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The Hecke quadratic relation from the Soergel square

Example

Fix n≥2 and a simple reflection si, and let A=Z[v,v−1] with q=v−2, Hn the type-A Hecke algebra with normalized generators Hi=v(Ti+1), and Φ:K0split(SBimn)→HSn the algebra isomorphism of The split Grothendieck group of the Soergel category is the type-A Hecke algebra. Then:

  1. The class identity. Taking split classes of the rank-one square Bi⊗RBi≅Bi(1)⊕Bi(−1) gives [Bi]2=[Bi⊗RBi]=[Bi(1)]+[Bi(−1)]=v[Bi]+v−1[Bi]=(v+v−1)[Bi] in K0split(SBimn), and applying Φ gives Hi2=(v+v−1)Hi in HSn.
  2. The standard quadratic relation. Substituting Hi=v(Ti+1) into Hi2=(v+v−1)Hi and cancelling the unit v gives v(Ti+1)2=(v+v−1)(Ti+1), which expands to vTi2+(v−v−1)Ti−v−1=0 and, after multiplying by v−1, to Ti2+(1−v−2)Ti−v−2=0,i.e.(Ti−v−2)(Ti+1)=0. This is exactly the quadratic relation Ti2=(q−1)Ti+q of the Hecke algebra in the normalization of The type-A Hecke algebra in Soergel normalization.
  3. Equivalence of the two forms. Conversely, (Ti−v−2)(Ti+1)=0 multiplied by v2 reads v2Ti2+(v2−1)Ti−1=0, and Hi2−(v+v−1)Hi=v2(Ti+1)2−(v2+1)(Ti+1)=v2Ti2+(v2−1)Ti−1, so the single-generator identities Hi2=(v+v−1)Hi and (Ti−v−2)(Ti+1)=0 are equivalent over A.

Facts & Assumptions

Given: The type-A Soergel category SBimn with its split Grothendieck ring, the Hecke algebra Hn over A=Z[v,v−1] with q=v−2, a simple reflection si, and the isomorphism Φ of Z[v,v−1]-algebras with Φ([Bi])=Hi and Φ(vX)=vΦ(X).

[F1]

The rank-one square: for a simple reflection si there is a degree-zero isomorphism of graded bimodules Bi⊗RBi≅Bi(1)⊕Bi(−1), the summands being free of rank two on each side (The rank-one Soergel bimodule square splits).

[F2]

In the split Grothendieck ring the product is [X][Y]=[X⊗Y], the shift satisfies v[X]=[X(1)]=[X{−1}] and v−1[X]=[X(−1)], and the unit is [R] (Split Grothendieck rings of the type-A Soergel categories).

[F3]

There is an isomorphism of Z[v,v−1]-algebras Φ:K0split(SBimn)→HSn with Φ([Bi])=Hi=v(Ti+1) and Φ(vX)=v Φ(X), and the classes satisfy [Bi]2=(v+v−1)[Bi] (The split Grothendieck group of the Soergel category is the type-A Hecke algebra).

[F4]

Hn is presented by the generators Ti with Ti2=(q−1)Ti+q, equivalently (Ti−q)(Ti+1)=0, where q=v−2; the normalized generators satisfy Hi=v(Ti+1), Hi2=(v+v−1)Hi and Ti=v−1Hi−1, and v is a unit of the Laurent ring A (The type-A Hecke algebra in Soergel normalization).

Proof

1.1

The class identity: by [F1] the bimodules Bi⊗RBi and Bi(1)⊕Bi(−1) are isomorphic, so their classes in K0split(SBimn) coincide; the product and shift rules of [F2] turn this into [Bi]2=[Bi⊗RBi]=[Bi(1)]+[Bi(−1)]=v[Bi]+v−1[Bi], and [F2] also gives v[Bi]+v−1[Bi]=(v+v−1)[Bi], an identity in the ring.

F1F2
2.1

The Hecke form: applying the algebra homomorphism Φ of [F3], which is Z[v,v−1]-linear and satisfies Φ([Bi])=Hi, to the identity of step 1.1 gives Hi2=Φ([Bi]2)=Φ((v+v−1)[Bi])=(v+v−1)Hi in HSn.

F3step 1.1
3.1

The translation: by [F4] Hi=v(Ti+1) and Ti=v−1Hi−1, so squaring Hi=v(Ti+1) and substituting the relation of step 2.1 gives v2(Ti+1)2=Hi2=(v+v−1)Hi=(v+v−1)v(Ti+1); multiplying both sides by the unit v−1 gives v(Ti+1)2=(v+v−1)(Ti+1).

F4step 2.1
4.1

The expansion: expanding v(Ti+1)2=v(Ti2+2Ti+1) and collecting terms in the identity of step 3.1 gives vTi2+(2v−v−v−1)Ti+(v−v−v−1)=0, that is vTi2+(v−v−1)Ti−v−1=0; multiplying by the unit v−1 gives Ti2+(1−v−2)Ti−v−2=0.

F4step 3.1
5.1

The factorisation: with q=v−2, expanding the product (Ti−q)(Ti+1)=Ti2+(1−q)Ti−q shows that the relation of step 4.1 is exactly (Ti−v−2)(Ti+1)=0, which is the quadratic relation Ti2=(q−1)Ti+q of [F4].

F4step 4.1
6.1

The converse: if (Ti−v−2)(Ti+1)=0, then Ti2+(1−v−2)Ti−v−2=0 and multiplication by v2 gives v2Ti2+(v2−1)Ti−1=0; expanding the difference in the Hecke algebra gives Hi2−(v+v−1)Hi=v2(Ti+1)2−(v2+1)(Ti+1)=v2(Ti2+2Ti+1)−(v2+1)Ti−(v2+1)=v2Ti2+(v2−1)Ti−1=0, so Hi2=(v+v−1)Hi; the two single-generator relations are therefore equivalent under Hi=v(Ti+1), with v a unit of A used in both directions.

F4step 5.1
7.1

Conclusion: the rank-one square produces [Bi]2=(v+v−1)[Bi] in K0split(SBimn) and, through the isomorphism Φ, the Hecke identity Hi2=(v+v−1)Hi; rewriting Hi=v(Ti+1) expands this into Ti2+(1−v−2)Ti−v−2=0, that is (Ti−v−2)(Ti+1)=0, which is the quadratic relation of the Hecke algebra in the standard generators, and the two displayed forms are equivalent by steps 3.1, 4.1, 5.1 and 6.1. Only identities between elements of A and of Hn are manipulated, so no choice principle is used. ∎

F3F4step 1.1step 6.1

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