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Parabolic freeness and bases of induced Hecke modules

Statement

Let (S,m), W, ℓ, R, and H be as in Coxeter matrices, the presented Coxeter group, reduced words, length, and standard parabolic subgroups and Universal parameters, the generic Coxeter Hecke algebra and generator conjugacy, and let J⊆S. Let HJ be the candidate submodule and let induction and restriction be as in Parabolic Hecke subalgebras, induction, and restriction. By Support, intrinsic parabolic presentations, minimal coset representatives and length additivity, with the type-A identification, WJ is the Coxeter group on J with the restricted matrix. The inherited parameters define its Hecke algebra over R by the same presentation.

Use the coset convention of Left and right cosets gH and Hg of a subgroup: the right cosets are WJd and the left cosets are dWJ. Define

DR(J):={d∈W:ℓ(sd)>ℓ(d) for every s∈J},DL(J):={d∈W:ℓ(ds)>ℓ(d) for every s∈J}.

These are respectively the unique minimal representatives of WJ\W and W/WJ.

  1. The candidate HJ=⨁u∈WJRTu is the subalgebra of H generated by Tj for j∈J. The homomorphism from the restricted-system Hecke algebra that sends each generator Tj to the same element of H is injective, with image HJ.

  2. There are direct-sum decompositions

H=⨁d∈DR(J)HJTdas a left HJ-module,H=⨁d∈DL(J)TdHJas a right HJ-module.

Thus the displayed Td are free module bases on the indicated sides. These assertions hold for arbitrary, possibly infinite, W.

  1. If M is a left HJ-module that is free over R with basis B, then H⊗HJM is free over R with basis
{Td⊗b:d∈DL(J), b∈B}.

For every left H-module N, the maps

Hom⁡H(H⊗HJM,N)⟶Hom⁡HJ(M,Res⁡JWN),F⟼[m↦F(1⊗m)],

and

g⟼[h⊗m↦h g(m)]

are inverse bijections. In particular, induction is left adjoint to restriction. If W is finite, the two bases of H over HJ have cardinality [W:WJ].

Facts & Assumptions

Given: A finite Coxeter matrix (S,m), its group W and length ℓ, the generic Hecke algebra H over R, a subset J⊆S, a left HJ-module M, and a left H-module N.

[F1]

The candidate parabolic module is HJ=⨁u∈WJRTu; induction is the balanced tensor product H⊗HJM, with (hk)⊗m=h⊗(km), and restriction uses the inclusion into H. (Parabolic Hecke subalgebras, induction, and restriction)

[F2]

For any finite Coxeter system and any commutative specialization of its universal parameter ring, the standard elements Tw form a basis of the Hecke algebra. (The standard basis of the generic Hecke algebra and base change)

[F3]

The reduced product Tw is well defined; the left and right length-multiplication rules hold for every s∈S,w∈W. (Reduced-word independence of T_w and the length-multiplication rules)

[F4]

Every right coset WJw has a unique minimal element d and a unique factorization w=ud with u∈WJ; then ℓ(w)=ℓ(u)+ℓ(d). Every left coset wWJ has a unique minimal element d and a unique factorization w=du with the same length additivity. (Support, intrinsic parabolic presentations, minimal coset representatives and length additivity, with the type-A identification)

[F5]

Under the library's coset convention, gH is a left coset and Hg is a right coset. (Left and right cosets gH and Hg of a subgroup)

[F6]

The restricted system on WJ has the same braid labels on J, and a Hecke algebra is the presented algebra with the quadratic and finite braid relations. Parameters constant on odd-edge components of S remain constant along odd-edge paths in J, so they specialize the restricted-system parameter ring to R. (Support, intrinsic parabolic presentations, minimal coset representatives and length additivity, with the type-A identification, Universal parameters, the generic Coxeter Hecke algebra and generator conjugacy)

Proof

Given: The data and hypotheses of the Statement.

1.1F1F3algebra

Let KJ:=⨁u∈WJRTu. If u∈WJ and j∈J, the left and right length-multiplication rules in [F3] express TjTu and TuTj as linear combinations of Tju,Tu and Tuj,Tu respectively; since ju,uj∈WJ, both products lie in KJ. Each Tu is a product of the generators indexed by J, so KJ is contained in the R-subalgebra they generate; conversely it is closed under multiplication by every such generator and contains 1, so every word in those generators lies in KJ. Hence KJ is exactly that generated subalgebra.

1.2F1F2F3F4F5

For each w∈W, [F4] gives a unique factorization w=ud with u∈WJ and d∈DR(J) and ℓ(w)=ℓ(u)+ℓ(d). Thus WJd is the right coset represented by d under [F5]. Choose reduced expressions for u and d; their concatenation has length ℓ(u)+ℓ(d)=ℓ(ud) and so is reduced, giving Tw=TuTd by [F3]. Thus the elements of HJTd span H. If a finite sum ∑dhdTd=0 with hd∈HJ is given, expand each hd as a finite sum ∑u∈WJru,dTu using [F1]. The resulting sum is ∑u,dru,dTud=0. Unique factorization makes the elements ud distinct for distinct pairs (u,d); linear independence of the standard basis [F2] forces every ru,d=0. This proves the left-module direct sum and its basis.

1.3F1F2F3F4F5

For each w∈W, the left-coset part of [F4] gives a unique factorization w=du with d∈DL(J), u∈WJ, and ℓ(w)=ℓ(d)+ℓ(u). By [F5], dWJ is the left coset represented by d. Reduced expressions for d followed by u concatenate to a reduced expression of du, so Tw=TdTu by [F3]. Hence the elements of TdHJ span H. If ∑dTdhd=0, expand hd=∑u∈WJrd,uTu; unique left-coset factorization makes all du distinct, and [F2] then forces every coefficient to vanish. This proves the right-module direct sum and its basis.

2.1F1F2F4F6step 1.1

By [F4], (WJ,J) is a Coxeter system. Any odd-edge path in J is also an odd-edge path in S, so the inherited parameters agree along every odd component of J and give a ring map from the restricted system's universal parameter ring to R. Thus [F6] supplies a homomorphism from the restricted Hecke presentation to H sending each Tj to Tj. Apply the standard-basis theorem [F2] to the restricted system and this parameter map: its standard elements Tu form an R-basis. Their images are the correspondingly named elements of the ambient H-basis, so the map is injective; its image is KJ by step 1.1 and because every u∈WJ has a word in J. Thus the candidate in [F1] is an embedded subalgebra, proving part 1.

2.2F1step 1.3constructalgebra

By step 1.3, every h∈H has a unique finite expansion h=∑d∈DL(J)Tdkd with kd∈HJ. Define Φ:⨁d∈DL(J)M→H⊗HJM by (md)d↦∑dTd⊗md, and define Ψ(h⊗m):=(kdm)d. The latter respects the balancing relation: the coefficients of hk are kdk, so Ψ(hk⊗m)=(kd(km))d=Ψ(h⊗km). Uniqueness of the expansion shows ΨΦ and ΦΨ are identities. Thus H⊗HJM≅⨁d∈DL(J)M; if B is an R-basis of M, the displayed tensors form an R-basis.

3.1F1step 2.2algebra

For an HJ-linear map g:M→Res⁡JWN, the formula g~(h⊗m)=hg(m) is balanced because hkg(m)=hg(km), and it is H-linear. Conversely, if F:H⊗HJM→N is H-linear, m↦F(1⊗m) is HJ-linear since 1⊗km=k⊗m. The two constructions are inverse: evaluation at 1⊗m recovers g(m), and H-linearity gives F(h⊗m)=hF(1⊗m). This proves the adjunction.

4.1F2F4step 1.2step 1.3step 3.1∎

The coset decompositions, their independence arguments, and the adjunction used no finiteness of W and no choice of coset representatives: [F4] supplies each unique minimal representative. If W is finite, each coset has ∣WJ∣ elements, the cosets partition W, and the number of representatives is ∣W∣/∣WJ∣=[W:WJ]. All coefficient arguments use standard bases and remain valid after any commutative base change of R because the standard basis in [F2] does.

Depends on

Used by

Cited to discharge well-definedness by Parabolic Hecke subalgebras, induction, and restriction.

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