Lie bialgebra

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In mathematics, a Lie bialgebra is the Lie-theoretic case of a bialgebra: it is a set with a Lie algebra and a Lie coalgebra structure which are compatible.

It is a bialgebra where the multiplication is skew-symmetric and satisfies a dual Jacobi identity, so that the dual vector space is a Lie algebra, whereas the comultiplication is a 1-cocycle, so that the multiplication and comultiplication are compatible. The cocycle condition implies that, in practice, one studies only classes of bialgebras that are cohomologous to a Lie bialgebra on a coboundary.

They are also called Poisson-Hopf algebras, and are the Lie algebra of a Poisson–Lie group.

Lie bialgebras occur naturally in the study of the Yang–Baxter equations.

Definition

A vector space 𝔤 is a Lie bialgebra if it is a Lie algebra, and there is the structure of Lie algebra also on the dual vector space 𝔤∗ which is compatible. More precisely the Lie algebra structure on 𝔤 is given by a Lie bracket [ , ]:𝔤⊗𝔤→𝔤 and the Lie algebra structure on 𝔤∗ is given by a Lie bracket δ∗:𝔤∗⊗𝔤∗→𝔤∗. Then the map dual to δ∗ is called the cocommutator, δ:𝔤→𝔤⊗𝔤 and the compatibility condition is the following cocycle relation:

δ([X,Y])=(adX⊗1+1⊗adX)δ(Y)−(adY⊗1+1⊗adY)δ(X)

where adXY=[X,Y] is the adjoint. Note that this definition is symmetric and 𝔤∗ is also a Lie bialgebra, the dual Lie bialgebra.

Example

Let 𝔤 be any semisimple Lie algebra. To specify a Lie bialgebra structure we thus need to specify a compatible Lie algebra structure on the dual vector space. Choose a Cartan subalgebra 𝔱⊂𝔤 and a choice of positive roots. Let 𝔟±⊂𝔤 be the corresponding opposite Borel subalgebras, so that 𝔱=𝔟−∩𝔟+ and there is a natural projection π:𝔟±→𝔱. Then define a Lie algebra

𝔤′:={(X−,X+)∈𝔟−×𝔟+ | π(X−)+π(X+)=0}

which is a subalgebra of the product 𝔟−×𝔟+, and has the same dimension as 𝔤. Now identify 𝔤′ with dual of 𝔤 via the pairing

⟨(X−,X+),Y⟩:=K(X+−X−,Y)

where Y∈𝔤 and K is the Killing form. This defines a Lie bialgebra structure on 𝔤, and is the "standard" example: it underlies the Drinfeld-Jimbo quantum group. Note that 𝔤′ is solvable, whereas 𝔤 is semisimple.

Relation to Poisson–Lie groups

The Lie algebra 𝔤 of a Poisson–Lie group G has a natural structure of Lie bialgebra. In brief the Lie group structure gives the Lie bracket on 𝔤 as usual, and the linearisation of the Poisson structure on G gives the Lie bracket on 𝔤∗ (recalling that a linear Poisson structure on a vector space is the same thing as a Lie bracket on the dual vector space). In more detail, let G be a Poisson–Lie group, with f1,f2∈C∞(G) being two smooth functions on the group manifold. Let ξ=(df)e be the differential at the identity element. Clearly, ξ∈𝔤∗. The Poisson structure on the group then induces a bracket on 𝔤∗, as

[ξ1,ξ2]=(d{f1,f2})e

where {,} is the Poisson bracket. Given η be the Poisson bivector on the manifold, define ηR to be the right-translate of the bivector to the identity element in G. Then one has that

ηR:G→𝔤⊗𝔤

The cocommutator is then the tangent map:

δ=TeηR

so that

[ξ1,ξ2]=δ∗(ξ1⊗ξ2)

is the dual of the cocommutator.

See also

References

  • H.-D. Doebner, J.-D. Hennig, eds, Quantum groups, Proceedings of the 8th International Workshop on Mathematical Physics, Arnold Sommerfeld Institute, Claausthal, FRG, 1989, Springer-Verlag Berlin, Template:Isbn.
  • Vyjayanthi Chari and Andrew Pressley, A Guide to Quantum Groups, (1994), Cambridge University Press, Cambridge Template:Isbn.
  • Template:Cite journal