Quasi-bialgebra

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Template:Short description In mathematics, quasi-bialgebras are a generalization of bialgebras: they were first defined by the Ukrainian mathematician Vladimir Drinfeld in 1990. A quasi-bialgebra differs from a bialgebra by having coassociativity replaced by an invertible element Ξ¦ which controls the non-coassociativity. One of their key properties is that the corresponding category of modules forms a tensor category.

Definition

A quasi-bialgebra β„¬π’œ=(π’œ,Ξ”,Ξ΅,Ξ¦,l,r) is an algebra π’œ over a field 𝔽 equipped with morphisms of algebras

Ξ”:π’œβ†’π’œβŠ—π’œ
Ξ΅:π’œβ†’π”½

along with invertible elements Ξ¦βˆˆπ’œβŠ—π’œβŠ—π’œ, and r,l∈A such that the following identities hold:

(idβŠ—Ξ”)βˆ˜Ξ”(a)=Ξ¦[(Ξ”βŠ—id)βˆ˜Ξ”(a)]Ξ¦βˆ’1,βˆ€aβˆˆπ’œ
[(idβŠ—idβŠ—Ξ”)(Ξ¦)] [(Ξ”βŠ—idβŠ—id)(Ξ¦)]=(1βŠ—Ξ¦) [(idβŠ—Ξ”βŠ—id)(Ξ¦)] (Ξ¦βŠ—1)
(Ξ΅βŠ—id)(Ξ”a)=lβˆ’1al,(idβŠ—Ξ΅)βˆ˜Ξ”=rβˆ’1ar,βˆ€aβˆˆπ’œ
(idβŠ—Ξ΅βŠ—id)(Ξ¦)=rβŠ—lβˆ’1.

Where Ξ” and Ο΅ are called the comultiplication and counit, r and l are called the right and left unit constraints (resp.), and Ξ¦ is sometimes called the Drinfeld associator.[1]Template:Rp This definition is constructed so that the category π’œβˆ’Mod is a tensor category under the usual vector space tensor product, and in fact this can be taken as the definition instead of the list of above identities.[1]Template:Rp Since many of the quasi-bialgebras that appear "in nature" have trivial unit constraints, ie. l=r=1 the definition may sometimes be given with this assumed.[1]Template:Rp Note that a bialgebra is just a quasi-bialgebra with trivial unit and associativity constraints: l=r=1 and Ξ¦=1βŠ—1βŠ—1.

Braided quasi-bialgebras

A braided quasi-bialgebra (also called a quasi-triangular quasi-bialgebra) is a quasi-bialgebra whose corresponding tensor category π’œβˆ’Mod is braided. Equivalently, by analogy with braided bialgebras, we can construct a notion of a universal R-matrix which controls the non-cocommutativity of a quasi-bialgebra. The definition is the same as in the braided bialgebra case except for additional complications in the formulas caused by adding in the associator.

Proposition: A quasi-bialgebra (π’œ,Ξ”,Ο΅,Ξ¦,l,r) is braided if it has a universal R-matrix, ie an invertible element Rβˆˆπ’œβŠ—π’œ such that the following 3 identities hold:

(Ξ”op)(a)=RΞ”(a)Rβˆ’1
(idβŠ—Ξ”)(R)=(Ξ¦231)βˆ’1R13Ξ¦213R12(Ξ¦213)βˆ’1
(Ξ”βŠ—id)(R)=(Ξ¦321)R13(Ξ¦213)βˆ’1R23Ξ¦123

Where, for every a1βŠ—...βŠ—akβˆˆπ’œβŠ—k, ai1i2...in is the monomial with aj in the ijth spot, where any omitted numbers correspond to the identity in that spot. Finally we extend this by linearity to all of π’œβŠ—k.[1]Template:Rp

Again, similar to the braided bialgebra case, this universal R-matrix satisfies (a non-associative version of) the Yang–Baxter equation:

R12Ξ¦321R13(Ξ¦132)βˆ’1R23Ξ¦123=Ξ¦321R23(Ξ¦231)βˆ’1R13Ξ¦213R12[1]Template:Rp

Twisting

Given a quasi-bialgebra, further quasi-bialgebras can be generated by twisting (from now on we will assume r=l=1) .

If β„¬π’œ is a quasi-bialgebra and Fβˆˆπ’œβŠ—π’œ is an invertible element such that (Ξ΅βŠ—id)F=(idβŠ—Ξ΅)F=1, set

Ξ”(a)=FΞ”(a)Fβˆ’1,βˆ€aβˆˆπ’œ
Ξ¦=(1βŠ—F) ((idβŠ—Ξ”)F) Ξ¦ ((Ξ”βŠ—id)Fβˆ’1) (Fβˆ’1βŠ—1).

Then, the set (π’œ,Ξ”,Ξ΅,Ξ¦) is also a quasi-bialgebra obtained by twisting β„¬π’œ by F, which is called a twist or gauge transformation.[1]Template:Rp If (π’œ,Ξ”,Ξ΅,Ξ¦) was a braided quasi-bialgebra with universal R-matrix R , then so is (π’œ,Ξ”,Ξ΅,Ξ¦) with universal R-matrix F21RFβˆ’1 (using the notation from the above section).[1]Template:Rp However, the twist of a bialgebra is only in general a quasi-bialgebra. Twistings fulfill many expected properties. For example, twisting by F1 and then F2 is equivalent to twisting by F2F1, and twisting by F then Fβˆ’1 recovers the original quasi-bialgebra.

Twistings have the important property that they induce categorical equivalences on the tensor category of modules:

Theorem: Let β„¬π’œ, β„¬π’œ be quasi-bialgebras, let ℬ'π’œ be the twisting of β„¬π’œ by F, and let there exist an isomorphism: Ξ±:β„¬π’œβ†’β„¬'π’œ. Then the induced tensor functor (Ξ±βˆ—,id,Ο•2F) is a tensor category equivalence between π’œβˆ’mod and π’œβˆ’mod. Where Ο•2F(vβŠ—w)=Fβˆ’1(vβŠ—w). Moreover, if Ξ± is an isomorphism of braided quasi-bialgebras, then the above induced functor is a braided tensor category equivalence.[1]Template:Rp

Usage

Quasi-bialgebras form the basis of the study of quasi-Hopf algebras and further to 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 XXZ in the framework of the Algebraic Bethe ansatz.

See also

References

  1. ↑ 1.0 1.1 1.2 1.3 1.4 1.5 1.6 1.7 C. Kassel. "Quantum Groups". Graduate Texts in Mathematics Springer-Verlag. Template:ISBN

Further reading

  • 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