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In mathematics, a Clifford module is a
representation Representation may refer to: Law and politics *Representation (politics), political activities undertaken by elected representatives, as well as other theories ** Representative democracy, type of democracy in which elected officials represent a ...
of a Clifford algebra. In general a Clifford algebra ''C'' is a central simple algebra over some
field extension In mathematics, particularly in algebra, a field extension is a pair of fields E\subseteq F, such that the operations of ''E'' are those of ''F'' restricted to ''E''. In this case, ''F'' is an extension field of ''E'' and ''E'' is a subfield of ...
''L'' of the field ''K'' over which the
quadratic form In mathematics, a quadratic form is a polynomial with terms all of degree two ("form" is another name for a homogeneous polynomial). For example, :4x^2 + 2xy - 3y^2 is a quadratic form in the variables and . The coefficients usually belong to ...
''Q'' defining ''C'' is defined. The abstract theory of Clifford modules was founded by a paper of M. F. Atiyah,
R. Bott Raoul Bott (September 24, 1923 – December 20, 2005) was a Hungarian-American mathematician known for numerous basic contributions to geometry in its broad sense. He is best known for his Bott periodicity theorem, the Morse–Bott functions whi ...
and Arnold S. Shapiro. A fundamental result on Clifford modules is that the
Morita equivalence In abstract algebra, Morita equivalence is a relationship defined between rings that preserves many ring-theoretic properties. More precisely two rings like ''R'', ''S'' are Morita equivalent (denoted by R\approx S) if their categories of modul ...
class of a Clifford algebra (the equivalence class of the category of Clifford modules over it) depends only on the signature . This is an algebraic form of Bott periodicity.


Matrix representations of real Clifford algebras

We will need to study ''anticommuting'' matrices () because in Clifford algebras orthogonal vectors anticommute : A \cdot B = \frac( AB + BA ) = 0. For the real Clifford algebra \mathbb_, we need mutually anticommuting matrices, of which ''p'' have +1 as square and ''q'' have −1 as square. : \begin \gamma_a^2 &=& +1 &\mbox &1 \le a \le p \\ \gamma_a^2 &=& -1 &\mbox &p+1 \le a \le p+q\\ \gamma_a \gamma_b &=& -\gamma_b \gamma_a &\mbox &a \ne b. \ \\ \end Such a basis of gamma matrices is not unique. One can always obtain another set of gamma matrices satisfying the same Clifford algebra by means of a similarity transformation. :\gamma_ = S \gamma_ S^ , where ''S'' is a non-singular matrix. The sets ''γ''''a''′ and ''γ''''a'' belong to the same equivalence class.


Real Clifford algebra R3,1

Developed by
Ettore Majorana Ettore Majorana (,, uploaded 19 April 2013, retrieved 14 December 2019 ; born on 5 August 1906 – possibly dying after 1959) was an Italian theoretical physicist who worked on neutrino masses. On 25 March 1938, he disappeared under mysteri ...
, this Clifford module enables the construction of a Dirac-like equation without complex numbers, and its elements are called Majorana spinors. The four basis vectors are the three Pauli matrices and a fourth antihermitian matrix. The signature is (+++−). For the signatures (+−−−) and (−−−+) often used in physics, 4×4 complex matrices or 8×8 real matrices are needed.


See also

* Weyl–Brauer matrices * Higher-dimensional gamma matrices * Clifford module bundle


References

* * . See als
the programme website
for a preliminary version. * . * {{citation, last1=Lawson, first1= H. Blaine, last2=Michelsohn, first2=Marie-Louise, author2-link=Marie-Louise Michelsohn, title=Spin Geometry, publisher= Princeton University Press, year=1989, isbn= 0-691-08542-0. Representation theory Clifford algebras