Ribbon Hopf algebra

A ribbon Hopf algebra (A,m,\Delta,u,\varepsilon,S,\mathcal{R},\nu) is a quasitriangular Hopf algebra which possess an invertible central element \nu more commonly known as the ribbon element, such that the following conditions hold:

\nu^{2}=uS(u), \; S(\nu)=\nu, \; \varepsilon (\nu)=1
\Delta (\nu)=(\mathcal{R}_{21}\mathcal{R}_{12})^{-1}(\nu \otimes \nu )

where u=m(S\otimes \text{id})(\mathcal{R}_{21}). Note that the element u exists for any quasitriangular Hopf algebra, and uS(u) must always be central and satisfies S(uS(u))=uS(u), \varepsilon(uS(u))=1, \Delta(uS(u)) = 
(\mathcal{R}_{21}\mathcal{R}_{12})^{-2}(uS(u) \otimes uS(u)), so that all that is required is that it have a central square root with the above properties.

Here

 A is a vector space
 m is the multiplication map m:A \otimes A \rightarrow A
 \Delta is the co-product map \Delta: A \rightarrow A \otimes A
 u is the unit operator u:\mathbb{C} \rightarrow A
 \varepsilon is the co-unit operator \varepsilon: A \rightarrow \mathbb{C}
 S is the antipode S: A\rightarrow A
\mathcal{R} is a universal R matrix

We assume that the underlying field K is \mathbb{C}

See also

References

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