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Coxeter quotient at the Hecke specialization q=1

Statement

Let n≥2, V be a complex vector space, Ui∈End⁡C(V), δ∈C, and q∈C× satisfy δ=q+q−1 and

Ui2=δUi,UiUi+1Ui=Ui,Ui+1UiUi+1=Ui+1,UiUj=UjUi(∣i−j∣>1).

Put Bi=qIV−Ui, and let ρn:Bn→GL⁡(V) be the homomorphism ρn(σi)=Bi from the preceding Temperley–Lieb–Hecke construction. At q=1 one has δ=2 and Bi=IV−Ui. These operators satisfy Bi2=IV, so ρn factors through the canonical quotient πn:Bn→Sn as a representation Sn→GL⁡(V). The q=1 Hecke generator relations are then the type-A Coxeter relations. For general q, the roots of the quadratic relation are q and −q−1; they coincide when q2=−1, and no diagonalizability is asserted. Involutivity is not imposed by the Hecke relation and need not hold.

Facts & Assumptions

Given: The operator family, parameter relation, and braid-group representation from Temperley–Lieb projectors give a Hecke braid representation.

[F1]

Temperley–Lieb projectors give a Hecke braid representation: the Bi satisfy the adjacent braid and distant-commutation relations and (Bi−qIV)(Bi+q−1IV)=0.

[F2]

The generic type-A Hecke algebra: the specialized generators have quadratic relation (Ti−v)(Ti+1)=0, together with type-A braid and distant-commutation relations.

[F3]

The symmetric group has the Coxeter presentation: the adjacent transpositions si present Sn with relators si2=1, the adjacent braid relations, and distant commutation.

[F4]

The braid group surjects onto the symmetric group: the canonical quotient sends σi↦si (in the library's transported indexing convention).

[F5]

Von Dyck's theorem: maps of generators that satisfy the relators extend uniquely from a presented group: a generator assignment satisfying all presentation relators extends uniquely to a homomorphism.

Proof

1.1F1givenalgebra

At q=1, the parameter relation gives δ=2. For every i, Bi2=(IV−Ui)2=IV−2Ui+Ui2=IV, using Ui2=2Ui from [F1].

1.2F1algebra

The general quadratic in [F1] factors as (Bi−qIV)(Bi+q−1IV)=0, whose scalar roots are q and −q−1; equality of those roots is equivalent to q2=−1. This polynomial relation alone asserts no diagonalization.

2.1F1F3F5step 1.1construct

By [F1], the Bi also satisfy the adjacent braid and distant-commutation relators. Along with step 1.1, these are exactly the Coxeter relators in [F3], so [F5] gives a homomorphism ρ~n:Sn→GL⁡(V) with ρ~n(si)=Bi.

3.1F1F4step 2.1algebra

The composite ρ~n∘πn, with πn from [F4], and the braid representation ρn from [F1] agree on every generator σi, since both send it to Bi. The generators determine a homomorphism from Bn, so ρn=ρ~n∘πn.

3.2F1F2F3step 1.1step 2.1algebra

The Hecke representation of the preceding theorem sends Ti to qBi, which equals Bi at q=1. The generic relation (Ti−v)(Ti+1)=0 in [F2] then becomes Ti2=IV; together with the braid and distant relations these are exactly the Coxeter generator relations in [F3]. Thus the specialized Hecke generators act by the same generator assignment as ρ~n.

4.1F1algebra∎

To see that involutivity is not forced for general q, take V=C, Ui=0 for every i, q=2, and δ=5/2. All Temperley–Lieb relations hold, while Bi=2IV and Bi2=4IV≠IV.

Remarks

At q=1 the Coxeter quotient is obtained by adding involutions to the braid presentation. At general q, the representation remains a braid/Hecke representation; no symmetric-group action follows unless the involution relations are separately verified.

Depends on

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