The Grassmann is Always Greener . . .: Fermions and Spins in Clifford Algebra

Matthew R. Francis

Abstract

Typically, the pseudoclassical path integral technique used in quantum field theory uses so-called Grassmann numbers to describe the anticommuting fermionic fields. Likewise, matrix methods are used to describe quantum spins. However, both the Grassman algebra and matrix algebra is are easily formulated in the Clifford algebra, an incredibly powerful mathematical toolbox that encompasses complex algebra, tensors, differential geometry, and so on ad nauseum.

In this talk, I will begin by defining what Clifford algebra _is_, focusing less on the abstract formalism and more on how we can use it in field theory. This includes the "second quantized" formalism and lattices, amongst others. Depending on the time, I may also make some connections with relativistic systems, which are useful in conformal field theory, and group-theoretic techniques.

The mathematical rigor of this talk will be low; I will send you to the literature or to Professor Kosowsky's class next fall for more information about the underlying formalism. However, many of the topics will be technical; I hope to be able to define the terms sufficiently well for those who do not have a strong background in field theory, but if I do not, please stop me and ask questions.

References

Some of the topics I discussed are, alas, unpublished, so until I get my notes into LaTeX form, they will stay that way. However, here are a few relevant papers; note that "Geometric Algebra" (or GA) is synonymous with Clifford algebra.