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An involutive Yang–Baxter operator factors through the symmetric group

Statement

Let C be a monoidal category, let X∈C, and let R be a Yang–Baxter operator on X with R2=1X⊗X. Then for every n≥2 the homomorphism ρn ⁣:Bn→Aut⁡(X⊗n) of A Yang–Baxter operator gives braid-group representations factors through the canonical surjection πn ⁣:Bn→Sn of The braid group surjects onto the symmetric group: there is a unique homomorphism ψn ⁣:Sn→Aut⁡(X⊗n) with ρn=ψn∘πn.

Conversely, if ρn factors through πn for some n≥2, then Ri2=1X⊗n for every local operator Ri, because σi2 lies in the kernel of πn; and since ρ2(σ1)=R, if ρ2 factors through π2 then R2=1X⊗X. Consequently an involutive Yang–Baxter operator is exactly one whose two-strand braid action factors through S2, and an involutive Yang–Baxter operator has its braid actions factoring through Sn for every n.

Facts & Assumptions

Given: a monoidal category C, an object X, a Yang–Baxter operator R on X, the homomorphisms ρn of A Yang–Baxter operator gives braid-group representations with ρn(σi)=Ri the local operator of R at position i, and the surjection πn ⁣:Bn→Sn.

[L1]

The local operators satisfy the Artin relations of [L3] (Local Yang–Baxter operators satisfy the Artin relations).

[L2]

The symmetric group Sn has the Coxeter presentation with generators s1,…,sn−1 and relations si2=1, the braid relations and the distant-commutativity relations (The symmetric group has the Coxeter presentation).

[L3]

The braid group has the Artin presentation (The braid group by Artin presentation as used in A Yang–Baxter operator gives braid-group representations), and the canonical surjection πn sends σi to si (The braid group surjects onto the symmetric group).

[L4]

A generator assignment that respects the relators of a presented group extends uniquely to a homomorphism; precomposition with a surjection is injective on homomorphisms (Von Dyck's theorem: maps of generators that satisfy the relators extend uniquely from a presented group).

[L5]

The local operator at position i is 1X⊗(i−1)⊗R⊗1X⊗(n−i−1) in a strict model and its bracket-corrected conjugate in general (A Yang–Baxter operator gives braid-group representations, Local Yang–Baxter operators satisfy the Artin relations).

Proof

technique · direct
1.1L1L2L4L5givenconstruct

The direct implication. Assume R2=1X⊗X. By [L5] the local operator satisfies Ri2=1X⊗n: in the strict model Ri2 is the tensor product of identities with R2, and the bracket correction of [L5] is by a common canonical isomorphism, so it preserves the identity. By [L1] the operators Ri also satisfy the braid relations and the distant-commutativity relations. Hence the assignment si↦Ri from the Coxeter generators of Sn satisfies all relators of [L2], and [L4] gives a homomorphism ψn ⁣:Sn→Aut⁡(X⊗n) with ψn(si)=Ri.

1.2L2L3givenalgebra

The converse. Suppose ρn=ψ∘πn for some homomorphism ψ and some n≥2. Then for every i, Ri2=ρn(σi)2=ψ(πn(σi))2=ψ(πn(σi)2)=ψ(πn(σi2))=ψ(1)=1X⊗n, using that si2=1 in Sn by [L2] and that πn is a homomorphism [L3].

2.1L3L4step 1.1algebra

Factorization. Both ρn and ψn∘πn are homomorphisms Bn→Aut⁡(X⊗n), and on every Artin generator σi they agree: ρn(σi)=Ri=ψn(si)=ψn(πn(σi)) by [L3] and step 1.1. By the uniqueness clause of [L4] applied to the Artin presentation, ρn=ψn∘πn. Since πn is surjective, ψn is unique with this property: two such homomorphisms agree on the image of πn, which is all of Sn.

3.1L5step 1.2step 2.1algebra

The two-strand converse. For n=2 the only local operator is R1=R, so step 1.2 gives R2=1X⊗X as soon as ρ2 factors through π2. Hence an involutive Yang–Baxter operator is exactly one whose two-strand braid action factors through S2: one direction is step 1.1 with n=2 together with step 2.1, the other is the present step. For n≥3, step 1.2 gives the weaker identity (R2)⊗1X⊗(n−2)=1X⊗n; in a general monoidal category this whiskering does not by itself imply R2=1, which is why the criterion is stated at n=2.

4.1step 1.1step 1.2step 2.1step 3.1∎

Conclusion. Step 1.1 with step 2.1 shows that an involutive Yang–Baxter operator has all its braid actions factoring through the symmetric groups, and steps 1.2 and 3.1 give the converse at the level of the two-strand action: ρ2 factors through π2 exactly when R2=1. This proves the proposition. The argument uses only the Coxeter and Artin presentations and von Dyck's theorem, so no choice principle is used.

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