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Unequal-Parameter Hecke Cells and Representations

1 · Prerequisites

2 · Summary

This page develops the weighted Hecke algebra and its cell quotients with a totally ordered abelian parameter group. The general basis and cell-module results are proved locally. The modular layer proves the general finite-Weyl canonical-basic-set theorem under its exact Lusztig and L-good hypotheses, with the A1×A1 identity-decomposition case retained as a worked example.

Companion: unequal-parameter-hecke-cells-and-representations-examples.

Reading context

The declared page-level reading route is hopf-hecke-and-quantum-symmetry-interfaces. It provides adjacent context; no item from that page is a logical supplier for the claims below.

Published Coxeter and Hecke suppliers remain canonical at their current homes, including Matsumoto's theorem: braid connectivity of reduced expressions, with singleton detection in dihedral subgroups, Support, intrinsic parabolic presentations, minimal coset representatives and length additivity, with the type-A identification, The standard basis of the generic Hecke algebra and base change, and The subword characterization of Bruhat order and its independence of the reduced expression. The local arbitrary-rank parabolic result reduces each claim to finite generator support before using those results.

Parameters and the standard basis

Let (W,S) be a Coxeter system, with length ℓ, and let Γ be a totally ordered abelian group, written additively. Its group algebra is A=Z[Γ], with basis symbols vγ, involution vγ‾=v−γ, and negative part A<0 spanned by vγ for γ<0.

A weight function L:W→Γ satisfies L(xy)=L(x)+L(y) whenever ℓ(xy)=ℓ(x)+ℓ(y). Its simple-generator labels must agree across every finite odd-labelled edge; even-labelled edges allow independent values. The weighted Hecke algebra uses

(Ts−vL(s))(Ts+v−L(s))=0

and the Coxeter braid relations. The arbitrary-rank standard-basis proof uses finite support to extend the finite-generator basis theorem and proves the bar involution and its strict Bruhat triangularity.

The local theorem Existence and uniqueness of the ordered-group unequal-parameter Kazhdan–Lusztig basis constructs the unique bar-invariant basis Cw=Tw+∑y<wpy,wTy with py,w∈A<0. It covers positive, zero, and negative values of L(s); the simple-generator normalization is stated separately in that theorem.

Cells and quotient modules

The preorders are generated by nonzero coefficients in CsCy and CyCs; the two-sided preorder uses either kind of step. Mutual comparability gives the left, right, and two-sided cells. For each cell, the lower span modulo the lower span outside that cell is a module on the appropriate side. Weighted cell quotients are well-defined modules and bimodules proves ideal closure and shows that the quotient basis is indexed exactly by the cell.

These constructions do not establish Lusztig's P1–P15, positivity, boundedness, semisimplicity, or a classification of irreducible modules. The exact boundedness convention and the conjectural status of P1–P15 in the general setting are recorded in Lusztig P1–P15 are not universally proved cell properties.

Finite-Weyl cells and modular basic sets

For A=Z[v,v−1], finite Weyl W, and a nonnegative integral weight, Finite-Weyl Lusztig data and the precise basic-set hypotheses states the split generic setup and precisely P2–P8 and P15′. These properties are explicit hypotheses. The theorem does not assert them for arbitrary unequal weights.

Finite-Weyl canonical basic sets from Lusztig properties applies to every θ:A→k with parameter u=θ(v)≠0, multiplicative parameter ξ=u2, and characteristic zero or L-good characteristic. Here L-good means that all leading Schur integers fE are nonzero in k, with cE(v)=fEv−2αE plus higher powers. The full Schur elements are allowed to vanish: the result includes nonsemisimple specializations.

The local proof constructs the asymptotic algebra J, its integral map ϕ:H→JA, and its compatible filtered layers. Explicit integral matrix units give the good-characteristic split J-models. The generic Hecke models are free globally over A, obtained by restricting those integral models through ϕ. Lifted projective-cover idempotents compare their generic ranks and special dimensions. Thus the proof does not infer freeness of arbitrary torsion-free modules over a two-dimensional local ring or assume exactness of arbitrary lattice reduction.

The result selects a unique generic label E(M) for every special simple, with multiplicity one and least Schur exponent; all other contributing labels have strictly larger exponent. Weighted cell quotients and the leading finite-Weyl basic-set labels proves its cell connection, explicitly retaining the dagger twist between the asymptotic and native cell conventions. It asserts neither that all cell modules are irreducible nor that all cell labels remain distinct.

The scope and proof status of the finite-Weyl basic-set theorem distinguishes the proved conditional implication, its complete local suppliers, and Geck's dated source-status report of known parameter regimes. It does not use unproved universal P1–P15 claims as logical premises.

The A1×A1 worked specialization

For W=A1×A1, L(s)=1,L(t)=2, and the specialization O=Zp, v↦1+p for an odd prime p, The four weighted cells of A1×A1 give a canonical basic set at odd residue characteristic computes all four singleton cells and their one-dimensional quotients. The specialized order is O4, the decomposition matrix is the identity, and the four cell modules form a canonical basic set under the stated definition.

This example lies in Geck's finite-Weyl setting. In his normalization Us=vL(s)Ts, the rank-one Schur elements are 1+v±2L(s); for A1×A1 their products specialize to 4, which is nonzero at odd residue characteristic. This verifies the nonvanishing hypothesis of Geck's Theorem 4.11. The worked theorem computes these lattice reductions directly. The separate general theorem above supplies the broader finite-Weyl modular connection under its explicit hypotheses.

The Schur-element convention used in that comparison is defined in Schur elements of a split semisimple algebra with a symmetrizing trace from the normalized character expansion of the canonical trace.

Sources and placement

The original batch-70 coverage is preserved as native history. The focused completion's full-source readings, local proof route and consumer dispositions are recorded in research/non-ml-math-remaining-81-2026-10-18-owner-unequal-basic-set-completion/. The main treatments are Lusztig's Hecke Algebras with Unequal Parameters (especially §§3–5 and 8), Geck's Modular Representations of Hecke Algebras (complete relevant §§4–6), and Björner–Brenti's Combinatorics of Coxeter Groups (Chapters 1–2).

The page and its companion stay within the planned PA-39 scope. Existing published items retain their canonical identities and placements; no type-A cell classification is promoted to an unequal-parameter theorem.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order

Definition

Let S be any set, possibly infinite, and let m:S×S→{1,2,3,…}∪{∞} be a Coxeter matrix: m(s,s)=1, and for distinct s,t, m(s,t)=m(t,s)∈{2,3,…}∪{∞}. Let F(S) be the free group on S, let N be the normal closure of

{s2:s∈S}∪{(st)m(s,t):s≠t, m(s,t)<∞},

and define W=F(S)/N. The image of s∈S in W is also denoted s. This is the Coxeter group presented by (S,m).

For w∈W, define its length by

ℓ(w)=min⁡{k∈N:w=s1⋯sk for some s1,…,sk∈S}.

The set is nonempty because every element of the quotient has a finite word in S∪S−1 and the relators give s−1=s; its minimum exists by the well-ordering principle. A word of length ℓ(w) for w is a reduced expression; the empty word is the reduced expression of 1.

Define the reflection set T={xsx−1:x∈W, s∈S}. Write u→v if v=ut for a reflection t∈T and ℓ(v)>ℓ(u). Define the reflection-chain Bruhat order by u≤v if there is a finite chain u=u0→u1→⋯→uk=v; the empty chain is allowed. Length strictly increases on each nonempty chain, so this relation is a partial order. The exact reduced-subword description and finite-interval consequence needed below are established in Finite-generator standard parabolics and the Bruhat subword property at arbitrary rank ↗.

When S is finite, the presentation and length agree with Coxeter matrices, the presented Coxeter group, reduced words, length, and standard parabolic subgroups, and the reflection-chain order agrees with The Bruhat graph by length-increasing reflection chains, the Bruhat order, inversion symmetry, and reflection parity. No exchange, standard-parabolic, reduced-subword, or interval-finiteness property is included in this definition; those properties are justified separately.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Canonical basic sets for split Hecke specializations

Definition

Let O be a Noetherian commutative local domain, with fraction field K, maximal ideal m and residue field k0=O/m. Allow a specified field extension k/k0 as the specialization field. The nonfield DVR case is included: a nonfield discrete valuation ring is equivalently a local PID with nonzero maximal ideal (Equivalent characterizations of a DVR); the original residue-field specialization is k=k0. Let HO be a finite free O-algebra, so it has finite rank as an O-module. Assume the generic algebra HK=K⊗OHO is split semisimple, meaning a finite product of full matrix algebras over K; assume Hk=k⊗OHO is split, meaning each simple module remains simple after extending the field. A simple module is a nonzero module with no proper nonzero submodule. Write Irr⁡(HK) and Irr⁡(Hk) for their isomorphism classes of simple modules. For each E∈Irr⁡(HK), choose an HO-stable O-lattice ΛE⊂E, meaning a finite free O-submodule spanning E over K. Assume each simple M∈Irr⁡(Hk) occurs in at least one reduction k⊗k0(ΛE/mΛE), so every column below is nonzero. For such M, let

dE,M=[k⊗k0(ΛE/mΛE):M]

be the multiplicity of M among the composition factors of this finite-dimensional Hk-module. A composition series is a finite strict submodule chain with simple successive quotients; one exists by induction on module dimension, and Jordan–Hölder makes its multiplicities independent of the chosen series (Composition series and composition factors of an object, Jordan-Holder theorem in an abelian category). The matrix D=(dE,M) is the decomposition matrix for these chosen lattices. This definition makes no choice-independence assertion for arbitrary local orders. The finite-Weyl theorem below supplies free integral models and proves their multiplicities independent in its complete local setting; the rank-one worked specialization gives its lattices directly.

Fix an integer-valued statistic αE on Irr⁡(HK). In Geck's finite-Weyl Hecke convention this is the Schur-element exponent denoted αE; its particular values do not enter the identity-matrix case. Put

αˇM=min⁡{αE:dE,M>0}.

A subset B⊆Irr⁡(HK) is a canonical basic set (relative to D and α) if there is a bijection M↦E(M) from Irr⁡(Hk) to B satisfying

dE(M),M=1,αE(M)=αˇM,

and, for every E,M,

dE,M>0⟹αˇM<αE or E=E(M).

This is a definition only; it makes no claim that such a subset exists in every specialization.

DefinitionDefinition: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Schur elements of a split semisimple algebra with a symmetrizing trace

Definition

Let K be a field and H a finite-dimensional split semisimple K-algebra, meaning H≅∏i=1nMdi(K) for positive integers di. Let τ:H→K be a symmetrizing trace: τ(ab)=τ(ba), and the bilinear form (a,b)↦τ(ab) is nondegenerate. For each simple H-module E, let χE(h)=Tr⁡K(h∣E) be its character. If the trace has an expansion

τ=∑E∈Irr⁡(H)cE−1χE

with all cE∈K×, the scalars cE are the Schur elements of the pair (H,τ). The definition makes no existence claim for an arbitrary functional; existence and values require a separate proof in the specified regime. The rank-one specialization computes them directly, while the finite-Weyl asymptotic theorem proves the full trace expansion and its leading coefficients.

For the canonical finite Coxeter Hecke trace and its symmetric perfect pairing, see The canonical Hecke trace and symmetrizing form and The canonical Hecke trace is symmetric and perfect.

RemarkRemark: Literature-sourcedProof: Not applicablejudge pass (gpt-6-luna)Open item page →

Lusztig P1–P15 are not universally proved cell properties

Scope note

In Lusztig's §13.1, preserving the setup of §3.1, one assumes L(s)>0 for every s∈S. The coefficient fx,y,z is defined by the standard-basis product TxTy=∑zfx,y,zTz; fx,y,z′ is defined by the same product in the c-basis, and hx,y,z by cxcy=∑zhx,y,zcz. Thus the f-coefficients do not belong to an auxiliary t-basis. Section 13.2 calls (W,L) bounded when there exists N∈N such that v−Nfx,y,z∈A≤0 for all x,y,z∈W. Section 14.1 retains the positive-weight assumption and assumes boundedness; §14.2 labels P1–P15 as conjectures in that setup. Lusztig verifies them in specified cases in later sections, but the general list is not a universally established theorem.

Geck separately notes in Remark 5.9 of his Modular Representations of Hecke Algebras that the arguments of his §5 (including the result he attributes there to Lusztig §5.2) also go through for L:W→N with some L(s)=0, provided Δ(z) is set to ∞ when the trace coefficient τ(cz) vanishes. This is a qualification for those §5 arguments, not a removal of the positive-weight hypothesis from Lusztig's §§13–14.

The general basis and quotient constructions establish the weighted bar-invariant basis and the ideal and quotient-module construction for all stated Coxeter systems. Those constructions prove none of P1–P15, no positivity theorem, no semisimplicity theorem, and no classification of irreducible representations. A separate finite-Weyl theorem on this page proves modular canonical-basic-set triangularity under the explicitly stated P2–P8 and P15′ hypotheses and good-characteristic condition; it does not prove those hypotheses universally. Any stronger cell property must be stated with its exact type, parameter, boundedness, and proof hypotheses.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passjudge pass (gpt-6-luna)Open item page →

Complete local modular systems and integral idempotent lifting

Statement

Assume the Axiom of Choice. Let A=Z[v,v−1] and let θ:A→k be a unital homomorphism to a field. Set p=ker⁡θ, k0=Frac⁡(A/p)⊆k, and let R be the maximal-adic completion of Ap. Then R is a complete separated Noetherian local domain with residue field k0, and A→R is injective. Thus Q(v) embeds in F=Frac⁡R, and A→R→k0→k equals θ.

Every finite projective R-module is free, with equal fraction-field and residue-field dimensions. In every finite associative unital R-algebra C, every idempotent of C/mRC lifts to an idempotent of C. For any right C-module, multiplication by such an idempotent is an exact projection commuting with scalar extension. In particular, a filtration with finite free layers remains exact on its projected layers after passing to F or k0. If JR=⨁EMdE(R), every R-finite-free JR-module has the same simple multiplicities in its generic and residue fibres.

Facts & Assumptions

Given: The homomorphism θ and the stated rings and modules. The Axiom of Choice is retained from the commutative-algebra suppliers.

[F1]

The Laurent ring Z[v,v−1] is a Noetherian domain; quotients and localizations of Noetherian rings are Noetherian, and a one-variable polynomial ring over a field is a PID (The Laurent polynomial ring is Noetherian and a unique factorisation domain, Every quotient and every localisation of a Noetherian ring is Noetherian, For every field F, F[x] is a principal ideal domain).

[F2]

A prime minimal over an n-generated ideal in a Noetherian ring has height at most n (Krull's height theorem).

[F3]

The completion of a Noetherian local ring is Noetherian local, complete and separated, with the same residue field, and the completion map is faithfully flat (Completion of a Noetherian local ring is local with the same residue field). Completion preserves regularity, and a regular local ring is a domain (completion preserves regular local rings, regular local rings are domains and cohen macaulay).

[F4]

A finite module M over a local ring with mM=M is zero (Assuming the Axiom of Choice, Nakayama's lemma). Every finite module over a complete Noetherian ring is complete for its maximal-adic topology (Finite modules over complete Noetherian rings are complete).

Proof

1.1F1givenalgebra

Put B=Ap. It is a nonzero Noetherian local domain by [F1]. Its residue is Frac⁡(A/p): modulo p, the inverted elements are exactly the nonzero elements of A/p. This identifies that field with k0⊆k. Localizing a domain is injective. The elementary prime correspondence used below follows directly from fractions: a prime disjoint from the denominators extends to a prime, and contraction recovers it because a fraction belongs to the extended ideal exactly when its numerator does.

2.1F1F2step 1.1algebra

If p∩Z=0, every nonzero integer is a unit in B, so fraction arithmetic identifies B with a prime localization of Q[v,v−1]. The latter is a PID: ideals in its localization are generated by the image of a generator of their contracted ideal in Q[v]. Thus B is a field or has a nonzero principal maximal ideal (a). In the second case [F2] and the chain (0)⊊(a) give dimension one. The class of a modulo (a)2 is nonzero, since a=a2b in the domain would imply 1=ab with a a nonunit. Hence its embedding dimension is one. In the field case both dimensions are zero. Thus B is regular in both cases.

3.1F1F2step 1.1step 2.1choosealgebra

Otherwise p∩Z=(ℓ) for a prime integer ℓ. The prime p/(ℓ) in the PID Fℓ[v,v−1] is zero or (f) for an irreducible Laurent polynomial f. If it is zero, p=(ℓ) and the principal-maximal-ideal argument of step 2.1 proves regularity. Otherwise choose a Laurent lift G of f; then the maximal ideal of B is m=(ℓ,G). The chain (0)⊊(ℓ)B⊊m and [F2] give dim⁡B=2. The quotient B/(ℓ) is the domain Fℓ[v,v−1](f). If ℓ=rℓ2+sℓG+tG2 in B, reduction modulo ℓ gives tˉf2=0, hence t=ℓt′. Cancellation of ℓ then gives 1=rℓ+sG+t′G2∈m, impossible. Thus ℓ∉m2. If aℓ+bG∈m2, reducing modulo ℓ gives bˉf∈(f2), so b∈m. It follows that aℓ∈m2, and ℓ∉m2 forces a∈m, since otherwise a is a unit. The two displayed generators therefore give a basis of m/m2; its dimension is two. Thus B is regular in this final case.

4.1F3step 1.1step 2.1step 3.1algebra

By [F3], R=B^ is complete separated Noetherian local with residue k0, is regular, and is a domain. Faithful flatness makes B→R injective: if b maps to zero, flat tensoring the inclusion bB↪B gives an injection bB⊗BR↪R whose image is zero; faithfulness forces bB=0, so b=0. Therefore A↪R induces Q(v)↪F, with the required residue map. If p=0, this also covers the field B=R=Q(v) with zero maximal ideal.

5.1F4step 4.1choosealgebra

For a finite projective module P over any local ring, lift a basis of P/mP to r elements of P. Nakayama on the finite cokernel makes Rr→P surjective. Projectivity splits it as Rr=P⊕Q, with Q finite. Reduction of this direct sum shows Q/mQ=0, so Nakayama gives Q=0. Hence P is free of rank r. Over our domain this rank equals both dim⁡F(F⊗RP) and dim⁡k0(k0⊗RP).

5.2F4step 4.1constructalgebra

Let x0∈C lift an idempotent modulo mRC. Define δi=xi2−xi and xi+1=xi+(1−2xi)δi. All factors here are polynomials in xi, so integer-polynomial expansion gives δi+1=δi2(4δi−3). Thus δi∈mR2iC and xi+1−xi∈mR2iC. The finite-module completeness in [F4] gives a limit q≡x0 modulo mRC. Multiplication is continuous, since these ideal powers are two-sided ideals, so separatedness gives q2=q. This construction involves no division and works in every characteristic.

6.1step 5.1step 5.2algebra

For any right C-module X, the R-linear decomposition X=Xq⊕X(1−q) shows that projection X↦Xq commutes with every scalar extension. It is exact: under a surjection X→Y, lift y∈Y to x, and then xq lifts yq; kernels and injections follow by restriction of the same projection. If 0→Ii+1→Ii→Bi→0 is a filtration sequence, projection gives 0→Ii+1q→Iiq→Biq→0. When Bi is finite free, Biq is finite projective and hence free by step 5.1; the sequence splits as R-modules. It therefore retains its exact layer after scalar extension, including reduction to k0.

7.1step 5.1step 6.1algebra∎

Finally let JR=⨁EMdE(R) act on an R-finite-free module X. With matrix units eijE, put QE=e11EX. It is a direct summand of X, hence finite free by step 5.1. The map RdE⊗RQE→eEX sending ui⊗x to ei1Ex has inverse y↦∑iui⊗e1iEy, by the matrix-unit identities. Therefore the generic and residue multiplicities of the E-standard simple are both rank⁡RQE. This proves the final assertion and completes the lemma.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Weight functions and ordered group-algebra coefficients

Definition

Let (W,S) be as in Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order. A totally ordered abelian group (Γ,+,0,<) is an abelian group with a total order invariant under translation. Its group algebra A=Z[Γ] consists of finite sums ∑γ∈Γaγvγ, where aγ∈Z, with vγvδ=vγ+δ. Define the ring involution vγ‾=v−γ, and set

A<0=⨁γ<0Zvγ,A≤0=⨁γ≤0Zvγ.

A weight function is a map L:W→Γ such that L(xy)=L(x)+L(y) whenever ℓ(xy)=ℓ(x)+ℓ(y). Its simple-generator parameters are L(s) for s∈S. The exact criterion for prescribing those values on the simple generators is proved in Simple-generator weights extend uniquely to a weight function ↗. No sign restriction on L(s) is part of this definition.

The coefficient ordering used on the weighted Kazhdan–Lusztig basis is the given order on Γ, through A<0. The group algebra elements vL(s) are units for every s∈S.

TheoremStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Finite-generator standard parabolics and the Bruhat subword property at arbitrary rank

Statement

Let S be any set with Coxeter matrix m, and let W,ℓ,T,≤ be as in Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order. For a finite J⊆S, let WJ∗ be the group presented by the restricted matrix m∣J, and let ϕJ:WJ∗→W send each generator to the same-named element.

  1. The map ϕJ is injective with image ⟨J⟩, and intrinsic length in WJ∗ equals ambient length in W on this subgroup.
  2. For y,w∈W, y≤w if and only if a reduced expression of y occurs as a subword of any fixed reduced expression of w. In particular, the interval {y:y≤w} is finite and has at most 2ℓ(w) elements.
  3. For every s∈S and w∈W, ℓ(sw)=ℓ(w)±1 and ℓ(ws)=ℓ(w)±1.

Facts & Assumptions

Given: The arbitrary-rank Coxeter presentation, its length and reflection-chain order, a finite subset J⊆S, and a finite set of generators K⊆S containing the supports used in a given argument.

[F1]

Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order: W is the quotient of the free group on S by the normal closure of the involution and finite braid relators; elements and relators have finite word support; ℓ is minimum word length; and y≤w means there is a finite chain of length-increasing right multiplications by reflections.

[F2]

Support, intrinsic parabolic presentations, minimal coset representatives and length additivity, with the type-A identification: for a finite Coxeter matrix on K and J⊆K, the canonical presentation map from the Coxeter group on J into the group on K is injective, and intrinsic J-length equals ambient K-length on that subgroup.

[F3]

Length parity, exchange, two-letter deletion, and faithfulness of the signed reflection action: in a finite-generator Coxeter system, left and right multiplication by a simple generator change length by exactly 1 in absolute value.

[F4]

The Bruhat graph by length-increasing reflection chains, the Bruhat order, inversion symmetry, and reflection parity: Bruhat comparison is the transitive closure of length-increasing right multiplication by reflections.

[F5]

The subword characterization of Bruhat order and its independence of the reduced expression: in a finite-generator Coxeter system, y≤w if and only if a reduced expression of y is a subword of any fixed reduced expression of w.

[F6]

Free group on a set of generators: every map from the generators of a free group to a group extends uniquely to a homomorphism.

[F7]

The normal closure of a subset of a group: the normal closure of a set is the intersection of all normal subgroups containing it.

Proof

Given: The data in the Statement.

1.1F1F2F6F7construct

Finite-generator parabolic embedding. The image of ϕJ is ⟨J⟩, since its image is generated by the named generators. To prove injectivity, let g∈WJ∗ map to 1, and represent g by a word u in J. In the free group F(S), the word u lies in the normal closure N of the Coxeter relators by [F1]. By [F7], N is the subgroup generated by all conjugates of those relators and their inverses: that subgroup is normal and contains the relators, and every normal subgroup containing the relators contains it. Therefore u is a finite product of conjugates of relators and their inverses. Let K contain J and every letter appearing in these finitely many conjugating words and relators. The inclusion F(K)→F(S) has a retraction sending generators outside K to 1, so it is injective by the free-group universal property [F6]. Thus the same finite product identity holds in F(K), and u is the identity in the Coxeter group presented on K. Applying [F2] to the finite system on K and its subset J shows that the map from WJ∗ into this group is injective. Hence g=1.

2.1F1F2step 1.1

Intrinsic and ambient lengths. Every J-word is an S-word, so ambient length is at most intrinsic J-length. Conversely, take w∈WJ∗ and a reduced ambient expression for ϕJ(w), of length r. Let K contain J and the letters in that expression. By step 1.1 applied to K, the presentation on K embeds in W; thus the equality between a J-word for w and the chosen ambient word already holds in the group on K. By [F2], intrinsic J-length equals K-length on WJ∗. The chosen expression gives K-length at most r, while every K-word is also an S-word and so has length at least r. Hence both lengths equal r, proving intrinsic and ambient length equality.

3.1F1F3step 1.1step 2.1

Simple-generator length changes. Fix s∈S and w∈W. Choose a finite K containing s and the letters of a word for w. Steps 1.1 and 2.1 embed the group on K and preserve lengths. Applying [F3] in that finite-generator system gives both asserted ±1 formulas in W.

3.2F1F2F4F5step 1.1step 2.1

Bruhat comparison implies a subword. Suppose y≤w, and fix a reduced expression of w. Choose a finite Bruhat chain from y to w. Each element in this chain has finite word support, and each reflection used in an edge is a conjugate of a simple generator by a finite word. The union of these supports and the letters of the fixed expression of w is contained in a finite K⊆S. By steps 1.1 and 2.1, the chain lies in the embedded finite-generator group on K with all lengths preserved; its edges are still right multiplications by reflections. The finite-generator subword theorem [F5] now gives a reduced expression of y as a subword of the fixed expression of w.

3.3F1F4F5step 1.1step 2.1

A reduced subword implies Bruhat comparison. Suppose a reduced expression of y occurs as a subword of a fixed reduced expression of w. Let J be the finite support of that expression of w. The subword theorem [F5] gives y≤w in the finite-generator Coxeter group on J. By steps 1.1 and 2.1 its presentation embeds in W and preserves lengths; each reflection in the finite Bruhat chain maps to a reflection in W. The chain therefore gives y≤w in the global reflection-chain order.

4.1F1step 3.1step 3.2step 3.3∎

Every element below w is represented by a subword of a fixed reduced expression of w, by step 3.2. There are at most 2ℓ(w) such subwords, so the lower interval is finite with the stated bound. A strict comparison has a nonempty length-increasing chain by [F1], hence ℓ(y)<ℓ(w) when y<w. Steps 3.1–3.3 prove all remaining clauses. All supports, products in the normal closure, and chains used above are finite.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Simple-generator weights extend uniquely to a weight function

Statement

Let S be any set with Coxeter matrix m, let (W,S) be the presented system of Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order, and let Γ be the ordered abelian group of Weight functions and ordered group-algebra coefficients. Every weight function L:W→Γ has L(s)=L(t) whenever s≠t, m(s,t)<∞, and m(s,t) is odd. Conversely, every label map λ:S→Γ satisfying these odd-edge equalities extends uniquely to a weight function with L(s)=λ(s).

Facts & Assumptions

Given: The arbitrary-rank Coxeter presentation, its length, an ordered abelian group Γ, and simple-generator labels.

[F1]

Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order: reduced expressions are finite words in S, and word length is the minimum length representing the element.

[F2]

Finite-generator standard parabolics and the Bruhat subword property at arbitrary rank: every finite set of simple generators gives an embedded standard parabolic, with the same intrinsic and ambient lengths.

[F3]

Matsumoto's theorem: braid connectivity of reduced expressions, with singleton detection in dihedral subgroups: for a finite Coxeter matrix, any two reduced expressions of one element are connected by finitely many braid moves; a move exchanges two alternating words of the same finite braid length.

[F4]

Weight functions and ordered group-algebra coefficients: a weight function is a map L additive on products whose lengths add.

[F5]

The rank-two block computation, exact dihedral orders, the signed reflection action, and ambient reducedness: for distinct generators with finite label m=m(s,t), every alternating word of length q≤m is reduced in the ambient Coxeter group.

Proof

Given: The data in the Statement.

1.1F1F2F3construct

For w∈W, take a reduced expression w=s1⋯sk and set L(w)=∑i=1kλ(si). This does not depend on the reduced expression: two reduced expressions have finite combined support J⊆S, and by [F2] are reduced expressions in the finite Coxeter system on J. By [F3] they are connected by braid moves. An even braid length uses each of its two letters equally often; an odd braid length uses one letter once more on one side and the other letter once more on the other, and those labels are equal by hypothesis. Thus each move preserves the sum, so L(w) is well defined.

2.1F1F4step 1.1algebra

If ℓ(xy)=ℓ(x)+ℓ(y), concatenating reduced expressions for x and y gives a reduced expression for xy. The sum defining L therefore gives L(xy)=L(x)+L(y). Any weight function with the prescribed simple labels must assign this same sum to every reduced expression (each prefix is reduced), proving both the weight-function property and uniqueness of the extension.

3.1F1F2F4F5algebra∎

Let s≠t have finite odd label m(s,t)=2k+1, and put J={s,t}. By [F2], the restricted two-generator Coxeter presentation embeds as WJ with intrinsic length equal to the ambient length. The two alternating words (st)ks and t(st)k have length m(s,t) and are reduced in the finite-rank Coxeter system on J by [F5], hence are reduced in W; they represent the same element by the braid relation. For any weight function L, additivity along the prefixes of each reduced word gives (k+1)L(s)+kL(t)=kL(s)+(k+1)L(t). Cancelling the common terms yields L(s)=L(t). This proves the necessary odd-edge condition.

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The unequal-parameter Coxeter Hecke algebra

Definition

Let (W,S), Γ, A=Z[Γ], and L:W→Γ be as in Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order and Weight functions and ordered group-algebra coefficients. For s∈S, write qs=vL(s)∈A×. Let F=A⟨Ts:s∈S⟩ be the free associative A-algebra and let I be the two-sided ideal generated by

(Ts−qs)(Ts+qs−1)(s∈S)

and, for each distinct s,t∈S with finite m(s,t), the equality of the two alternating products of Ts,Tt having m(s,t) factors. Define the unequal-parameter Coxeter Hecke algebra by HA(W,L)=F/I, and use Ts for the image of a generator. For m(s,t)=∞ there is no braid relation between Ts and Tt.

The quadratic relation is equivalently

Ts2=(qs−qs−1)Ts+1,

so each Ts is invertible with Ts−1=Ts−(qs−qs−1). The basis, bar, and Bruhat support properties are not part of this definition; they are proved in The arbitrary-rank weighted Hecke basis and Bruhat-triangular bar ↗.

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The arbitrary-rank weighted Hecke basis and Bruhat-triangular bar

Statement

Let S be any set with Coxeter group W, let L:W→Γ be a weight function as in Weight functions and ordered group-algebra coefficients, and let HA(W,L) be as in The unequal-parameter Coxeter Hecke algebra. Then:

  1. For each w, the product Tw along a reduced expression is independent of the chosen expression, and {Tw:w∈W} is an A-basis of HA(W,L).
  2. The assignments vγ‾=v−γ and Ts‾=Ts−1 extend to an involutive semilinear algebra automorphism of HA(W,L).
  3. For every reduced expression of w, the expansion of Tw‾−Tw in the standard basis is supported on Ty with y<w in Bruhat order.

Facts & Assumptions

Given: An arbitrary-rank Coxeter system, a weight function L, the group algebra A, and the Hecke presentation HA(W,L).

[F1]

Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order: every word uses finitely many generators; the group has the Coxeter presentation; and Bruhat order is the reflection-chain order.

[F2]

Weight functions and ordered group-algebra coefficients and Simple-generator weights extend uniquely to a weight function: A=Z[Γ], vγ‾=v−γ, L is additive on length-additive products, and its simple-generator values are equal along every finite odd-labelled edge.

[F3]

The unequal-parameter Coxeter Hecke algebra: HA(W,L) is generated by Ts with (Ts−vL(s))(Ts+v−L(s))=0 and the finite Coxeter braid relations; the quadratic relation gives Ts−1=Ts−(vL(s)−v−L(s)).

[F4]

Finite-generator standard parabolics and the Bruhat subword property at arbitrary rank: every finite set of simple generators gives an embedded finite-generator Coxeter presentation with the same intrinsic and ambient lengths, and Bruhat comparisons in it are reduced-subword comparisons.

[F5]

The standard basis of the generic Hecke algebra and base change: for a finite Coxeter generator set and parameters constant on odd-edge components, the generic Hecke algebra has standard basis {Tw}; that basis survives arbitrary commutative coefficient-ring base change without a flatness assumption.

[F6]

The subword characterization of Bruhat order and its independence of the reduced expression: in a finite-generator Coxeter system, for a fixed reduced expression w=s1⋯sk, one has y≤w exactly when y is the product of some subsequence si1⋯sir, whether or not that subsequence is reduced.

Proof

Given: The data in the Statement.

1.1F2F4F5construct

Finite-support spanning. Fix a finite J⊆S. Its odd-edge components have a universal Laurent coefficient ring with one unit parameter for each component. By [F2], sending that parameter to vL(s)∈A× is independent of s in the component, so it defines a coefficient-ring homomorphism. By [F4] and [F5], the finite Hecke algebra on J, after this base change, has basis {Tu:u∈WJ}. Every word representing an element of the global presented algebra uses some finite J, so applying this finite spanning statement to that word shows that the global elements Tw span HA(W,L).

1.2F2F3algebra

The bar automorphism. The quadratic relation in [F3] gives Ts−1=Ts−(qs−qs−1), where qs=vL(s). Define a semilinear multiplicative map on the free algebra by vγ↦v−γ and Ts↦Ts−1. The image of a quadratic relator is (Ts−1−qs−1)(Ts−1+qs), which is zero because multiplying Ts2−(qs−qs−1)Ts−1=0 by Ts−2 gives that same identity. The image of a braid relation is the inverse of the reversed alternating relation; reversal of either alternating word is one of the two defining alternating words, so the relation is preserved. The map descends to HA(W,L). Its square fixes every coefficient and every Ts, hence is the identity.

2.1F1F3F5step 1.1algebra

Independence by finite support. Suppose a finite sum ∑w∈FawTw is zero in HA(W,L). In the free associative presentation, a representative belongs to the two-sided ideal generated by the quadratic and braid relations. Such membership is a finite sum of products of generators and relations, so only finitely many simple generators occur in that expression and in the reduced words for w∈F. Put them in a finite set J. The same relation then holds in the finite Hecke presentation on J, where [F5] gives independence of its standard basis. Thus every aw=0. Together with step 1.1 this proves that {Tw} is an A-basis and that the reduced product Tw is independent of the chosen expression.

3.1F1F3F4step 2.1algebra

Multiplication by a simple generator. By [F4], exactly one of ℓ(sx)=ℓ(x)+1 and ℓ(sx)=ℓ(x)−1 holds. In the first case, a reduced word for x prefixed by s is reduced, so TsTx=Tsx. In the second, x=s(sx) is reduced and the quadratic relation gives TsTx=Tsx+(qs−qs−1)Tx. Thus, when a simple letter is prepended to a standard-basis term, each output label is either the value with that letter prepended or the value with that letter omitted.

4.1F4F6step 3.1algebra

Bruhat support. Write a reduced expression w=s1⋯sk, and let J⊆S be its finite set of letters. Then Tw‾=Ts1−1⋯Tsk−1. Expanding each inverse as Tsi−(qsi−qsi−1) gives scalar multiples of products along subwords. Build each selected product from its rightmost letter toward its left; at each multiplication step 3.1 shows that its standard-basis labels are still values of subsequences of the original reduced expression, though a selected subsequence need not itself be reduced. Each such label and its subsequence lie in the finite parabolic on J. By [F4], that parabolic is embedded with lengths preserved; applying the full arbitrary-subword clause of [F6] there gives y≤w in the finite parabolic and hence in the global reflection-chain order. If the subsequence is proper, then ℓ(y) is at most its number of letters, hence at most k−1, so y≠w and y<w. The full reduced subsequence contributes only Tw with coefficient one, since each of its suffixes is reduced and its standard-basis product is Tw. Hence Tw‾−Tw is supported strictly below w.

5.1step 1.1step 2.1step 1.2step 4.1∎

Steps 1.1 and 2.1 prove the standard-basis clause, step 1.2 constructs the involution, and step 4.1 proves its strict Bruhat support. All reductions take place in finite supports, so no finite-rank hypothesis or choice axiom is used.

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Existence and uniqueness of the ordered-group unequal-parameter Kazhdan–Lusztig basis

Statement

Let S be any set with Coxeter group W, let L:W→Γ be any weight function into a totally ordered abelian group, let A=Z[Γ], and let HA(W,L) and its bar involution be as above. For each w∈W, there is a unique element Cw∈HA(W,L) such that

Cw‾=Cw,Cw=Tw+∑y<wpy,wTy,py,w∈A<0.

The family {Cw:w∈W} is an A-basis. For a simple generator s the normalization is Cs={Ts+v−L(s),L(s)>0,Ts,L(s)=0,Ts−vL(s),L(s)<0.

Facts & Assumptions

Given: An arbitrary-rank Coxeter system, a weight function L, its ordered group algebra A, the Hecke algebra HA(W,L), and its bar involution.

[F1]

Weight functions and ordered group-algebra coefficients: A=Z[Γ], the bar sends vγ to v−γ, and A<0 is the subgroup spanned by monomials vγ with γ<0.

[F2]

The arbitrary-rank weighted Hecke basis and Bruhat-triangular bar: {Tw} is an A-basis, bar is a semilinear involution, and Tw‾−Tw is supported on Ty with y<w.

[F3]

Finite-generator standard parabolics and the Bruhat subword property at arbitrary rank: every lower Bruhat interval is finite, y<w implies ℓ(y)<ℓ(w), and the Bruhat order is described by reduced subwords.

Proof

Given: The data in the Statement.

1.1F2F3induction

Fix w∈W. By [F3], its strict lower interval {y:y<w} is finite and consists only of shorter elements, so construct Cy for those y by induction on length. Their triangular expansions show that the Cy form an A-basis of V<w:=span⁡A{Ty:y<w}: the transition matrix is finite, unitriangular, and ordered by length.

2.1F2step 1.1algebra

Set Dw=Tw‾−Tw. By [F2], there are unique coefficients ay∈A with Dw=∑y<wayCy. Since bar is an involution and each Cy is bar invariant by induction, Dw‾=−Dw implies ∑y<way‾Cy=−∑y<wayCy. The basis property in step 1.1 gives ay‾=−ay for each y<w.

3.1F1step 2.1algebra

Write ay=∑γnγvγ with finite support. The equality ay‾=−ay forces n0=0 and n−γ=−nγ. Let py=∑γ<0nγvγ∈A<0; then py−py‾=ay. Define Cw=Tw+∑y<wpyCy. Applying bar and using Dw=∑ayCy gives Cw‾=Tw+∑y<w(ay+py‾)Cy=Cw. Expanding the Cy in the standard basis shows that all coefficients below Tw remain in A<0, because a sum of two negative exponents is negative. This constructs a normalized bar-invariant Cw.

4.1F1F2F3step 3.1

Suppose Cw′ is another element with the stated properties. Then h=Cw′−Cw=∑y<wbyTy is bar invariant with each by∈A<0. Choose a nonzero by with ℓ(y) maximal. In h‾, the coefficient of Ty is by‾: every other term of maximal length has a distinct leading basis vector, while all lower bar terms have strictly smaller length by [F2, F3]. Bar invariance gives by=by‾, but A<0∩A<0‾={0}, a contradiction. Hence Cw′=Cw.

4.2F2F3step 3.1algebra

The family Cw is linearly independent: in any finite relation, choose a term of maximal length; its coefficient at the corresponding Tw is unchanged by the unitriangular expansions and must vanish. It spans by induction on ℓ(w), because Tw=Cw−∑y<wpy,wTy and all terms on the right other than Cw have smaller length. Thus it is an A-basis.

5.1F1F2step 3.1∎

For a simple generator s, write Cs=Ts+p with p∈A<0. The bar formula in [F2] gives Ts‾=Ts−vL(s)+v−L(s). Bar invariance is therefore equivalent to p−p‾=v−L(s)−vL(s). Splitting into negative and positive exponents gives p=v−L(s) if L(s)>0, p=0 if L(s)=0, and p=−vL(s) if L(s)<0, proving the displayed normalization by uniqueness.

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Unequal-parameter left, right, and two-sided cells and cell quotients

Definition

Let Cw be the basis of Existence and uniqueness of the ordered-group unequal-parameter Kazhdan–Lusztig basis. For x,y∈W, write x←Ly if the coefficient of Cx in CsCy is nonzero for some s∈S. Write x≤Ly if there is a finite chain x=w0,…,wn=y with wi←Lwi+1 at every step. Define x←Ry from the coefficient of Cx in CyCs, and define ≤R by finite chains of such steps. Define x≤LRy by finite chains in which each step is either a left or a right step. The length-zero chain makes each relation reflexive, and concatenation makes each transitive. Mutual comparability defines equivalence relations; their classes are the left, right, and two-sided cells.

For a left cell C, define I≤CL=span⁡A{Cx:x≤Ly for some y∈C},I<CL=span⁡A{Cx:x≤Ly for some y∈C, x∉C}. Define I≤CR,I<CR for a right cell and I≤CLR,I<CLR for a two-sided cell in the same way, using the corresponding preorder. The associated left cell quotient, right cell quotient, and two-sided cell quotient are respectively I≤CL/I<CL, I≤CR/I<CR, and I≤CLR/I<CLR. Weighted cell quotients are well-defined modules and bimodules ↗ proves that these quotients inherit the stated module or bimodule actions and have bases indexed by their cells.

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Finite-Weyl Lusztig data and the precise basic-set hypotheses

Definition

Work in the split generic finite-Weyl setting: W is a finite Weyl group, L:W→Z≥0 is a weight function, A=Z[v,v−1], and H=HA(W,L) has the symmetric normalization (Ts−vL(s))(Ts+v−L(s))=0. Its KL basis is Cw. Write K=Q(v) and assume the generic algebra HK is split semisimple, as in the generic setup of Canonical basic sets for split Hecke specializations. This hypothesis supplies the generic labels; this item asserts no new theorem on generic rational splitting. Let τ(Tw)=δw,1 be the canonical symmetrizing trace.

The A-linear algebra involution † is Ts↦−Ts−1, and put Dw=Cw†. Define structure constants by CxCy=∑zhx,y,zCz; equivalently DxDy=∑zhx,y,zDz. Define

a(z)=min⁡{n≥0:vnhx,y,z∈Z[v] for all x,y∈W},γx,y,z=[v0](va(z)hx,y,z−1).

The integer a(z) exists since W is finite and all h are Laurent polynomials invariant under bar. Let Δ(z) be the negative of the largest exponent in τ(Cz), and nz its nonzero coefficient. If τ(Cz)=0, put Δ(z)=∞ and nz=0. Let D={z:a(z)=Δ(z)}. In particular Δ(1)=0 and n1=1; P3 below forces a(1)=0.

The following are explicit hypotheses, not assertions for every unequal weight. They are precisely the subset used in Geck section 5.2:

  • P2: if d∈D and γx,y,d≠0, then x=y−1.
  • P3: for every y there is a unique d∈D with γy−1,y,d≠0.
  • P4: hx,y,z≠0 implies a(z)≥a(x) and a(z)≥a(y).
  • P5: in P3, γy−1,y,d=nd=±1.
  • P6: every d∈D satisfies d2=1.
  • P7: γx,y,z=γy,z,x.
  • P8: γx,y,z≠0 implies a(x)=a(y)=a(z).
  • P15′: if a(w)=a(y), then

∑uhx,u,yγw,x′,u−1=∑uhx,w,uγu,x′,y−1.

All sums are finite. These hypotheses produce the asymptotic algebra and modular theorem in the following proved suppliers; they do not assume positivity or irreducibility of cell modules. The generic Schur element cE(v) is determined by τK=∑EcE(v)−1tr⁡E. We use Geck's notation αE∈N and fE∈Z>0 for the Schur exponent and leading integer in Theorem 4.4. The local leading-Schur lemma below proves, from the stated P hypotheses, that cE(v) has lowest term fEv−2αE and that αE equals the support degree of VE in J. A specialization θ:A→k has u=θ(v)∈k×, multiplicative parameter ξ=u2, and is L-good when θ(fE)≠0 for every generic label E. Characteristic zero is always L-good. The modular theorem does not require θ(cE(v))≠0.

To compare normalizations, Geck's multiplicative generator is Ss=vL(s)Ts and obeys (Ss−v2L(s))(Ss+1)=0; after specialization its parameter is ξL(s). The asymptotic formulas below use Lusztig's revised convention Dw↔tw and coefficients nd in ϕ, with no diagonal sign change. Geck's signed starred convention is not mixed into these formulas.

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Weighted cell quotients are well-defined modules and bimodules

Statement

For every Coxeter system and weight function of The unequal-parameter Coxeter Hecke algebra, the spans I≤CL and I<CL attached to a left cell are left ideals; the right-cell spans are right ideals; and the two-sided-cell spans are two-sided ideals. Therefore the quotients defined in Unequal-parameter left, right, and two-sided cells and cell quotients are left modules, right modules, or bimodules, respectively. Each quotient has an A-basis consisting exactly of the images of the KL basis elements indexed by its cell. No further cell property, semisimplicity, or irreducible-module classification is asserted.

Facts & Assumptions

Given: The weighted Hecke algebra HA(W,L), its KL basis, the coefficient preorders, and a cell C.

[F1]

Unequal-parameter left, right, and two-sided cells and cell quotients: x←Ly means Cx occurs with nonzero coefficient in CsCy for some s∈S; ≤L is its finite-chain closure; the left cell quotient is the span of all Cx with x≤LC, modulo the span with x∉C. The right and two-sided definitions use right or either kind of step.

[F2]

Existence and uniqueness of the ordered-group unequal-parameter Kazhdan–Lusztig basis: {Cw:w∈W} is an A-basis; each product CsCy and CyCs has a finite basis expansion; and Ts=Cs−ηs for a scalar ηs∈A.

Proof

Given: The data in the Statement.

1.1F1F2algebra

The left spans are left ideals. If Cx occurs in CsCy, then x←Ly, hence x≤Ly. Therefore, if y≤LC, every basis term in CsCy also has index ≤LC, proving closure of I≤CL under left multiplication by each Cs. If y<LC, each such x is also outside C: otherwise some g∈C satisfies g≤Lx≤Ly≤Lg, forcing y∈C, a contradiction. Thus I<CL is also closed under left multiplication by each Cs. Since Ts=Cs−ηs, the Cs and scalars generate HA(W,L), so both spans are left ideals.

1.2F1F2algebra

The right spans are right ideals. If Cx occurs in CyCs, then x←Ry, hence x≤Ry. Thus right multiplication by each Cs preserves the right numerator. If y is in the right denominator and x∈C, choose g∈C with y≤Rg; since g and x lie in the same cell, g≤Rx, while x≤Ry. Transitivity would make g equivalent to y, contradicting y∉C. So right multiplication also preserves the right denominator. The generators Ts=Cs−ηs then show that these spans are right ideals of HA(W,L).

2.1F1F2step 1.1step 1.2algebra

The two-sided spans are two-sided ideals. A two-sided preorder step is a left step or a right step. Applying the closure arguments of steps 1.1 and 1.2 to each type of step shows that left and right multiplication by every Cs, and hence by every Ts, preserves both I≤CLR and I<CLR. They are therefore two-sided ideals.

3.1F1F2step 1.1step 1.2step 2.1∎

Quotient bases and actions. The KL basis is an A-basis by [F2]. For the corresponding preorder, every x∈C belongs to the numerator because x≤x; every numerator index outside C belongs to the denominator by its definition. Thus the numerator basis indices are the disjoint union of the cell C and the denominator indices, so their quotient has basis exactly the images of Cw with w∈C. The induced left, right, or bimodule action is well defined because the numerator and denominator are ideals of the required sidedness, as proved in steps 1.1, 1.2, and 2.1.

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The asymptotic algebra, filtered layers and the specialization homomorphism

Statement

Assume Finite-Weyl Lusztig data and the precise basic-set hypotheses, including P2–P8 and P15′. The free abelian group J=⨁w∈WZtw is an associative algebra under txty=∑zγx,y,z−1tz, with identity ∑d∈Dndtd. It has an anti-involution ιJ(tw)=tw−1 and a perfect symmetrizing trace μ(tw)=nw for w∈D and zero otherwise, with μ(txty)=δx,y−1.

Put Ji=⟨tw:a(w)=i⟩Z and Ii=⟨Dw:a(w)≥i⟩A, and Bi=Ii/Ii+1. These are respectively mutually orthogonal two-sided ideals of J, two-sided ideals of H, and free layers on the classes [Dw] with a(w)=i. The identification [Dw]↦tw makes Bi a left JA-module and a (JA,H)-bimodule. The map

ϕ:H⟶JA,ϕ(Dx)=∑z∈W, d∈Da(z)=a(d)hx,d,zndtz

is a unital algebra homomorphism, and the natural left H action on Bi is exactly restriction along ϕ. Here the sum means z∈W,d∈D.

All these statements survive any commutative coefficient specialization. With N=max⁡wa(w), (ker⁡ϕR)N+1=0 for every specialization to a field or ring R. Over K=Q(v), ϕK is an isomorphism. The rational algebra JQ is split semisimple. Its simple modules VE can be indexed by the generic labels E so that K⊗VE, restricted through ϕK, is E. Each has a unique support degree νE such that JQνEVE=VE and the other Ji act by zero.

Facts & Assumptions

Given: The finite-Weyl split generic setup, KL/dagger bases and the exact P hypotheses.

[F1]

Finite-Weyl Lusztig data and the precise basic-set hypotheses supplies the structure constants, a, γ, D, nd, generic splitting and P2–P8/P15′.

Proof

1.1F1givenalgebra

Reversing words gives the anti-involution Tw↦Tw−1 of the Hecke presentation. It commutes with bar. Inversion preserves length and sends a reflection-chain step u→ut to u−1→tu−1=u−1(utu−1), again a length-increasing right-reflection step; hence it preserves Bruhat order. Thus it preserves Bruhat triangularity, and KL uniqueness gives Cw↦Cw−1. Hence hx,y,z=hy−1,x−1,z−1, a(z)=a(z−1), and γx,y,z=γy−1,x−1,z−1. Comparing coefficients in the bar-invariant products CxCy also gives hx,y,z‾=hx,y,z. P3 with y=1 forces a(1)=0 and 1∈D, since C1C1=C1 makes the required nonzero coefficient possible only for d=1 and exponent zero. The assignment Ts↦−Ts−1 preserves the quadratic relation and braid relations (the signs agree at equal braid length and inverse reversed braid words agree), is involutive and is A-linear. Thus DxDy has the same constants h.

2.1F1step 1.1algebra

P8 implies that products in J vanish across distinct a-degrees. For a fixed degree i, multiply P15′ by vi and take its constant coefficient. Whenever a γ term is nonzero, P8 forces every participating index to have degree i. The resulting identity is ∑uγx,u,y−1γw,x′,u−1=∑uγx,w,u−1γu,x′,y−1, exactly equality of the coefficients of ty in tx(twtx′) and (txtw)tx′. Other degree combinations vanish. This proves associativity without using any unlisted P property.

3.1F1step 1.1step 2.1algebra

The coefficient of ty in tx∑dndtd is ∑dndγx,d,y−1=∑dndγy−1,x,d by P7. P2 makes it zero unless y=x; then P3 and P5 give the unique coefficient nd2=1. The left identity is proved in the same way, using cyclic symmetry with γx,y−1,d; the appropriate unique d comes from P3 applied to x−1. Step 1.1 proves that ιJ reverses products. Since d=d−1 by P6, μ(txty)=∑dγx,y,dnd is δx,y−1 by P2, P3 and P5. This symmetric permutation Gram matrix is invertible over Z, proving every trace assertion.

4.1F1step 2.1step 3.1algebra

P4 implies that each Ii is a two-sided ideal. Its layer has exactly the stated basis since both ideals are spans of subsets of the D-basis. P8 and step 3.1 give the orthogonal ideal decomposition J=⨁iJi, with central identities 1i=∑d:a(d)=indtd. On the free layer Bi, identify [Dw] with tw for a(w)=i and give it the left regular JAi action. Natural left and right H multiplication are well defined on the layer.

5.1F1step 4.1algebra

Let Ax be natural left multiplication by Dx on Bi. The coefficient of [Dy] in AxRtx′[Dw] is ∑uhx,u,yγw,x′,u−1; the coefficient in Rtx′Ax[Dw] is ∑uhx,w,uγu,x′,y−1. Here only indices of degree i=a(w)=a(y) survive. P15′ gives equality. Thus Ax commutes with every right regular JAi multiplication and is left multiplication by its value on 1i. That value is ∑z:a(z)=i∑d:a(d)=ihx,d,zndtz, the degree-i component of the displayed ϕ(Dx). This proves compatibility of the left H action with ϕ.

6.1F1step 1.1step 4.1step 5.1algebra

Composition of natural left H actions gives Lϕ(hh′)=Lϕ(h)Lϕ(h′) on ⨁iJAi. Evaluating on its identity proves ϕ(hh′)=ϕ(h)ϕ(h′); evaluating the identity action proves ϕ(1H)=1J. For the right H action to commute with left J, apply P15′ with (x,x′,w,y) replaced by (x−1,z−1,w−1,y−1) and replace the summation variable by its inverse. Using step 1.1 gives ∑uγz,w,u−1hu,x,y=∑uhw,x,uγz,u,y−1, exactly the coefficient equality for (tz⋅[Dw])Dx=tz⋅([Dw]Dx). Thus Bi is the asserted bimodule. This argument requires no equality between ϕ and its opposite/adjoint version.

7.1F1step 5.1step 6.1algebra

The bases, identities and multiplication equalities above are finite integral coefficient identities; they remain valid after every commutative base change. If h∈ker⁡ϕR, compatibility says that hIi⊆Ii+1 for all i. A product of N+1 such elements therefore kills I0=HR and in particular its unit, proving the nilpotence bound. Over K, the algebra HK is a product of full matrix algebras by the given split generic hypothesis. A nilpotent two-sided ideal of such a product is zero: its intersection with any simple matrix factor is either zero or that factor, and a nonzero factor contains its identity and is not nilpotent. Thus ϕK is injective and, since both sides have dimension ∣W∣, is an isomorphism.

8.1F1step 4.1step 7.1constructalgebra∎

Transport matrix units of HK through ϕK. Their coordinates in the integral basis tw are rational functions of v, and their coordinate determinant is nonzero. Choose a nonzero rational value avoiding the finitely many zeros of their denominators and that determinant; such a value exists because a nonzero polynomial has finitely many roots and Q× is infinite. Evaluating the coordinates preserves the finite matrix-unit and unit identities and retains their linear independence. They therefore give an isomorphism JQ≅∏EMat⁡dE(Q). After scalar extension back to K, this decomposition has the same primitive central blocks: in the center of a split matrix product every idempotent has only zero/one coordinates. Relabel its factors accordingly. This gives rational models VE for all generic labels. Finally the central orthogonal identities 1i act on a simple module through exactly one component; denote its index by νE.

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The four weighted cells of A1×A1 give a canonical basic set at odd residue characteristic

Statement

Let W=⟨s,t∣s2=t2=1, (st)2=1⟩, the finite Weyl group A1×A1, and let L(s)=1, L(t)=2. Form its weighted Hecke algebra with coefficient v and the symmetric quadratic convention (Tr−vL(r))(Tr+v−L(r))=0. Let O=Zp for an odd prime p, let q=1+p, and specialize v↦q. Write K=Qp, k=Fp, and let D be the decomposition matrix of the four explicit O-lattices obtained from the cell quotients.

The left, right, and two-sided cells are the four singleton sets {1},{s},{t},{st}. Their four cell modules are pairwise distinct one-dimensional K-modules, and each has an O-stable rank-one lattice. Their reductions are the four distinct simple Hk-modules, so D is the 4×4 identity matrix up to the displayed ordering. Consequently, relative to any integer-valued statistic α on the generic simple modules, these four cell modules form a canonical basic set in the sense of Canonical basic sets for split Hecke specializations.

This is a finite Weyl case. In Geck's normalization, its specialization also satisfies the exact hypothesis θ(cχ)≠0 for every generic irreducible character in Theorem 4.11; the proof below verifies the decomposition matrix directly.

Facts & Assumptions

Given: The weighted Coxeter and Hecke conventions in the Statement, an odd prime p, and the definitions of the KL basis, cells, cell modules, and canonical basic set.

[F1]

Arbitrary-rank Coxeter presentations, length, reflections, and Bruhat order and Finite-generator standard parabolics and the Bruhat subword property at arbitrary rank: the Coxeter presentation determines length and Bruhat order; reduced words and subwords give the finite lower intervals needed for triangularity.

[F2]

Weight functions and ordered group-algebra coefficients and Simple-generator weights extend uniquely to a weight function: a weight function is additive on length-additive products, and simple-generator labels extend exactly when they agree along finite odd-labelled edges.

[F3]

The unequal-parameter Coxeter Hecke algebra and The arbitrary-rank weighted Hecke basis and Bruhat-triangular bar: the Hecke generators satisfy their stated quadratic and braid relations, and the standard elements form a free coefficient-module basis after specialization to a commutative coefficient ring.

[F4]

Existence and uniqueness of the ordered-group unequal-parameter Kazhdan–Lusztig basis: the elements Cw form a bar-invariant triangular basis, with Cs=Ts+v−L(s) for L(s)>0.

[F5]

Unequal-parameter left, right, and two-sided cells and cell quotients and Weighted cell quotients are well-defined modules and bimodules: coefficient transitions define the cell preorders, and the cell quotients are modules with bases given by their cell elements.

[F6]

Canonical basic sets for split Hecke specializations: for the chosen lattice decomposition matrix D, the minimum αˇM and the two multiplicity/order conditions define a canonical basic set.

[F7]

The canonical Hecke trace and symmetrizing form and The canonical Hecke trace is symmetric and perfect: for a finite Coxeter group, the coefficient of the identity standard basis element defines a trace with a symmetric perfect pairing, and this trace is preserved by commutative base change.

[F8]

Schur elements of a split semisimple algebra with a symmetrizing trace: for a split semisimple algebra with symmetrizing trace τ, the Schur elements cE, when they exist, are the nonzero scalars in τ=∑EcE−1χE.

Proof

Given: The presentation W, weights L(s)=1,L(t)=2, the specialization v↦q=1+p, and the facts above.

1.1F1F2constructalgebra

From (st)2=1 and s2=t2=1, st=(st)−1=ts. Thus every word reduces to one of 1,s,t,st. The homomorphism to (Z/2Z)2 sending s↦(1,0), t↦(0,1) respects all relators and separates these four elements, so they are distinct. Their lengths are 0,1,1,2, respectively. Since the only finite edge has even label 2, the odd-edge condition in [F2] permits the unequal labels 1,2; it gives a well-defined weight function L.

2.1F1F3F4step 1.1algebra

Put C1=1, Cs=Ts+v−1, and Ct=Tt+v−2. The rank-two relations give Ts2=(v−v−1)Ts+1 and Tt2=(v2−v−2)Tt+1, so direct expansion gives Cs2=(v+v−1)Cs and Ct2=(v2+v−2)Ct. The generators commute because m(s,t)=2, and Cst:=CsCt=CtCs=Tst+v−2Ts+v−1Tt+v−3. These elements are bar invariant and have leading standard term Tw with lower Bruhat support and negative coefficients; uniqueness in [F4] identifies them as the KL basis.

2.2F3step 1.1algebra

For r∈{s,t}, set as=q, at=q2. The specialized quadratic relation is (Tr−ar)(Tr+ar−1)=0. Since ar+ar−1≡2(modp), it is a unit in O, so er+=(Tr+ar−1)/(ar+ar−1) and er−=(ar−Tr)/(ar+ar−1) belong to HO. They sum to 1, their product is zero by the quadratic relation, and (Tr−ar)er+=(Tr+ar−1)er−=0, so they are complementary idempotents. Every rank-one element b+cTr equals (b+car)er++(b−car−1)er−, making both summands free of rank one. The commuting rank-one subalgebras tensor to HO with the standard rank-four basis [F3], so the four products esϵetδ give HO≅O4 and hence HK≅K4, Hk≅k4.

3.1F3F4step 2.1algebra

The complete left-product table is determined by CsC1=Cs, CtC1=Ct, Cs2=(v+v−1)Cs, CtCs=Cst, CsCt=Cst, Ct2=(v2+v−2)Ct, CsCst=Cs2Ct=(v+v−1)Cst, and CtCst=CsCt2=(v2+v−2)Cst. The right table is identical because the algebra is commutative. With an arrow y→x when Cx occurs in CrCy or CyCr, the only non-loop arrows are 1→s, 1→t, s→st, and t→st. No transition points back, so mutual comparability has four singleton classes for each left, right, and two-sided preorder.

4.1F3F4F5step 3.1algebra

In the quotient for {1}, both Cs and Ct vanish, so Ts=Cs−v−1 and Tt=Ct−v−2 act by −v−1 and −v−2. In the quotient for {s}, CtCs=Cst vanishes while Cs2=(v+v−1)Cs; hence (Ts,Tt) acts by (v,−v−2). In the quotient for {t}, CsCt=Cst vanishes, so Ts acts by −v−1; Ct2=(v2+v−2)Ct gives Tt-eigenvalue v2. In the quotient for {st}, CsCst=(v+v−1)Cst and CtCst=(v2+v−2)Cst, so the action is (v,v2). By [F5] each is a well-defined one-dimensional cell module. Their four eigenvalue pairs are distinct over K, since q+q−1≠0 and q2+q−2≠0 in the characteristic-zero field K.

5.1F5step 4.1step 2.2

The four cell characters from step 4.1 take values in O, so Λ=O with the displayed scalar actions is an HO-stable rank-one lattice for each. Their reductions have Ts,Tt eigenvalues respectively (−1,−1), (1,−1), (−1,1), and (1,1) in k. Since p is odd these are four distinct characters of Hk≅k4; each is simple, and each reduced lattice has composition multiplicity one for exactly its matching character. Thus D=I4, up to ordering.

6.1F7F8step 1.1step 2.2step 5.1algebra

Let K0=Q(v) be the generic coefficient field and put Ur=vL(r)Tr, which has eigenvalues Qr=v2L(r) and −1. By [F7], the canonical trace on the normalized standard basis Uw takes value 1 on the identity and 0 on nonidentity elements, and its generic pairing is symmetrizing. For one rank-one factor, the algebra over K0 is K0×K0, with characters χ+(Ur)=Qr, χ−(Ur)=−1. By [F8], write τ=c+−1χ++c−−1χ−. Evaluating at 1 and Ur gives c+−1+c−−1=1 and Qrc+−1−c−−1=0; solving yields c+=1+Qr and c−=1+Qr−1. For A1×A1, the algebra and trace are tensor products of the rank-one factors, so the four Schur elements are products of one term from {1+v2,1+v−2} and one from {1+v4,1+v−4}. Under the residue map v↦1 in k, each product is 4≠0. Thus Geck's Theorem 4.11 has its exact finite-Weyl and nonvanishing hypotheses here and gives the identity decomposition matrix; step 5.1 has already proved the same conclusion directly.

7.1F6step 5.1∎

For any integer-valued α, an identity decomposition matrix has exactly one nonzero entry in each column, equal to 1. Thus for each simple M, αˇM is the α-value of its matching cell module; all other rows in that column vanish. Both conditions in [F6] hold, so the four cell modules form a canonical basic set. The claim is restricted to this explicit finite Weyl group and this odd-characteristic specialization.

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Leading Schur coefficients and split good-characteristic asymptotic specializations

Statement

Use the data and hypotheses of Finite-Weyl Lusztig data and the precise basic-set hypotheses. For each rational simple JQ-module VE supplied by The asymptotic algebra, filtered layers and the specialization homomorphism, let χEJ be its character and νE its support degree. There are positive integers fE such that

μQ=∑EfE−1χEJ,cE(v)=fEv−2νE+strictly higher powers of v.

Consequently νE=αE, where αE is the Schur-element exponent fixed in Finite-Weyl Lusztig data and the precise basic-set hypotheses. The full Schur elements cE(v) lie in A. Each VE has a full finite free J-stable integral lattice ΛE. Put F=∏EfE and S=Z[1/F]. There is an explicit algebra isomorphism

JS ≅ ∏EEnd⁡S(S⊗ZΛE).

Consequently, for every field k of characteristic zero or characteristic not dividing any fE, the algebra Jk is split semisimple with simple modules VE,k=k⊗ΛE, preserving dimensions and support degrees. More generally the displayed matrix decomposition holds after base change to any commutative ring in which every fE is a unit. The actual Hecke model is already free globally: LE,A=A⊗ZΛE, with HA acting through the integral map ϕA and the integral J-matrices. Its generic fibre is E, and every local model used below is the base change of this displayed free module. No assertion that arbitrary torsion-free lattices over higher-dimensional local rings are free is used. No hypothesis that every specialized full Schur element θ(cE(v)) is nonzero is imposed.

Facts & Assumptions

Given: The stated finite-Weyl data, generic splitting and exact P hypotheses.

[F1]

The asymptotic algebra, filtered layers and the specialization homomorphism gives the integral algebra J, its inverse-index dual basis, positive coordinate form, rational splitting, generic isomorphism ϕK, and orthogonal support ideals.

[F2]

Finite-Weyl Lusztig data and the precise basic-set hypotheses fixes Dw=Cw†, the P conditions, generic Schur trace and coefficient conventions.

[F3]

The canonical Hecke trace is symmetric and perfect proves that the standard Hecke basis Tw has trace-dual basis Tw−1, also after weighted base change.

[F4]

Every finitely generated torsion-free module over a PID is free says a finitely generated torsion-free module over a PID is finite free.

[F5]

Schur elements of a split semisimple algebra with a symmetrizing trace defines the Schur scalars by the irreducible-character expansion of a symmetrizing trace.

[F6]

Proof

1.1F1F2F5algebra

On a split matrix algebra, a symmetric linear functional is a scalar multiple of ordinary matrix trace: commuting eii with eij forces its value on eij to be zero for i≠j, and commuting eij with eji makes all diagonal values equal. Thus on a split product it is ∑EsETr⁡E. Nondegeneracy forces every sE≠0, since otherwise an entire block is orthogonal to the algebra. Apply this to JQ from [F1], and set fE=sE−1∈Q×. The same argument gives the generic Hecke Schur scalars in [F5].

2.1F1F3step 1.1algebra

For any finite split algebra with symmetrizing trace ∑fE−1Tr⁡E and dual bases br,br∨, its inverse pairing tensor is basis-independent and equals ∑EfE∑i,jeijE⊗ejiE. Indeed both tensors represent the identity map under the trace pairing; in the matrix-unit basis the dual of eijE is fEejiE. Applying the matrix-coefficient functions gives ∑rρG(br)ijρE(br∨)ab=δG,EfEδi,bδj,a. Summing the appropriate diagonal entries gives ∑rχE(br)χE(br∨)=fEdim⁡VE. These are actual coefficient identities over Q or K, with no character-orthogonality result left as a citation.

2.2F1F4step 1.1construct

Choose a rational basis of VE and let L0 be its integer span. The sum ΛE=∑w∈WZρE(tw)L0 is finitely generated, contains L0 since 1J∈J, and is stable under every tx because the multiplication constants of J are integers. It is torsion-free of rank dE=dim⁡VE. The integers form a PID (division with remainder makes each nonzero ideal generated by its least positive member), so [F4] makes ΛE finite free. In such a basis all ρE(tw) have integer entries and χEJ(tw)∈Z.

3.1F1step 2.1step 2.2algebra

Let zE=∑wχEJ(tw−1)tw∈J. The coefficient identity in step 2.1 says that its action on VG is δE,GfEid⁡. Left multiplication by zE on the integral basis of J has an integer matrix. The Cayley–Hamilton identity therefore shows that the rational number fE is an algebraic integer; a rational root of a monic integer polynomial is an integer, by clearing its reduced denominator in that polynomial. Hence fE∈Z∖{0}.

3.2F1F2step 2.2algebra

Put a=νE. The character of E=K⊗VE satisfies χE(Dx)=∑z,d:a(z)=a(d)=ahx,d,zndχEJ(tz) by [F1]. Each vahx,d,z is in Z[v] by the definition of a(z). Taking its constant term gives ∑z,d:a(z)=a(d)=aγx,d,z−1ndχEJ(tz)=χEJ(tx), since the degree-a identity ∑d:a(d)=andtd acts as the identity on VE and all other support degrees act by zero. Thus vaχE(Dx)∈Z[v] and it is congruent to χEJ(tx) modulo vZ[v].

4.1F1step 2.1step 3.1algebra

To see positivity, use the rational positive definite form ⟨x,y⟩=μ(xιJ(y)) on JQ: [F1] makes its basis tw orthonormal. Trace symmetry implies ⟨ax,y⟩=⟨x,ιJ(a)y⟩. A rational simple left ideal UE⊂JQ exists from its matrix decomposition and is invariant under both a and ιJ(a); restriction of this positive form to UE is nondegenerate. Thus their matrices on UE are adjoints and have equal trace. It follows that χEJ(tw−1)=χEJ(tw). Step 2.1 now gives fEdE=∑wχEJ(tw)2>0. The strict inequality holds because χEJ is a nonzero linear functional on JQ, so it cannot vanish on the basis {tw}; at least one rational summand is nonzero. Therefore fE>0.

4.2F1step 2.1step 2.2step 3.1algebra

In JS set qijE=fE−1∑wρE(tw−1)jitw. Step 2.1 gives ρG(qijE)=δE,Geij. These elements lie in JS by step 2.2 and send every block to its indicated matrix unit. Hence they provide an inverse to ρ:JS→∏EEnd⁡S(S⊗ΛE): their composites are the identity after extension to Q, and both modules are torsion-free, so they are already the identity over S. This proves the displayed algebra isomorphism. Since it is defined by inverse coefficient matrices over S, it survives every commutative base change out of S, including all stated fields.

4.3F1F2step 3.2algebra

Let j be the semilinear algebra involution sending v to v−1 and Ts to −Ts. It is the product of bar with †, so Dx=j(Cx) since Cx is bar invariant. The native negative triangular expansion of Cx therefore gives Dx=(−1)ℓ(x)Tx+∑y<xry,xTy with every ry,x∈vZ[v]. Its finite unitriangular inverse gives Tx=(−1)ℓ(x)Dx+vZ[v]-linear combinations of lower Dy. Applying step 3.2 yields vaχE(Tx)≡(−1)ℓ(x)χEJ(tx)(modvZ[v]).

5.1F1step 2.2step 4.2algebra

Each central 1i acts on VE as either zero or the identity, with the identity occurring only for i=νE. These are exact integral matrix equalities on ΛE, so they remain the same after every base change in step 4.2. All special simple dimensions and support degrees are therefore the stated ones.

5.2F1step 2.2step 4.2constructalgebra

The integral matrices ρE(tw) from step 2.2 define the action of JA on the explicitly free module LE,A=A⊗ZΛE. Composing with the integral homomorphism ϕA of [F1] gives Laurent-integer Hecke action matrices. Its generic fibre is exactly the simple E by [F1]. For any coefficient ring R, set LE,R=R⊗ALE,A; it remains free with its displayed basis. When the fE are units, step 4.2 identifies this same module as the standard module of the corresponding full matrix block of JR. Thus the needed generic irreducible models are genuinely free by construction even over a two-dimensional local base.

5.3F2F3F5step 2.1step 4.1step 4.3algebra

Apply step 2.1 to the generic Hecke symmetrizing trace, using the exact dual basis of [F3]. It gives cE(v)dE=∑xχE(Tx)χE(Tx−1). Multiply by v2a and insert step 4.3. The two length signs cancel, and the constant coefficient is ∑xχEJ(tx)χEJ(tx−1)=fEdE by step 2.1. All higher coefficients have strictly positive powers of v. Dividing by the nonzero integer dE in characteristic zero gives cE(v)=fEv−2a plus strictly higher powers. Since a=νE and αE is the Schur-element exponent fixed in [F2], comparison of the lowest power gives νE=αE. This proves the exponent and leading coefficient assertions directly from the trace pairing. It also shows the Schur element is a Laurent polynomial over Q, sufficient for its lowest term; no cyclotomic factorization is assumed or needed.

6.1F2F6step 2.1step 2.2step 3.2step 4.2step 4.3step 5.3algebra∎

Step 3.2 expresses each χE(Dx) as an integral Laurent combination of the integer characters χEJ(tz); step 4.3 does the same for χE(Tx), so all these values lie in A. The element zEH=∑xχE(Tx−1)Tx therefore lies in the finite free A-algebra H. By the matrix coefficient identity in step 2.1 it acts on the generic block E as cE(v) and on all other generic blocks as zero. The Cayley–Hamilton polynomial of its integral left multiplication shows that cE(v)∈K is integral over A. By [F6], write it as a coprime fraction f/g in the UFD A. A monic equation for f/g, multiplied by its denominator, implies g∣fm; unique factorization forces g to be a unit. Thus cE(v)∈A, so its specialization is defined even when it vanishes. The good-characteristic condition used in step 4.2 concerns fE, not this full Laurent polynomial.

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Asymptotic induction identifies leading modular simples

Statement

In the finite-Weyl setting of Finite-Weyl Lusztig data and the precise basic-set hypotheses, assume its specified Lusztig properties and let θ:A→k have characteristic zero or satisfy θ(fE)≠0 for every generic simple label E. Write H=Hk, and let VE be the corresponding simple module of the split asymptotic algebra Jk, supported in degree αE. A star denotes restriction through ϕk:H→Jk.

For each simple H-module M, let aM=max⁡{a(w):DwM≠0}, where Dw=Cw†. There is an injective assignment M↦E(M) such that αE(M)=aM, M occurs once in ∗VE(M), and all its other simple factors have strictly smaller a-value. Moreover H is split: every simple H-module remains simple over every field extension.

Facts & Assumptions

Given: The stated finite-Weyl data, exact Lusztig-property hypotheses and good-characteristic specialization.

[F1]

The finite filtration Ii=⟨Dw:a(w)≥i⟩ has two-sided ideals, I0=H, IN+1=0, and layers Bi=Ii/Ii+1 carrying commuting left Jk and right H actions. The original left H action equals restriction through ϕk. The left Jk action on Bi is supported in degree i (Finite-Weyl Lusztig data and the precise basic-set hypotheses, The asymptotic algebra, filtered layers and the specialization homomorphism).

[F2]

Jk is split semisimple, with simples VE supported in degree αE (Leading Schur coefficients and split good-characteristic asymptotic specializations).

Proof

1.1F1givenconstructalgebra

Every simple H-module M is finite-dimensional, since for 0≠m∈M the map H→M, h↦hm, is surjective. Since D1=1, the maximum a=aM exists; Ia+1M=0 and IaM≠0. Set T(M)=Ba⊗HM. Its map π:T(M)→M, [f]⊗m↦fm, is well-defined: changing f by Ia+1 changes no value, and the tensor balancing relation is respected. It is H-linear by multiplication and nonzero by IaM≠0, so it is surjective.

2.1F1F2step 1.1algebra

If x=∑j[fj]⊗mj∈ker⁡π and g∈Ia, then gx=∑j[gfj]⊗mj=[g]⊗∑jfjmj=0 by tensor balancing. Thus Ia annihilates ker⁡π. Every simple factor M′ of that kernel has aM′<a, because all Dw with a(w)≥a belong to Ia. In particular [∗T(M):M]=1. Every Jk-simple factor of T(M) has degree a, by the degree support of Ba.

3.1F2step 2.1constructalgebra

Decompose the semisimple Jk-module T(M)=⨁EVEmE. Restriction preserves the direct sum. The equality [∗T(M):M]=1 implies that exactly one occurring label E has M as a factor of ∗VE, and both mE and [∗VE:M] equal one. Define this label to be E(M). Its degree is αE(M)=aM. The direct-sum inclusion of this ∗VE into ∗T(M) and step 2.1 show that all its other simple factors have strictly smaller a-value. If E(M)=E(M′), differing a-values would contradict their common degree; at equal degree the unique factor just proved forces M≅M′. This proves the assignment's injectivity.

4.1F2step 3.1algebra

Put Δ=End⁡H(M). A nonzero endomorphism of the simple finite-dimensional module is bijective, so Δ is a division k-algebra. It acts on T(M) by 1⊗d, commuting with Jk. Consequently it preserves every Jk-isotypic component. The E(M)-component has multiplicity one, so restriction gives a unital homomorphism Δ→End⁡Jk(VE(M))=k. The equality on the right follows from the full matrix block of the split algebra Jk. The homomorphism's kernel is zero because Δ is a division algebra, and its image contains all scalar maps. Thus Δ=k.

5.1step 4.1choosealgebra∎

We verify explicitly that Δ=k implies absolute simplicity here. A finite direct sum of copies of a simple module is semisimple: by induction, every submodule has a complement. Indeed, in S⊕U, split its intersection with U by the induction hypothesis, quotient that intersection, and consider its projection to S; this is zero or S, and in the latter case the remaining submodule is the graph of a homomorphism from S into the remaining summand of U. That graph has the remaining U as a complement. Now choose a k-basis m1,…,mr of M. The image of H→Mr, h↦(hm1,…,hmr), is a submodule. If it were proper, semisimplicity would give a nonzero map Mr→M vanishing on that image. Its components belong to End⁡H(M)=k, so they are scalars ci, not all zero. Evaluating at h=1 would give ∑icimi=0, contrary to basis independence. Thus the map is surjective. Every prescribed list of images of the basis is realized by some h, proving that H→End⁡k(M) is surjective. After any field extension, its image remains the full matrix algebra acting on the extended vector space; its standard module is simple. Hence every M is absolutely simple, and H is split.

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Filtered projectives prove canonical basic-set reciprocity

Statement

Assume the Axiom of Choice and the finite-Weyl data and Lusztig properties of Finite-Weyl Lusztig data and the precise basic-set hypotheses. Let θ:A→k have characteristic zero or θ(fE)≠0 for every generic simple label E. Put k0=Frac⁡(θ(A))⊆k, let R=Aker⁡θ^, and let F=Frac⁡R. Take the explicit global free model LE,A=A⊗ZΛE of the Schur supplier, whose Hecke matrices are integral because the J-matrices and ϕA are integral. Let LE=R⊗ALE,A. This is the standard free module of the E-matrix block of JR, restricted through ϕR; its freeness is by this construction, not an inference from torsion-freeness over R. Its fraction fibre is the generic simple EF; its residue is the restricted asymptotic simple ∗VE. Define

dE,M=[k⊗k0(LE/mRLE):M]

for simple Hk-modules M. These multiplicities agree with those of any other free stable R-models of the same generic simples. They are unchanged by extension from k0 to k, using the simple-label bijection.

For a simple Hk-module M, choose an idempotent e∈Hk such that Hke is its projective cover. Regarding the layers Bi=Ii/Ii+1 as left Jk-modules and right Hk-modules, one has

mult⁡Jk(VE,Bie)={dE,M,i=αE,0,i≠αE.

Moreover dE,M=[∗VE:M]. No identification of the right action on Bi with right multiplication by ϕk is assumed.

Facts & Assumptions

Given: The stated finite-Weyl data, exact Lusztig properties, good specialization, and the Axiom of Choice.

[F1]

The layers Bi are finite free before specialization, are (J,H)-bimodules with left H action through ϕ, and have J-support only in degree i. The generic ϕ is an isomorphism (The asymptotic algebra, filtered layers and the specialization homomorphism).

[F2]

Inverting the integers fE gives integral full matrix blocks for J, whose standard modules correspond through generic ϕ to the generic Hecke simples and whose degrees are αE (Leading Schur coefficients and split good-characteristic asymptotic specializations).

[F3]

R is a complete local domain with residue k0, fraction field containing Q(v), integral idempotent lifting, finite-projective freeness, and exact projected-layer base change. Multiplicities for an integral split matrix algebra are preserved between the fraction and residue fibres (Complete local modular systems and integral idempotent lifting).

[F4]

Every good specialization of H is split, and every simple M has endomorphism algebra its ground field (Asymptotic induction identifies leading modular simples).

[F5]

Every finite-dimensional module over a finite-dimensional algebra has a projective cover, unique up to isomorphism over its target (Every finite-dimensional module has a projective cover, unique up to isomorphism over the target); by definition its kernel is superfluous (An essential epimorphism is a surjection with superfluous kernel, and a projective cover is a projective source with such a map).

Proof

1.1F4F5choosealgebra

First work over k0 and write H0=Hk0. Corestrict θ to θ0:A→k0=Frac⁡(θ(A)); it has the same characteristic as k and every θ0(fE) is nonzero whenever θ(fE) is, so [F4] applies and H0 is split. For a simple M, take a projective cover π:P→M with superfluous kernel K by [F5]. A nonzero vector of M gives a surjection H0→M. Projectivity of the free module H0 lifts it to s:H0→P; the image of s together with K is P, so superfluity makes s surjective. Projectivity of P splits s, realizing P as a direct summand of H0. Its projection is right multiplication by an idempotent e, since a left-linear endomorphism of H0 is determined by its value at 1. Hence P≅H0e. Every maximal submodule of P contains K: otherwise its sum with K is P, contradicting superfluity. Since K itself is maximal, it is the unique maximal submodule, and the head of P is the single copy M.

1.2F4algebra

We justify extension to k without assuming an unproved radical base-change rule. For any finite-dimensional split algebra T over k0, choose representatives S1,…,Sr of its simple modules; there are finitely many because every simple is a quotient of the regular module and thus a factor of a composition series of T. The ideal N=⋂jAnn⁡T(Sj) is nilpotent: it annihilates each factor of such a series, so its successive powers lower the series and Ndim⁡T=0. The action map T→⨁jEnd⁡k0(Sj) is surjective. Indeed choose bases in the Sj and consider the image of T in the direct sum of the corresponding tuples. If this image were proper, semisimplicity of the direct sum of simples would give a nonzero map to some Sj killing the image. Maps between distinct simple modules are zero, and End⁡T(Sj)=k0, so this would yield a nontrivial scalar relation among the selected basis vectors of Sj by evaluation at 1. This is impossible. Thus T/N is the displayed product of full matrix algebras. Under extension to k, the ideal k⊗N stays nilpotent, hence annihilates every simple: if it acted surjectively on a simple, nilpotence would contradict its nonzeroness. The quotient is still a product of full matrix algebras. It follows that all simples are exactly the extensions of the Sj, and extending a composition series preserves its simple factors and multiplicities. For completeness, a finite direct sum of simple modules is semisimple by induction: split a submodule's intersection with the previous summands, quotient that intersection, and project to the final simple summand. The projection is zero or onto; in the latter case its remaining submodule is the graph of a homomorphism from that simple into the complementary previous summands, and that graph has those previous summands as a complement. This justifies the semisimplicity used in the simultaneous action-map argument.

2.1F4step 1.1algebra

For a simple M′, every nonzero map P→M′ has that unique maximal kernel K, so Hom⁡H0(P,M′) is k0 when M′=M and zero otherwise, using [F4]. The evaluation map Hom⁡H0(H0e,X)→eX, f↦f(e), is an isomorphism, with inverse x↦(he↦hx). Thus dim⁡eM′=1 for M′=M and zero otherwise. Multiplication by e is exact, so applying it along any composition series of a finite-dimensional module X yields [X:M]=dim⁡k0eX.

3.1F2F3step 2.1algebra

By [F3] lift e to an idempotent q∈HR. The model LE is free by the explicit integral construction in [F2]. If L is any other explicitly R-free stable model of EF, then qL is a direct summand of L, hence free with equal generic and residue ranks. Therefore [L/mRL:M]=dim⁡e(L/mRL)=dim⁡FqEF. The last expression is independent of L. In particular it applies to the free JR-standard model LE from [F2], proving dE,M=[∗VE:M] over k0 and agreement with every other free model. If a chosen model was initially free over Aker⁡θ, extension to R is a free model of this same generic representation and its residue is the original specialized module, so the same equality applies. The explicit global model in [F2] itself gives a free Aker⁡θ-model. No assertion about arbitrary nonfree torsion-free lattices, or exactness of their reduction, is made.

4.1F1F2F3step 3.1algebra

Filter HRq by Iiq. Exact projection gives its layer Bi,Rq, which is finite free over R and is a left JR-module because right HR commutes with left JR. By [F2] and [F3] its E-multiplicity is the same in the generic and residue fibres. In the generic fibre, [F1] identifies its JF-simples with the Hecke simples EF, and only layer i=αE can contain EF. Additivity of composition multiplicities along the finite filtration therefore says that its multiplicity in that layer is its multiplicity in HFq. On the matrix block End⁡F(EF), right multiplication by q has image consisting of matrices with rank⁡(q∣EF) independent columns after a basis change; as a left module this is exactly that many copies of EF. Consequently the multiplicity is dim⁡FqEF=dE,M by step 3.1. Reduction gives the asserted reciprocity over k0, with zero multiplicity in all other degrees.

5.1F1F3F4F5step 1.2step 2.1step 4.1algebra∎

Apply step 1.2 to T=H0 and to the split algebra Jk0. Their simple labels, the reductions defining d, and the decompositions of the layers all extend with unchanged multiplicities. For P=H0e, let N be the nilpotent ideal from step 1.2 and K the kernel of its projective-cover map. Since N annihilates M, NP⊆K, so P/NP is nonzero. This quotient is semisimple over H0/N, and every simple quotient of it is a simple quotient of P, hence is M by step 2.1. Moreover, Hom⁡H0(P/NP,M)≅Hom⁡H0(P,M)=k0 by step 2.1, so P/NP≅M and K=NP. After extension, the kernel is (k⊗N)(k⊗P) and the quotient is the extended simple M. This kernel is superfluous: if a submodule together with it generates k⊗P, the quotient by that submodule equals its image under the nilpotent ideal k⊗N, and iteration forces the quotient to be zero. Thus the extended idempotent again gives a projective cover with simple head M. Therefore reciprocity from step 4.1 holds over k for these idempotents. Any other projective cover of M is isomorphic to it by [F5]; an isomorphism Hke≅Hke′ is represented by mutually inverse corner elements, so right multiplication by those elements identifies Bie and Bie′ as Jk-modules. The formula therefore holds for every idempotent allowed in the statement, completing the proof.

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Finite-Weyl canonical basic sets from Lusztig properties

Statement

Assume the Axiom of Choice. Let W be a finite Weyl group with integral nonnegative weight function L, and impose exactly the generic splitting and Lusztig properties specified in Finite-Weyl Lusztig data and the precise basic-set hypotheses, namely P2–P8 and P15′. Let HA be its Hecke algebra over A=Z[v,v−1]. For every unital specialization θ:A→k into a field, assume that k has characteristic zero or that every leading Schur integer fE is nonzero in k. Write the generic Schur element as cE=fEv−2αE plus terms of strictly higher v-degree.

Then Hk is split and has a unique canonical basic set for the decomposition matrix dE,M furnished by the free asymptotic models in Filtered projectives prove canonical basic-set reciprocity. Explicitly, there is an injection M↦E(M) from simple Hk-labels to generic labels, with

dE(M),M=1,αE(M)=min⁡{αE:dE,M>0},

and

dE,M>0 ⟹ E=E(M) or αE>αE(M).

Its image is the canonical basic set of Canonical basic sets for split Hecke specializations. In normalized generators the parameters are θ(v)L(s); in Geck's multiplicative generators they are θ(v2)L(s). No condition θ(cE)≠0 is imposed: nonsemisimple specializations are included. The Lusztig properties here are hypotheses, not universal assertions for all unequal weights or all Coxeter groups.

Facts & Assumptions

Given: The finite-Weyl data, the stated P2–P8 and P15′ hypotheses, the good specialization, and the Axiom of Choice.

[F1]

The homomorphism is ϕ(Dx)=∑z∈W, d∈Da(d)=a(z)hx,d,zndtz, with the sum over z∈W and distinguished d∈D. The layers Bi are (J,H)-bimodules, and P4 gives a(x)≤a(z) whenever hx,d,z≠0 (Finite-Weyl Lusztig data and the precise basic-set hypotheses, The asymptotic algebra, filtered layers and the specialization homomorphism).

[F2]

The Jk-simple VE has support in degree αE, the lowest Schur exponent; Jk is split under the nonvanishing of the leading integers fE (Leading Schur coefficients and split good-characteristic asymptotic specializations).

[F3]

The algebra Hk is split. For each simple M, with aM=max⁡{a(w):DwM≠0}, there is an injective assignment M↦E(M) with αE(M)=aM and [∗VE(M):M]=1 (Asymptotic induction identifies leading modular simples).

[F4]

The completion/free-model construction is available for every θ, including field extensions of its prime-generated residue field. It gives dE,M=[∗VE:M] and mult⁡Jk(VE,Bie)=δi,αEdE,M for a projective cover Hke of M (Complete local modular systems and integral idempotent lifting, Filtered projectives prove canonical basic-set reciprocity).

[F5]

The canonical basic-set axioms are multiplicity one, attainment of the least α in each column, and strict inequality for every other positive entry in that column (Canonical basic sets for split Hecke specializations).

Proof

1.1F1F2F4choosealgebra

Suppose dE,M>0. Choose w with a(w)=aM and DwM≠0. Since M is a composition factor of ∗VE by [F4], Dw cannot act as zero on that whole module. Thus ϕ(Dw) acts nontrivially on VE. In the formula of [F1], some surviving summand has hw,d,z≠0 and tzVE≠0. The latter implies a(z)=αE by [F2], while P4 gives aM=a(w)≤a(z). Hence every positive entry satisfies aM≤αE.

2.1F3F4step 1.1algebra

By [F3] and [F4], dE(M),M=1 and αE(M)=aM. Together with step 1.1 this proves that every column is nonzero and its least α is exactly aM. The assignment M↦E(M) is already injective. It remains to prove uniqueness of a generic label at that minimum.

2.2F1F2F3F4F6step 1.1choosealgebra

Fix M and a projective cover P=Hke as in [F4]. Put b=min⁡{i:Bie≠0}. The finite filtration starts with I0e=P and ends with zero, so this minimum exists, and the vanishing earlier layers implies P=Ibe. The quotient Pb=Bbe=P/Ib+1e is nonzero. The kernel K of the projective-cover map P→M is maximal, and superfluity makes it the unique maximal submodule: any proper submodule not contained in K would sum with K to P. Hence Ib+1e⊆K, so the cover map factors through a surjection πˉ:Pb→M. Its kernel Kˉ=K/Ib+1e is superfluous in Pb, since any submodule whose sum with Kˉ is Pb lifts to a submodule whose sum with K is P. The kernel Kˉ is also maximal because the quotient is simple. Therefore it is the unique maximal submodule and Pb has simple head M. This makes Pb indecomposable: a direct sum of two nonzero finite-dimensional modules has at least two simple summands in its head, even if isomorphic. But Pb is semisimple as a Jk-module and each Jk-summand is an Hk-submodule, since the action restricts through ϕ. Consequently it is exactly one VE1, with multiplicity one. Reciprocity gives αE1=b and dE1,M>0. Step 1.1 yields aM≤b. Conversely, [F3] and [F4] give dE(M),M=1 and αE(M)=aM, so reciprocity makes BaMe nonzero and b≤aM. Hence b=aM. Reciprocity then puts VE(M) in the single Jk-simple summand of Bbe, so E1=E(M) and dE1,M=1.

3.1F4step 2.1step 2.2algebra

If dE,M>0 and αE=aM, reciprocity puts VE in the nonzero layer BαEe, so αE≥b. Since aM≤b by step 2.2, equality holds throughout. The unique summand in Bbe is VE1, so E=E1. This applies to E(M) by step 2.1, giving E1=E(M). Thus a positive entry at the least α has precisely the label E(M); every other positive entry has strictly larger α.

4.1F2F3F4F5step 1.1step 3.1algebra∎

The image of the injection in [F3] now satisfies all axioms in [F5], proving existence. Those axioms also make the generic label the unique minimum in each column, proving uniqueness of the set and bijection. The parameter identities follow from Ss=vL(s)Ts, which changes (Ts−vL(s))(Ts+v−L(s))=0 into (Ss−v2L(s))(Ss+1)=0; applying θ gives the claimed specializations. Only fE was inverted in [F2] and [F4], and step 1.1 used the explicitly assumed Lusztig properties. Hence the proof imposes neither full-Schur nonvanishing nor any unstated general Coxeter assertion.

Source notes

This is Geck's Theorem 6.6 under its standing Section 5.2 hypotheses. Geck cites the asymptotic-algebra constructions, sketches the leading-Schur argument and splitting, and refers elsewhere for Proposition 6.7. The local supplier chain named above supplies these arguments; citations record provenance rather than replacing proof. In particular the reciprocity proof uses projected free modules over a complete local domain, so it does not assert that the right layer action is right multiplication by ϕ.

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Weighted cell quotients and the leading finite-Weyl basic-set labels

Statement

Under the hypotheses of Finite-Weyl canonical basic sets from Lusztig properties, the function a is constant on every left, right and two-sided weighted cell. Each a-layer of the KL cell filtration has a finite filtration with cell quotients. For the dagger basis Dw=Cw†, these quotients are the dagger twists of the native cell modules of Unequal-parameter left, right, and two-sided cells and cell quotients: on the twist, h acts as h† on the original module.

Every generic simple E occurs in a dagger-twisted left cell module with cell a-value αE, and every generic constituent of such a module has that same Schur exponent. For each specialized simple M, its canonical basic-set label E(M) occurs in a dagger-twisted generic left cell module of a-value aM=αE(M), whose specialization contains M. In that specialization the contribution from E(M) has multiplicity one per generic copy, and every other generic label contributing to M has strictly larger Schur exponent; hence no other generic label of that same cell a-value contributes to M.

This is a general finite-Weyl cell/basic-set connection, including nonsemisimple fibers. It does not assert that every cell module is simple or that cells themselves are in bijection with special simples.

Facts & Assumptions

Given: The specified finite-Weyl weight, exact Lusztig properties, generic splitting, good specialization, and Axiom of Choice of the cited theorem.

[F1]

Unequal-parameter left, right, and two-sided cells and cell quotients and Weighted cell quotients are well-defined modules and bimodules give the coefficient preorders, ideal closure and bases of the left/right/two-sided cell quotients.

[F2]

Finite-Weyl Lusztig data and the precise basic-set hypotheses and The asymptotic algebra, filtered layers and the specialization homomorphism give P4, D=C†, the same structure constants, the filtration Ii, and Bi≅JAi with left H action via ϕ and split generic ϕ. Each J-simple VE has a unique support degree νE.

[F3]

Complete local modular systems and integral idempotent lifting and Filtered projectives prove canonical basic-set reciprocity give the complete local ring, exact projected free layers, and dE,M=dim⁡FqEF for a lifted projective-cover idempotent q.

[F4]

Finite-Weyl canonical basic sets from Lusztig properties gives the unique label E(M), dE(M),M=1 and strict Schur-exponent inequality for every other contributing label.

Proof

1.1F1F2algebra

If a coefficient transition leads from y to x, P4 applied to its generator product gives a(x)≥a(y). This holds on both sides and along every finite preorder chain. Mutual comparison therefore makes a constant on each cell of all three types. Dagger is an algebra involution and carries CxCy=∑zhx,y,zCz to the identical formula in D; hence the coefficient preorders have the same labels. The map from the dagger quotient to the native quotient sending [Dw] to [Cw] intertwines the action of h on the former with h† on the latter. This proves the precise twist convention.

2.1F1F2step 1.1constructalgebra

Fix an integer i and consider the finite set of left cells with value i. Their preorder descends to a partial order because mutual comparison is the cell equivalence. Repeatedly take a minimal remaining cell to obtain a total listing with every smaller cell earlier. This finite construction terminates as the number of remaining cells decreases by one. In Bi, the spans of initial unions in that listing are left submodules: an action term either has strictly larger a and vanishes in the layer, or has the same a and lies in a cell no later than the input cell. Their successive quotients have exactly one cell as basis and exactly its quotient multiplication law, by [F1]. The same argument on right or two-sided cells gives the corresponding filtrations with their sidedness. These modules and their successive layers are free in their displayed bases.

3.1F2F3step 2.1algebra

Over the fraction field F of [F3], HF≅JF and the layer Bi,F≅JFi is its regular support ideal. Its generic simple constituents are exactly the EF with support degree νE=i, each with positive multiplicity: in a matrix block MdE(F) the left regular module consists of dE copies of its standard simple. For each E, the explicit free model in [F3] has nonzero finite-dimensional residue, hence some simple factor M with dE,M>0. Reciprocity in [F3] then puts VE in BαE,ke for a projective-cover idempotent e of M. Since Bi is supported in J-degree i by [F2], this forces νE=αE. Thus the generic simple constituents of Bi,F are exactly the labels with αE=i. Additivity along the finite cell filtration in step 2.1 shows that every such EF occurs in at least one dagger cell quotient and that every generic constituent of each of those quotients has exponent i. The same statements hold over Q(v) because all generic blocks are split and extension to F preserves their multiplicities.

4.1F3step 2.1step 3.1algebra

For a fixed special simple M work first over its prime-generated field k0, as in [F3], and lift its projective-cover idempotent e to q over the complete local ring. If XR is any displayed free dagger cell module, then qXR is a direct summand of a finite free R-module, so it is finite projective and local-free. Its residue and generic ranks agree. Exactness of multiplication by e along a composition series gives [Xk0:M]=dim⁡k0eXk0=dim⁡FqXF=∑E[XF:EF]dE,M, where the last equality follows from split generic decomposition and [F3]. The field-extension part of [F3] preserves this equality over k. No reduction-exactness assertion for arbitrary nonfree lattices is used.

5.1F4step 3.1step 4.1algebra∎

Take E=E(M) and i=αE=aM. Step 3.1 supplies a dagger cell module X of value i with [XF:EF]>0. The sum of nonnegative integers in step 4.1 then has a positive contribution [XF:EF]dE,M=[XF:EF], so M occurs in its specialization. By [F4], any other generic label contributing to M must have exponent strictly larger than i. Step 3.1 says all constituents of this cell module have exponent i, so those other contributions vanish. Thus the selected label gives precisely the claimed leading contribution, without asserting that the cell module has only one generic constituent or one special factor.

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The scope and proof status of the finite-Weyl basic-set theorem

Remark

The general local basic-set theorem is the finite-Weyl theorem corresponding to Geck's Theorem 6.6, with its standing section 5.2 hypotheses P2–P8 and P15′ written explicitly. The local chain supplies the asymptotic algebra, integral homomorphism and layer compatibility, Schur leading coefficients, good-characteristic splitting, actual free integral models, lifted-idempotent reciprocity and strict triangularity. Geck's notes cite Lusztig for the algebra constructions, sketch the leading-term and splitting arguments, and refer elsewhere for Proposition 6.7; those source omissions are supplied locally rather than silently treated as proofs.

The hypotheses are finite Weyl W, nonnegative integral L, the split generic setup, θ:Z[v±1]→k with θ(v)≠0, and characteristic zero or L-good characteristic: every leading Schur integer fE is nonzero. The multiplicative parameter is ξ=θ(v)2. The full Schur elements may vanish. Requiring all θ(cE)≠0 would instead restrict the theorem to a semisimple identity-decomposition situation and would lose its modular content. The general theorem and its cell corollary retain that content.

These statements prove a conditional implication under the exact stated Lusztig properties; they do not prove those properties for an unspecified unequal weight. As source-status context, Geck section 5.2 records proofs in the equal-parameter finite-Weyl case, in asymptotic type Bn with b>(n−1)a>0, and the b=0,a>0 type-D reduction, with citations to the relevant original papers. His type G2 and F4 discussions also describe separate calculation-based results. This is a dated account of that source's regimes, not a current census and not a logical premise asserting their proofs locally. No result for arbitrary Coxeter groups or universal P1–P15 is inferred.

The cell corollary uses the dagger twist explicitly. It links the unique leading generic basic-set label to a cell quotient and its specialization; it does not replace a canonical basic set by all cell labels or claim all cell modules are irreducible.

5 · Examples, counterexamples and false statements

None yet.

Sources