Ribbon Hopf algebra explained

A ribbon Hopf algebra

(A,\nabla,η,\Delta,\varepsilon,S,l{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:

\nu2=uS(u),S(\nu)=\nu,\varepsilon(\nu)=1

\Delta(\nu)=(l{R}21l{R}12)-1(\nu\nu)

where

u=\nabla(Sid)(l{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))=(l{R}21l{R}12)-2(uS(u)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

\nabla

is the multiplication map

\nabla:AAA

\Delta

is the co-product map

\Delta:AAA

η

is the unit operator

η:CA

\varepsilon

is the co-unit operator

\varepsilon:AC

S

is the antipode

S:AA

l{R}

is a universal R matrix

We assume that the underlying field

K

is

C

If

A

is finite-dimensional, one could equivalently call it ribbon Hopf if and only if its category of (say, left) modules is ribbon; if

A

is finite-dimensional and quasi-triangular, then it is ribbon if and only if its category of (say, left) modules is pivotal.

See also

References