In supergravity and supersymmetric representation theory, Adinkra symbols are a graphical representation of supersymmetric algebras.[1][2][3][4][5] Mathematically they can be described as colored finite connected simple graphs, that are bipartite and n-regular.[6] Their name is derived from Adinkra symbols of the same name, and they were introduced by Michael Faux and Sylvester James Gates in 2004.[1]
One approach to the representation theory of super Lie algebras is to restrict attention to representations in one space-time dimension and having [math]\displaystyle{ N }[/math] supersymmetry generators, i.e., to [math]\displaystyle{ (1|N) }[/math] superalgebras. In that case, the defining algebraic relationship among the supersymmetry generators reduces to
Here [math]\displaystyle{ \partial_\tau }[/math] denotes partial differentiation along the single space-time coordinate. One simple realization of the [math]\displaystyle{ (1|1) }[/math] algebra consists of a single bosonic field [math]\displaystyle{ \phi }[/math], a fermionic field [math]\displaystyle{ \psi }[/math], and a generator [math]\displaystyle{ Q }[/math] which acts as
Since we have just one supersymmetry generator in this case, the superalgebra relation reduces to [math]\displaystyle{ Q^2 = i \partial _\tau }[/math], which is clearly satisfied. We can represent this algebra graphically using one solid vertex, one hollow vertex, and a single colored edge connecting them.