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The constituents of a general finite principal series

Statement

Assume the Axiom of Choice, used through Tits deformation. Let G=GL⁡n(Fq), χ∈T^ with equal-character blocks of sizes n1,…,nk and Weyl stabiliser Wχ=Sn1×⋯×Snk. Then the isomorphism classes of simple constituents of the principal series I(χ) are indexed by the tuples (λ(1),…,λ(k)) of partitions λ(r)⊢nr, and the multiplicity of the constituent attached to such a tuple equals ∏r=1kfλ(r), the product of the numbers of standard tableaux of the parts; equivalently End⁡G(I(χ))≅∏(λ(1),…,λ(k))M⁡∏rfλ(r)(C). In particular, if χ is regular (k=n, all nr=1) then I(χ) is irreducible, and if χ is trivial (k=1, n1=n) the multiplicities are the hook-length numbers fλ of The constituents of the spherical principal series of GL_n.

Facts & Assumptions

Given: G=GL⁡n(Fq) with Borel B and diagonal torus T, a character χ∈T^ with equal-character block sizes n1,…,nk, the stabiliser Wχ=Sn1×⋯×Snk, the principal series I(χ) and its endomorphism algebra E=End⁡G(I(χ)).

[F1]

Assume AC; E≅⨂rHq(Snr)=Hq(Wχ), and E≅C[Wχ] preserving the number and dimensions of simple modules, with the identification E≅Hq(Wχ) itself choice-free (The endomorphism algebra of a general finite principal series, The Axiom of Choice).

[F2]

C[G] and hence every finite-dimensional complex G-module is semisimple (Maschke's theorem for finite groups over fields whose characteristic does not divide ∣G∣).

[F3]

For a finite-dimensional semisimple C-algebra A and a semisimple finite-dimensional A-module M≅⨁iVi⊕mi over pairwise non-isomorphic simples, E=End⁡A(M) is semisimple with E≅∏iM⁡mi(C), and its simple modules are the spaces Hom⁡A(Vi,M) of dimension mi (Constituent multiplicities are dimensions of simple modules over the endomorphism algebra).

[F4]

A nonzero semisimple finite-dimensional C-algebra is isomorphic to a product of matrix algebras, with simple modules the natural column modules of the factors (The trace form detects semisimplicity over the complex numbers).

[F5]

The simple C[Sm]-modules are the Specht modules Sλ, λ⊢m, pairwise non-isomorphic, and dim⁡CSλ=fλ is the number of standard λ-tableaux (Specht modules classify the complex irreducibles of Sn, The hook length formula).

Proof

technique · direct
1.1F1F2F3

By [F2] the module I(χ) is a semisimple C[G]-module, so [F3] applies to it with A=C[G] and M=I(χ): the constituents Vi of I(χ) are in bijection with the simple E-modules Hom⁡G(Vi,I(χ)), and the multiplicity of Vi equals the dimension of that simple E-module. By [F1] we have E≅⨂rHq(Snr) and, through the Tits isomorphism, E≅C[Wχ]=⨂rC[Snr].

2.1F4F5step 1.1algebra

By [F4] each factor is a product of matrix algebras, C[Snr]≅∏iM⁡di(r)(C), with simple modules the column modules of dimensions di(r); by [F5] these simple modules are exactly the Specht modules Sλ(r), λ(r)⊢nr, of dimension fλ(r). For matrix algebras there is an algebra isomorphism M⁡a(C)⊗M⁡b(C)≅M⁡ab(C) sending the matrix units Eij⊗Fkl to the matrix units indexed by the pairs (i,k),(j,l), which is multiplicative because the products of pairs multiply componentwise; tensoring over the factors therefore gives ⨂rC[Snr]≅∏(λ(1),…,λ(k))M⁡∏rfλ(r)(C), with the simple module of the tuple (λ(1),…,λ(k)) being the external tensor product Sλ(1)⊠⋯⊠Sλ(k) of dimension ∏rfλ(r).

3.1F3step 2.1algebra

Transporting the simple E-modules of step 2.1 along the isomorphism E≅C[Wχ] and applying the parametrisation of step 1.1, the constituents of I(χ) are indexed by the tuples (λ(1),…,λ(k)), and the constituent attached to a tuple has multiplicity ∏rfλ(r); by [F3] the endomorphism algebra is ∏(λ(1),…,λ(k))M⁡∏rfλ(r)(C), as displayed. If χ is regular then every nr=1 and the only partition of each nr=1 is (1), with f(1)=1, so the tuple index set has one element and its multiplicity is 1: I(χ) is irreducible. If χ is trivial then k=1, n1=n, and the formula is the spherical multiplicity formula of The constituents of the spherical principal series of GL_n.

4.1F1F3step 1.1step 2.1step 3.1∎

Steps 1.1, 2.1 and 3.1 give the index set, the multiplicities, the endomorphism algebra and the two boundary cases. AC is carried only from the Tits-deformation supplier inside [F1], as declared; all remaining arguments are finite-dimensional over C.

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