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Affine Hecke Algebras Beyond Type A: Examples and Counterexamples

1 · Prerequisites

2 · Summary

These examples test the root-data and parameter conventions on the affine B2 Coxeter system and compare a positive p-adic parameter with a finite type-A root-of-unity parameter. The computations prove only the displayed relations and scalar boundary; they supply no general Bernstein PBW or tempered/Langlands classification theorem.

Affine root-data example

A rank-two affine B2 Hecke algebra with unequal parameters gives the paired B2 lattices, short and long coroots, affine simple reflections, Coxeter diagram, two positive parameters, and the resulting Iwahori–Matsumoto basis.

Parameter-boundary example

A positive p-adic parameter and a finite root-of-unity parameter computes quantum characteristic ∞ for the positive real parameter 3 and 4 for the finite parameter i. This distinguishes parameter regimes without asserting that the affine and finite Hecke algebras cannot be equivalent.

Companion: affine-hecke-algebras-beyond-type-a.

The selected SL⁡2(Q3) Iwahori corner is now proved on the A page, with Haar normalization and explicit root-coset counts. The scalar example uses no category equivalence or choice assumption; the corner theorem carries its own AC hypothesis.

3 · Logical flowchart

4 · Definitions, theorems and proofs

None yet.

5 · Examples, counterexamples and false statements

ExampleConstruction: AI-generatedVerification: AI-generatedprecheck passOpen item page →

A positive p-adic parameter and a finite root-of-unity parameter

Example

Take the unnormalized split p-adic Iwahori parameter qF=3 (for instance, the residue-field cardinality of Q3) and the finite type-A Hecke parameter ξ=i∈C×. The first is positive real and greater than 1; the second is a primitive fourth root of unity. Their quantum characteristics differ, so the parameters belong to different regimes. This calculation does not assert that the resulting affine and finite Hecke algebras are nonisomorphic or non-Morita-equivalent.

Facts & Assumptions

Given: The affine parameter qF=3 and the finite type-A parameter ξ=i.

[F1]

Every real affine parameter q>1 has e(C,q)=∞ (A real affine-Hecke parameter greater than one has infinite quantum characteristic).

[F2]

For a field F and u∈F×, the quantum characteristic is the least n≥2 with 1+u+⋯+un−1=0, or ∞ if no such n exists (The quantum characteristic of an invertible Hecke parameter).

Verification

Given: qF=3 and ξ=i as above.

1.1F1givenalgebra

Since 3>1, [F1] gives e(C,3)=∞.

1.2F2givenalgebra

The first candidate geometric sums for i are 1+i≠0, 1+i+i2=i≠0, and 1+i+i2+i3=0. By the least-exponent definition [F2], e(C,i)=4.

2.1step 1.1step 1.2algebra∎

Thus the p-adic positive-real parameter has infinite quantum characteristic and the finite type-A root-of-unity parameter has finite quantum characteristic 4. Since ∣3∣=3 and ∣i∣=1, they are different scalars. These calculations establish only the stated parameter distinction.

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A rank-two affine B2 Hecke algebra with unequal parameters

Example

Let E=R2 with the dot product and standard vectors e1,e2. Set

Y=Z(e1−e2)+Z(2e2)={(a,b)∈Z2:a+b is even},X=Ze1+Z12(e1+e2).

The displayed bases of X and Y are dual under the dot product. Let

Φ={±e1,±e2,±(e1+e2),±(e1−e2)},

with coroot α∨=2α for the short roots α=±ei and α∨=α for the long roots α=±e1±e2. Choose Δ={α1=e1−e2,α2=e2}. The affine alcove is

A0={(x1,x2):0<x2<x1, x1+x2<1}.

Its simple reflections are s1(x1,x2)=(x2,x1), s2(x1,x2)=(x1,−x2), and s0(x1,x2)=(1−x2,1−x1). The affine Iwahori–Matsumoto parameters are qs0=qs1=2 on the long-root walls and qs2=3 on the short-root wall.

Facts & Assumptions

Given: The lattice pair X,Y, root and coroot sets, simple roots, and affine alcove stated above.

[F1]

A reduced root datum consists of finite-rank free lattices in perfect integral duality, a finite root set and coroot set in bijection, and Weyl reflections preserving both sets (Abstract root data and their Weyl groups).

[F2]

The Iwahori–Matsumoto algebra uses (Ts−qs)(Ts+1)=0 and the affine Coxeter braid relations; Ns=qs−1/2Ts satisfies (Ns−qs1/2)(Ns+qs−1/2)=0 (The Iwahori–Matsumoto affine Hecke algebra of a based root datum).

[F3]

For a reduced crystallographic root system, affine reflections in the integer root hyperplanes generate the affine Coxeter group, whose simple reflections are those of the fundamental alcove; the product order of two simple wall reflections is determined by the angle between their walls (Affine root hyperplanes, coroot translations, alcoves, and the affine reflection group, Alcove transitivity, the affine Coxeter presentation, and the length function).

[F4]

In the generic Coxeter Hecke presentation, parameters are allowed exactly when they are constant on the odd-edge connected components of the simple-generator graph; simple generators are conjugate exactly within those components (Universal parameters, the generic Coxeter Hecke algebra and generator conjugacy).

[L1]

The elements TwUω form a basis of the extended Iwahori–Matsumoto algebra (The extended Iwahori–Matsumoto basis).

Verification

Given: The proposed B2 root datum and affine Hecke parameters.

1.1F1givenalgebra

The vectors e1 and 12(e1+e2) form a basis of X, while e1−e2 and 2e2 form a basis of Y: an integer pair (a,b) has even coordinate sum exactly when (a,b)=a(e1−e2)+a+b2(2e2). The dot-product matrix between these two bases is the identity, so the pairing is perfect and integral. The roots lie in X, the coroots lie in Y, and direct pairings on α1,α2 give the Cartan matrix (2−2−12). The positive roots are α1,α2,α1+α2=e1,α1+2α2=e1+e2, so Δ is a base and the root set is reduced. The displayed root set is the union of the signed-permutation orbits of α1 and α2. The prescribed coroot map is equivariant under signed permutations: it doubles each short root and fixes each long-root vector, and signed permutations preserve root length. Thus the simple-root checks give ⟨α,α∨⟩=2 for every listed root, and the generated reflections preserve both root sets. The signed-permutation group generated by s1,s2 is finite. Therefore [F1] applies and these data are a reduced based B2 root datum.

1.2F3givenalgebra

The simple walls of A0 are x1=x2, x2=0, and x1+x2=1. In its interior, 0<x2<1, 0<x1−x2<1, and 0<x1+x2<1; the remaining positive-root function satisfies 0<x1<1 because x2>0 and x1+x2<1. Thus no other integer root wall cuts it. Their reflections are respectively the displayed s1,s2,s0. The product s1s2 is (x1,x2)↦(−x2,x1), a quarter-turn of order 4. The product s2s0 is (x1,x2)↦(1−x2,x1−1); it fixes (1,0) and its linear part about that point is the same quarter-turn, so it has order 4. The product s0s1 is (x1,x2)↦(1−x1,1−x2), a half-turn of order 2. Hence the affine Coxeter labels are m(s1,s2)=m(s2,s0)=4 and m(s1,s0)=2.

2.1F2F4step 1.2algebra

The affine roots defining s0 and s1 are long and the one defining s2 is short. The displayed basis of Y is α1∨,α2∨, so Y=Q∨ and Ω=1 by [F2]. Thus conjugacy in the extended group is conjugacy in the affine Coxeter group. The Coxeter labels just computed are all even, so the odd-edge graph has three singleton components; by [F4] the three assigned positive parameters are constant on every required conjugacy class. In the symmetric convention the parameters are vs0=vs1=2 and vs2=3, with the quadratic relations of [F2].

3.1F2L1step 1.1step 1.2step 2.1∎

Here Y=Q∨, so the extended group has trivial length-zero quotient and Ω={1}. Applying [L1] to the affine Coxeter system identified in step 1.2, with the valid affine Coxeter parameters from step 2.1, shows that {Tw:w∈Waff} is a C-basis. This verifies the claimed unequal-parameter affine B2 example.

Coxeter diagram

The nodes label the three affine simple reflections. An edge labelled 4 means the product of the two reflections has order 4; no edge between s0 and s1 means their product has order 2. The node text records which walls are long-root and short-root walls.

s0s2s144longshortlong

Sources