Birman–Wenzl algebra

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Short description: 2-parameter family of algebras with the Hecke algebra of the symmetric group as a quotient

In mathematics, the Birman–Murakami–Wenzl (BMW) algebra, introduced by Joan Birman and Hans Wenzl (1989) and Jun Murakami (1987), is a two-parameter family of algebras Cn(,m) of dimension 135(2n1) having the Hecke algebra of the symmetric group as a quotient. It is related to the Kauffman polynomial of a link. It is a deformation of the Brauer algebra in much the same way that Hecke algebras are deformations of the group algebra of the symmetric group.

Definition

For each natural number n, the BMW algebra Cn(,m) is generated by G1±1,G2±1,,Gn1±1,E1,E2,,En1 and relations:

GiGj=GjGi,if|ij|2,
GiGi+1Gi=Gi+1GiGi+1,         EiEi±1Ei=Ei,
Gi+Gi1=m(1+Ei),
Gi±1GiEi±1=EiGi±1Gi=EiEi±1,      Gi±1EiGi±1=Gi1Ei±1Gi1,
Gi±1EiEi±1=Gi1Ei±1,      Ei±1EiGi±1=Ei±1Gi1,
GiEi=EiGi=l1Ei,     EiGi±1Ei=lEi.

These relations imply the further relations:

EiEj=EjEi,if|ij|2,
(Ei)2=(m1(l+l1)1)Ei,
Gi2=m(Gi+l1Ei)1.

This is the original definition given by Birman and Wenzl. However a slight change by the introduction of some minus signs is sometimes made, in accordance with Kauffman's 'Dubrovnik' version of his link invariant. In that way, the fourth relation in Birman & Wenzl's original version is changed to

  1. (Kauffman skein relation)
    GiGi1=m(1Ei),

Given invertibility of m, the rest of the relations in Birman & Wenzl's original version can be reduced to

  1. (Idempotent relation)
    (Ei)2=(m1(ll1)+1)Ei,
  2. (Braid relations)
    GiGj=GjGi,if |ij|2, and GiGi+1Gi=Gi+1GiGi+1,
  3. (Tangle relations)
    EiEi±1Ei=Ei and GiGi±1Ei=Ei±1Ei,
  4. (Delooping relations)
    GiEi=EiGi=l1Ei and EiGi±1Ei=lEi.

Properties

Isomorphism between the BMW algebras and Kauffman's tangle algebras

It is proved by (Morton Wassermann) that the BMW algebra Cn(,m) is isomorphic to the Kauffman's tangle algebra KTn, the isomorphism ϕ:CnKTn is defined by
and

Baxterisation of Birman–Murakami–Wenzl algebra

Define the face operator as

Ui(u)=1isinusinλsinμ(ei(uλ)Giei(uλ)Gi1),

where λ and μ are determined by

2cosλ=1+(ll1)/m

and

2cosλ=1+(ll1)/(λsinμ).

Then the face operator satisfies the Yang–Baxter equation.

Ui+1(v)Ui(u+v)Ui+1(u)=Ui(u)Ui+1(u+v)Ui(v)

Now Ei=Ui(λ) with

ρ(u)=sin(λu)sin(μ+u)sinλsinμ.

In the limits u±i, the braids Gj± can be recovered up to a scale factor.

History

In 1984, Vaughan Jones introduced a new polynomial invariant of link isotopy types which is called the Jones polynomial. The invariants are related to the traces of irreducible representations of Hecke algebras associated with the symmetric groups. (Murakami 1987) showed that the Kauffman polynomial can also be interpreted as a function F on a certain associative algebra. In 1989, (Birman Wenzl) constructed a two-parameter family of algebras Cn(,m) with the Kauffman polynomial Kn(,m) as trace after appropriate renormalization.

References

  • Birman, Joan S.; Wenzl, Hans (1989), "Braids, link polynomials and a new algebra", Transactions of the American Mathematical Society (American Mathematical Society) 313 (1): 249–273, doi:10.1090/S0002-9947-1989-0992598-X, ISSN 0002-9947 
  • Murakami, Jun (1987), "The Kauffman polynomial of links and representation theory", Osaka Journal of Mathematics 24 (4): 745–758, ISSN 0030-6126, http://projecteuclid.org/euclid.ojm/1200780357 
  • Morton, Hugh R.; Wassermann, Antony J. (1989). "A basis for the Birman–Wenzl algebra". arXiv:1012.3116 [math.QA].