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The rank-one Hecke parameter for equal torus characters

Statement

For Weyl-sorted η, each simple s∈Sη exchanges two adjacent equal coordinates a,a. The associated rank-one Levi has principal series (a∘det⁡)⊕(St⁡⊗a∘det⁡) on its GL⁡2 factor, tensored with one-dimensional characters on the remaining torus factors, with constituent degrees 1,q. The canonical raw intertwiner has eigenvalues a(−1)q and −a(−1). The normalized Ts=a(−1)−1Bs satisfies Ts2=(q−1)Ts+q id; thus the parameter is exactly q, and the normalization of Length-additive products of the standard intertwiners gives λw=∏rar(−1)−ℓ(wr). For arbitrary χ this assertion holds for the transported generators after Weyl sorting. In particular the naive generator fails the parameter-q relation when a(−1)=−1: for q=3 and the nontrivial character of F3×, its eigenvalue on a∘det⁡ is −3, which is neither 3 nor −1. No choice principle is used.

Facts & Assumptions

Given: A Weyl-sorted character η=(a1n1,…,aknk) of the diagonal torus T of G=GL⁡n(Fq) with distinct ar, a simple reflection s∈Wη in the block r of size nr≥2, the characters ψr=ar∘det⁡ and ρ=∏rar∘det⁡r of L=∏rGL⁡nr(Fq), the idempotents er=∣Br∣−1∑b∈Brη~r(b)−1b and eBr, and the operators Bs=RΘs−1, Ts=ρ(s˙)−1Bs of Standard intertwining operators for the finite principal series and Length-additive products of the standard intertwiners.

[F1]

For the block GL⁡nr the standard basis element Ts(r)=q eBrs˙eBr satisfies Ts(r)2=(q−1)Ts(r)+q eBr (The rank-one quadratic relation in the finite Hecke algebra, The Bruhat double-coset basis of the finite Hecke algebra).

[F2]

The map mr(g)=ψr(g)−1g is an algebra automorphism of C[GL⁡nr(Fq)] with mr(eBr)=er; it sends Ts(r)=q eBrs˙eBr to ψr(s˙)−1Θs(r) with Θs(r)=q ers˙er, because ψr(b)=ar(det⁡b)=η~r(b) for upper triangular b (The group ring R[G] is a unital R-algebra with basis G, and each g∈G is a unit of R[G], For same-sized finite square matrices over a commutative ring, det⁡(AB)=det⁡(A)det⁡(B), The determinant of a triangular matrix is the product of its diagonal entries, Length-additive products of the standard intertwiners, The principal series module for finite GL_n).

[F3]

ψr(s˙)=ar(det⁡Ps)=ar(−1)∈{1,−1}, and ρ(s˙)=ar(−1) for s in block r. The element Θs(r) satisfies Θs(r)2=(q−1)ψr(s˙)Θs(r)+q er, and er acts as the identity on the module erC[GL⁡nr]er. [F2, algebra]

[F4]

For the rank-one Levi M=GL⁡2(Fq)×(Fq×)n−2 attached to s, the principal series of the restriction of η is [(a∘det⁡)⊕(St⁡⊗a∘det⁡)]⊠ξ with ξ a one-dimensional character of (Fq×)n−2; in particular its constituents have degrees 1 and q, and the constituent of degree 1 is isomorphic to ρ restricted to M (The equal-coordinate rank-one principal series of GL_2, Compositions, partial flags, and standard parabolics, Block Levi decomposition of standard parabolics).

[F5]

On the M2=GL⁡2(Fq) factor of the rank-one Levi, the idempotent models of I(1) and I(a,a) are C[M2]eB2 and C[M2]eψ, respectively (Principal series endomorphisms as the chi-idempotent corner). The spherical operator RTs has eigenvalues q on the trivial constituent and −1 on St⁡ (The equal-coordinate rank-one principal series of GL_2).

Proof

technique · direct
1.1F1F2F3algebra

Fix s in block r. Apply the algebra automorphism mr of [F2] to the block identity Ts(r)2=(q−1)Ts(r)+q eBr of [F1]: since mr is multiplicative and mr(Ts(r))=ψr(s˙)−1Θs(r), one gets ψr(s˙)−2Θs(r)2=(q−1)ψr(s˙)−1Θs(r)+q er, that is Θs(r)2=(q−1)ψr(s˙)Θs(r)+q er because ψr(s˙)2=1.

1.2F2F4F5algebra

Write the rank-one Levi as M2×D with M2=GL⁡2(Fq) and D=(Fq×)n−2 carrying the character ξ of [F4]. Covariant functions on this product satisfy f(g,d)=ξ(d)−1f(g,1), identifying its principal series with IM2(a,a)⊠ξ. Put ψ=a∘det⁡ on M2. The map m(g)=ψ(g)−1g of [F2] sends C[M2]eB2 bijectively to C[M2]eψ and satisfies m(hv)=ψ(h)−1h m(v). It therefore identifies IM2(1)⊗ψ with IM2(a,a) and intertwines RTs with Rm(Ts), since m(vTs)=m(v)m(Ts). Here m(Ts)=a(−1)−1Θs, the normalized operator. By [F5] its eigenvalues are q and −1 on the respective degree-1 and degree-q constituents; tensoring with ξ preserves these scalars. The raw intertwiner thus acts by a(−1)q and −a(−1) on those constituents.

2.1F3step 1.1algebra

On the module erC[GL⁡nr]er the idempotent er acts as the identity, so the operator RΘs(r) on this module satisfies RΘs(r)2=(q−1)ψr(s˙)RΘs(r)+q id; in the ambient corner eηGC[G]eηG the element Θs(r) is corrected by the idempotent eUP, whose right multiplication acts as the identity on C[G]eηG, so the raw operator Bs on I(η) satisfies Bs2=(q−1)ar(−1)Bs+q id with ar(−1)=ψr(s˙) by [F3].

3.1step 2.1algebra

Put Ts=ρ(s˙)−1Bs=ar(−1)−1Bs, which is the normalization of Length-additive products of the standard intertwiners; since ar(−1)2=1, multiplying the relation of step 2.1 by ar(−1)−2 gives Ts2=(q−1)Ts+q id. Hence the polynomial (X−q)(X+1) annihilates Ts, so every eigenvalue of Ts on any finite-dimensional constituent of I(η) lies in {q,−1}, and every eigenvalue of the raw operator Bs=ar(−1)Ts lies in {ar(−1)q, −ar(−1)}.

4.1F4step 3.1givenalgebra

For the normalization, ρ(w˙)=∏rar(det⁡Pwr)=∏rar(−1)ℓ(wr) for w∈Wη, so the factor λw=ρ(w˙)−1 of Length-additive products of the standard intertwiners is exactly ∏rar(−1)−ℓ(wr); for an arbitrary χ the transported generators of that lemma inherit the relation Ts2=(q−1)Ts+q id through the sorting isomorphism. For q=3 and the nontrivial character a of F3× one has a(−1)=a(2)=−1, so the raw eigenvalue on a∘det⁡ is a(−1)q=−3, which is neither 3 nor −1: the naive generator fails the parameter-q relation.

5.1step 1.1step 1.2step 2.1step 3.1step 4.1∎

Steps 1.1, 2.1 and 3.1 compute the rank-one quadratic relation with parameter exactly q after normalization; step 1.2 identifies the two constituent degrees and eigenvalues, and step 4.1 records the normalizing cocharacter λw, the transport to arbitrary χ and the explicit q=3 failure of the naive normalization. All groups, idempotents and eigenvalues are explicit and finite, and no choice principle is used.

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