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Temperley–Lieb projectors give a Hecke braid representation

Statement

For a complex vector space V, let End⁡C(V) be its set of complex-linear endomorphisms, with composition as multiplication, and define GL⁡(V) to be the group of bijective elements of End⁡C(V). A complex Hilbert space is a complete complex inner-product space; here the inner product is linear in its first variable and ∥x∥:=⟨x,x⟩. A linear operator A:V→V on such a space is bounded if some C<∞ satisfies ∥Ax∥≤C∥x∥ for every x∈V, self-adjoint if ⟨Ax,y⟩=⟨x,Ay⟩ for all x,y∈V, and unitary if it is surjective and preserves the inner product. In the formulas below, IV denotes the identity map of V.

Let n≥2, let V be a complex vector space, and let U1,…,Un−1∈End⁡C(V). Suppose δ∈C, q∈C×, and δ=q+q−1, and assume

Ui2=δUi(1≤i<n),UiUi+1Ui=Ui,Ui+1UiUi+1=Ui+1(1≤i≤n−2),UiUj=UjUi(∣i−j∣>1).

Define Bi:=qIV−Ui. Then each Bi is invertible with Bi−1=q−1IV−Ui; the Bi satisfy the Artin braid and far-commutation relations; and

(Bi−qIV)(Bi+q−1IV)=0.

Thus σi↦Bi defines a group homomorphism Bn→GL⁡(V). If Hv(n) is the generic type-A Hecke algebra with (Ti−v)(Ti+1)=0, its scalar specialization Hq2(n) has a unital algebra representation Ti↦qBi. This is the standard Hecke normalization because (qBi−q2IV)(qBi+IV)=0. If V is a complex Hilbert space and each Ui is bounded self-adjoint, then δ∈R and ∣q∣=1 imply that each Bi is unitary. No faithfulness, diagonalizability, or physical realization is asserted.

Facts & Assumptions

Given: n≥2, the operator family on V, and q,δ satisfying the hypotheses in the Statement.

[F1]

Vacuum-channel anyonic projectors satisfy Temperley–Lieb relations: on the repeated-a path space Ui=δaPi with δa=κada; its Statement gives the square relation, UiUi+1Ui=Ui, and distant commutation.

[F2]

Vacuum projectors obey the reverse adjacent Temperley–Lieb relation: on the same path space the omitted reverse relation Ui+1UiUi+1=Ui+1 holds, so [F1] and [F2] supply the complete adjacent Temperley–Lieb relations.

[F3]

The generic type-A Hecke algebra: Hv(n) is presented by generators Ti, the type-A braid and distant-commutation relations, and (Ti−v)(Ti+1)=0; specialization at a unit v=q2 preserves this presentation.

[F4]

The Hecke generators satisfy the Artin relations and are units: the generators of the Hecke tower are units and the standard assignment σi↦Ti defines the braid-group homomorphism into the Hecke unit group.

[F5]

The braid group by Artin presentation: Bn has precisely the adjacent braid and distant-commutation relators displayed in the Statement.

[F6]

Von Dyck's theorem: maps of generators that satisfy the relators extend uniquely from a presented group: a map from the generators of a presented group extends uniquely to a homomorphism when every defining relator maps to the identity.

Proof

1.1givenalgebra

Since Ui2=δUi and δ=q+q−1, (qIV−Ui)(q−1IV−Ui)=IV−(q+q−1)Ui+Ui2=IV. The product in the reverse order is the same polynomial in Ui, so Bi−1=q−1IV−Ui.

1.2givenalgebra

For adjacent i,i+1, expansion and the square and adjacent Temperley–Lieb relations give (qIV−Ui)(qIV−Ui+1)(qIV−Ui)−(qIV−Ui+1)(qIV−Ui)(qIV−Ui+1)=−(q2−qδ+1)(Ui−Ui+1)=0, since qδ=q2+1. Thus the adjacent braid relation holds.

2.1givenstep 1.1algebra

We have Bi−qIV=−Ui and Bi+q−1IV=δIV−Ui; hence (Bi−qIV)(Bi+q−1IV)=−δUi+Ui2=0.

2.2F5givenstep 1.1algebra

If ∣i−j∣>1, then BiBj−BjBi=UiUj−UjUi=0. Together with step 1.1, the Bi are units satisfying all relators of [F5].

3.1F5F6step 2.2construct

By [F6] applied to [F5] and the assignment σi↦Bi, step 2.2 supplies a unique homomorphism ρn:Bn→GL⁡(V) with ρn(σi)=Bi.

3.2F3step 2.1step 1.2step 2.2algebra

Let T~i:=qBi. They satisfy the braid and distant relations by steps 1.2–2.2, and (T~i−q2IV)(T~i+IV)=q2(Bi−qIV)(Bi+q−1IV)=0. Consequently the generator map from the free unital algebra kills every defining relator of Hq2(n), so its defining ideal lies in the kernel and the map factors through the quotient Hq2(n). This gives the stated unital Hecke-algebra representation.

4.1F3F4step 3.2construct

Apply the coefficient map Z[v±1,z]→C, v↦q2, z↦0, to the Hecke tower in [F4]. By its defining scalar-extension construction and the specialization in [F3], the resulting algebra is Hq2(n); base change carries [F4]'s braid homomorphism to ηn:Bn→Hq2(n)× with ηn(σi)=Ti. Composing with Φn from step 3.2 sends σi to qBi, identifying the chosen normalization against the standard Hecke generator assignment. No Markov trace or link-invariant claim is used.

5.1F1F2givenstep 1.1algebra∎

If V is a complex Hilbert space, Ui is bounded self-adjoint, δ∈R, and ∣q∣=1, then for all x,y∈V self-adjointness and Ui2=δUi give ⟨Bix,Biy⟩=∣q∣2⟨x,y⟩−(q+q‾)⟨x,Uiy⟩+δ⟨x,Uiy⟩=⟨x,y⟩, since q−1=q‾ and δ=q+q−1. Thus Bi preserves the inner product; it is surjective by its inverse in step 1.1, and so it is unitary by the convention in the Statement. For the repeated-a anyonic path family, [F1] and [F2] supply both adjacent relations, the square relation, and distant commutation with the signed δa=κada; whenever q+q−1=δa, it therefore meets the operator hypotheses of this theorem. No sign is replaced by +1.

Remarks

The finite-dimensional anyonic path-space operators are one algebraic source of the Ui. The conclusion is conditional on their displayed relations and signed loop parameter. It does not identify these operators with an experimentally realized adiabatic exchange.

Depends on

Dependency tree · 2 levels

Sources