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The q=2 torus boundary

Example

Assume the Axiom of Choice, used through Tits deformation. For q=2 the multiplicative group F2× is trivial, so the diagonal torus T≅(F2×)n is trivial and there is exactly one character χ=1 of T for every n: the regular case is empty for n≥2 (for n=1 the unique coordinate is vacuously pairwise distinct), Wχ=Sn for all n, and every principal series is spherical, I(χ)=I(1)=C[G/B]. The general theorems remain valid: dim⁡End⁡G(I(1))=∣Sn∣=n!, the constituents are indexed by partitions λ⊢n with multiplicities fλ, and the finite Hecke algebra Hq(n) at q=2 is semisimple by The finite spherical Hecke algebra is semisimple with nondegenerate trace form, so Tits deformation still identifies it with C[Sn]. Its generators also satisfy Ti2=Ti+2, with distinct roots 2 and −1. The boundary phenomenon is the collapse of the parametrising torus and of the Weyl action, not a failure of the constituent description.

Facts & Assumptions

Given: The prime power q=2, the group G=GL⁡n(F2) with Borel B and diagonal torus T, its character group T^, the Weyl group W=Sn with its action on T^, and the spherical principal series I(1).

[F1]

For q=2 the group F2× is trivial, so T≅(F2×)n is trivial and T^={1}; the Weyl action is trivial and Wχ=Sn for the unique character, while the regular case consists of characters whose coordinates are pairwise distinct (Diagonal torus characters and the Weyl action).

[F2]

I(1)≅C[G/B], the permutation module on the complete flags (The spherical principal series is the flag permutation module).

[F3]

dim⁡CEnd⁡G(I(χ))=∣Wχ∣, so for the unique character this dimension is n! (The Weyl stabiliser controls the principal series endomorphisms).

[F4]

The constituents of the spherical principal series are indexed by the partitions λ⊢n with multiplicities fλ, the numbers of standard tableaux (The constituents of the spherical principal series of GL_n).

[F5]

The finite Hecke algebra Hq(n) is semisimple, with quadratic relation Tsi2=(q−1)Tsi+q 1; at q=2 this is Tsi2=Tsi+2, whose two roots 2 and −1 are distinct (The finite spherical Hecke algebra is semisimple with nondegenerate trace form, The rank-one quadratic relation in the finite Hecke algebra).

[F6]

Assume AC; Tits deformation identifies Hq(n) with C[Sn] for every prime power q, hence also for q=2 (The finite Hecke algebra is non-canonically isomorphic to the group algebra of S_n, The Axiom of Choice).

Verification

technique · direct
1.1F1F2

For q=2 the group F2×={1} is trivial, so the diagonal torus T≅(F2×)n is the trivial group and its character group has the single element 1; the Weyl action fixes it, so W1=Sn, and every principal series is I(1). A regular character would need pairwise distinct coordinates, impossible in a one-element group when n≥2; for n=1 the single coordinate is vacuously pairwise distinct.

1.2F3F4

Since the unique character is fixed by W, [F3] gives dim⁡CEnd⁡G(I(1))=n!, and [F4] gives the constituent indexing by partitions with multiplicities fλ.

1.3F5F6

By [F5] the Hecke algebra is semisimple with quadratic relation Tsi2=Tsi+2 at q=2, and the two roots 2≠−1 are distinct; by [F6] Tits deformation identifies it with C[Sn] in this case as in every other. Hence the collapse of T^ to a point and of the Weyl action to the trivial action is a genuine boundary phenomenon of the parametrising torus, while the endomorphism algebra, the constituent multiplicities and the Tits isomorphism retain their general form.

2.1F1F2F3F4F5F6∎

Steps 1.1-1.3 establish the two boundary statements: the torus and the regular characters collapse, whereas the endomorphism algebra, the partition parametrisation with multiplicities fλ and the Tits isomorphism to C[Sn] remain valid. AC is carried only from the Tits-deformation supplier [F6], as declared.

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