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Supersymmetry as a quantum group : ウィキペディア英語版
Supersymmetry as a quantum group

The concept in theoretical physics of supersymmetry can be reinterpreted in the language of noncommutative geometry and quantum groups. In particular, it involves a mild form of noncommutativity, namely supercommutativity.
==Unitary (-1)''F'' operator==
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
:^2=1
with the counit
:\epsilon((-1)^F)=1
and the coproduct
:\Delta (-1)^F=(-1)^F \otimes (-1)^F
and the antipode
: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 \mathbb_2. Supersymmetry comes in when introducing the nontrivial quasitriangular structure
:\mathcal=\frac\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.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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