Clifford algebra
A finite-dimensional associative algebra over a commutative ring; it was first investigated by W. Clifford in 1876. Let be a commutative ring with an identity, let
be a free
-module and let
be a quadratic form on
. By the Clifford algebra of the quadratic form
(or of the pair
) one means the quotient algebra
of the tensor algebra
of the
-module
by the two-sided ideal generated by the elements of the form
, where
. Elements of
are identified with their corresponding cosets in
. For any
one has
, where
is the symmetric bilinear form associated with
.
For the case of the null quadratic form ,
is the same as the exterior algebra
of
. If
, the field of real numbers, and
is a non-degenerate quadratic form on the
-dimensional vector space
over
, then
is the algebra
of alternions, where
is the number of positive squares in the canonical form of
(cf. Alternion).
Let be a basis of the
-module
. Then the elements
form a basis of the
-module
. In particular,
is a free
-module of rank
. If in addition the
are orthogonal with respect to
, then
can be presented as a
-algebra with generators
and relations
and
. The submodule of
generated by products of an even number of elements of
forms a subalgebra of
, denoted by
.
Suppose that is a field and that the quadratic form
is non-degenerate. For even
,
is a central simple algebra over
of dimension
, the subalgebra
is separable, and its centre
has dimension 2 over
. If
is algebraically closed, then when
is even
is a matrix algebra and
is a product of two matrix algebras. (If, on the other hand,
is odd, then
is a matrix algebra and
is a product of two matrix algebras.)
The invertible elements of
(or of
) for which
form the Clifford group
(or the special Clifford group
) of the quadratic form
. The restriction of the transformation
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to the subspace defines a homomorphism
, where
is the orthogonal group of the quadratic form
. The kernel
consists of the invertible elements of the algebra
and
. If
is even, then
and
is a subgroup of index 2 in
, which in the case when
is not of characteristic 2, is the same as the special orthogonal group
. If
is odd, then
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Let be the anti-automorphism of
induced by the anti-automorphism
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of the tensor algebra . The group
![]() |
is called the spinor group of the quadratic form (or of the Clifford algebra
).
The homomorphism has kernel
. If
or
and
is positive definite, then
and
coincides with the classical spinor group.
References
[1] | N. Bourbaki, "Elements of mathematics" , Addison-Wesley (1966–1977) (Translated from French) |
[2] | J.A. Dieudonné, "La géométrie des groups classiques" , Springer (1955) |
[3] | A.A. Kirillov, "Elements of the theory of representations" , Springer (1976) (Translated from Russian) |
[4] | E. Cartan, "Leçons sur la théorie des spineurs" , Hermann (1938) |
Comments
The algebra generated by products of an even number of elements of the free
-module
is also called the even Clifford algebra of the quadratic form
. See also the articles Exterior algebra (or Grassmann algebra), and Cartan method of exterior forms for more details in the case
.
References
[a1] | C. Chevalley, "The algebraic theory of spinors" , Columbia Univ. Press (1954) |
[a2] | O.T. O'Meara, "Introduction to quadratic forms" , Springer (1973) |
[a3] | C. Chevalley, "The construction and study of certain important algebras" , Math. Soc. Japan (1955) pp. Chapt. III |
Clifford algebra. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Clifford_algebra&oldid=11429