be the anti-automorphism of $C(Q)$ induced by the anti-automorphism

$$x_1\otimes\cdots \otimes x_n \mapsto x_n\otimes\cdots \otimes x_1$$ of the tensor algebra $T(E)$. The group

$$\def\Spin{ {\rm Spin}}\Spin(Q) = \{s\in G^+(Q) : \beta(s) = s^{-1} \}$$ is called the spinor group of the quadratic form $Q$ (or of the Clifford algebra $C(Q)$).

The homomorphism $\phi: \Spin(Q) \to \O^+(Q) $ has kernel $\{\pm1\}$. If $K=\C$ or $K=\R$ and $Q$ is positive definite, then ${\rm Im}\;\phi : \O^+(Q) = \SO(Q)$ and $\Spin(Q)$ coincides with the classical spinor group.

Comments

The algebra $C^+(Q)$ generated by products of an even number of elements of the free $K$-module $E$ is also called the even Clifford algebra of the quadratic form $Q$. See also the articles Exterior algebra (or Grassmann algebra), and Cartan method of exterior forms for more details in the case $Q=0$.


References

[Bo] N. Bourbaki, Éléments de mathématique. Première partie: Les structures fondamentales de l'analyse. Livre II: Algèbre. Chapitre 9: Formes sesquilinéaires et formes quadratiques. Addison-Wesley (1966–1977) MR0107661 Zbl 0102.25503
[Ca] E. Cartan, "Leçons sur la théorie des spineurs", Hermann (1938) Zbl 0022.17101 Zbl 0019.36301 Zbl 64.1382.04
[Ch] C. Chevalley, "The algebraic theory of spinors", Columbia Univ. Press (1954) MR0060497 Zbl 0057.25901
[Ch2] C. Chevalley, "The construction and study of certain important algebras", Math. Soc. Japan (1955) pp. Chapt. III MR0072867
[Ki] A.A. Kirillov, "Elements of the theory of representations", Springer (1976) (Translated from Russian) MR0412321 Zbl 0342.22001
[OM] O.T. O'Meara, "Introduction to quadratic forms", Springer (1973) Zbl 0259.10018
How to Cite This Entry:
Clifford algebra. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Clifford_algebra&oldid=11429
This article was adapted from an original article by I.V. Dolgachev (originator), which appeared in Encyclopedia of Mathematics - ISBN 1402006098. See original article