In mathematics, a Clifford module is a representation of a Clifford algebra. In general a Clifford algebra C is a central simple algebra over some field extension L of the field K over which the quadratic form Q defining C is defined.
The abstract theory of Clifford modules was founded by a paper of M. F. Atiyah, R. Bott and Arnold S. Shapiro. A fundamental result on Clifford modules is that the Morita equivalence 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.
We will need to study anticommuting matrices because in Clifford algebras orthogonal vectors anticommute
A ⋅ B=
1 | |
2 |
(AB+BA)=0.
For the real Clifford algebra
Rp,q
2 | |
\begin{matrix} \gamma | |
a |
&=&+1&if&1\lea\lep
2 | |
\\ \gamma | |
a |
&=&-1&if&p+1\lea\lep+q\\ \gammaa\gammab&=&-\gammab\gammaa&if&a\neb. \\ \end{matrix}
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.
\gammaa'=S\gammaaS-1,
where S is a non-singular matrix. The sets γa′ and γa belong to the same equivalence class.
Developed by Ettore Majorana, 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.