Supersymmetry as a quantum group

Following is the essence of supersymmetry, which is encapsulated within the following minimal quantum group. We have the two dimensional Hopf algebra generated by (-1)F subject to

${\displaystyle {(-1)^{F}}^{2}=1}$

with the counit

${\displaystyle \epsilon ((-1)^{F})=1}$

and the coproduct

${\displaystyle \Delta (-1)^{F}=(-1)^{F}\otimes (-1)^{F}}$

and the antipode

${\displaystyle S(-1)^{F}=(-1)^{F}}$

Thus far, there is nothing supersymmetric about this Hopf algebra at all; it is isomorphic to the Hopf algebra of the two element group ${\displaystyle \mathbb {Z} _{2}}$. Supersymmetry comes in when introducing the nontrivial quasitriangular structure

${\displaystyle {\mathcal {R}}={\frac {1}{2}}\left[1\otimes 1+(-1)^{F}\otimes 1+1\otimes (-1)^{F}-(-1)^{F}\otimes (-1)^{F}\right]}$

where +1 eigenstates of (-1)^F are called bosons and -1 eigenstates are called fermions.

This describes a fermionic braiding; don't pick up a phase factor when interchanging two bosons or a boson and a fermion, but multiply by -1 when interchanging two fermions. This provides the essence of the boson/fermion distinction.

The previous analysis only introduced the concept of fermions, and is not actual supersymmetry. The Hopf algebra is ${\displaystyle \mathbb {Z} _{2}}$ graded and contains even and odd elements. Even elements commute with (-1)^F; odd ones anticommute. The subalgebra not containing (-1)^F is supercommutative.

Let's say we are dealing with a super Lie algebra with even generators x and odd generators y.

Then,

${\displaystyle \Delta x=x\otimes 1+1\otimes x}$

${\displaystyle \Delta y=y\otimes 1+(-1)^{F}\otimes y}$

This is compatible with ${\displaystyle {\mathcal {R}}}$.

Supersymmetry is the symmetry over systems where interchanging two fermions attain a minus sign.

• Introduction to quantum mechanics
• Group theory
• Symmetry group