• Source: Quasi-Hopf algebra
  • A quasi-Hopf algebra is a generalization of a Hopf algebra, which was defined by the Russian mathematician Vladimir Drinfeld in 1989.
    A quasi-Hopf algebra is a quasi-bialgebra






    B

    A




    =
    (


    A


    ,
    Δ
    ,
    ε
    ,
    Φ
    )


    {\displaystyle {\mathcal {B_{A}}}=({\mathcal {A}},\Delta ,\varepsilon ,\Phi )}

    for which there exist



    α
    ,
    β



    A




    {\displaystyle \alpha ,\beta \in {\mathcal {A}}}

    and a bijective antihomomorphism S (antipode) of





    A




    {\displaystyle {\mathcal {A}}}

    such that







    i


    S
    (

    b

    i


    )
    α

    c

    i


    =
    ε
    (
    a
    )
    α


    {\displaystyle \sum _{i}S(b_{i})\alpha c_{i}=\varepsilon (a)\alpha }








    i



    b

    i


    β
    S
    (

    c

    i


    )
    =
    ε
    (
    a
    )
    β


    {\displaystyle \sum _{i}b_{i}\beta S(c_{i})=\varepsilon (a)\beta }


    for all



    a



    A




    {\displaystyle a\in {\mathcal {A}}}

    and where




    Δ
    (
    a
    )
    =



    i



    b

    i




    c

    i




    {\displaystyle \Delta (a)=\sum _{i}b_{i}\otimes c_{i}}


    and







    i



    X

    i


    β
    S
    (

    Y

    i


    )
    α

    Z

    i


    =

    I

    ,


    {\displaystyle \sum _{i}X_{i}\beta S(Y_{i})\alpha Z_{i}=\mathbb {I} ,}








    j


    S
    (

    P

    j


    )
    α

    Q

    j


    β
    S
    (

    R

    j


    )
    =

    I

    .


    {\displaystyle \sum _{j}S(P_{j})\alpha Q_{j}\beta S(R_{j})=\mathbb {I} .}


    where the expansions for the quantities



    Φ


    {\displaystyle \Phi }

    and




    Φ


    1




    {\displaystyle \Phi ^{-1}}

    are given by




    Φ
    =



    i



    X

    i




    Y

    i




    Z

    i




    {\displaystyle \Phi =\sum _{i}X_{i}\otimes Y_{i}\otimes Z_{i}}


    and





    Φ


    1


    =



    j



    P

    j




    Q

    j




    R

    j


    .


    {\displaystyle \Phi ^{-1}=\sum _{j}P_{j}\otimes Q_{j}\otimes R_{j}.}


    As for a quasi-bialgebra, the property of being quasi-Hopf is preserved under twisting.


    Usage


    Quasi-Hopf algebras form the basis of the study of Drinfeld twists and the representations in terms of F-matrices associated with finite-dimensional irreducible representations of quantum affine algebra. F-matrices can be used to factorize the corresponding R-matrix. This leads to applications in Statistical mechanics, as quantum affine algebras, and their representations give rise to solutions of the Yang–Baxter equation, a solvability condition for various statistical models, allowing characteristics of the model to be deduced from its corresponding quantum affine algebra. The study of F-matrices has been applied to models such as the Heisenberg XXZ model in the framework of the algebraic Bethe ansatz. It provides a framework for solving two-dimensional integrable models by using the quantum inverse scattering method.


    See also


    Quasitriangular Hopf algebra
    Quasi-triangular quasi-Hopf algebra
    Ribbon Hopf algebra


    References


    Vladimir Drinfeld, "Quasi-Hopf algebras", Leningrad Math J. 1 (1989), 1419-1457
    J. M. Maillet and J. Sanchez de Santos, Drinfeld Twists and Algebraic Bethe Ansatz, Amer. Math. Soc. Transl. (2) Vol. 201, 2000

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