Vertex Operator Superalgebra
When the underlying vector space V has a Z2 grading, so that it splits as a sum of even and odd parts
with 1 in V+, the structure of a vertex superalgebra can be defined on V by incorporating the usual rule of signs in the axiom for the four point function:
- (Four point function) For any a, b, c ∈ V±, there is an element
such that Y(a,z)Y(b,w)c, εY(b,w)Y(a,z)c, and Y(Y(a,z-w)b,w)c are the expansions of X(a,b,c;z,w) in V((z))((w)), V((w))((z)), and V((w))((z-w)), respectively, where ε is -1 if both a and b are odd and 1 otherwise.
If in addition there is a Virasoro element ω in the even part of V2, then V is called a vertex operator superalgebra. One of the simplest examples is the vertex operator superalgebra generated by a single complex fermion.
Read more about this topic: Vertex Operator Algebra