Clifford module explained

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.

Matrix representations of real Clifford algebras

We will need to study anticommuting matrices because in Clifford algebras orthogonal vectors anticommute

AB=

1
2

(AB+BA)=0.

For the real Clifford algebra

Rp,q

, we need mutually anticommuting matrices, of which p have +1 as square and q have −1 as square.
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.

Real Clifford algebra R3,1

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.

See also

References