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A fixed singular Verma chain with globally generated final bundle

Statement

Assume the complex flag-variety setup, including the Axiom of Choice, of Flag-variety twisted differential operators and their modules. Let κ be antidominant, put Φκ={β∈Φ:⟨κ,β∨⟩=0},J=Δ∩Φκ, and assume J is a simple system for the full zero-root subsystem Φκ. Choose a reduced expression wJ=sαN⋯sα1 for the longest element of WJ. Set μ0=ρ, μj=sαjμj−1, and Hj=M(−κ−ρ+μj),Ej=Eκ+ρB(Hj), using the exact twisted associated-bundle functor in Exact twisted associated bundles and simple-parabolic descent. The rational B-action has highest-vector weight μj. Then there are embeddings HN⊆⋯⊆H0,EN⊆⋯⊆E0=Dκ⊗OXOX(ρ). For each j, a coherent module Nj over Dκ−ραj satisfies Ej−1/Ej≅OX(ρ)⊗pαj†Nj. Furthermore EN is generated as a Dκ-module by finitely many global sections: for a finite-dimensional rational irreducible G-module V of highest weight ρ there is a surjection Dκ⊗CV↠EN, with horizontal constant V-factor. The sequence of roots depends only on the chosen reduced expression in WJ, not on any later module to which the chain is applied. When J is empty, N=0 and the same assertions hold with HN=H0.

Facts & Assumptions

Given: Complex antidominant κ, the full zero-subsystem condition, the chosen reduced expression, and the objects defined in the statement.

[F1]

Finite Weyl groups have closed-chamber stabilizers generated by the perpendicular roots; reduced expressions have positive prefix roots and longest elements reverse all positive roots (Finite Weyl closed chambers and stabilizers, Finite Weyl positive roots and simple reflections, Finite Weyl strong exchange and deletion).

[F2]

Complex antidominance implies κ−wκ∉Q+∖{0} for every w∈W (Complex-weight separation of Harish-Chandra characters).

[F3]

V exists as a rational G-module by The Borel-Weil theorem; its weights are W-invariant, lie below ρ, and every extremal weight wρ has multiplicity one (Extremal Weyl-orbit weights). The Borel–Weil convention there uses the line with character −ρ; its section module has highest weight −w0ρ=ρ.

[F4]

PBW gives exact induction from b and identifies Verma modules with negative-root monomials. The central character of M(λ) is χλ+ρ, and two such shifted characters coincide exactly on a Weyl orbit (Verma modules, PBW gives an ordered monomial basis for the enveloping algebra, Harish-Chandra isomorphism for the center).

[F5]

The exact associated-bundle functor, its PBW identification, the finite-G tensor identity with horizontal constant factor, and its partial-parabolic descent are proved in Exact twisted associated bundles and simple-parabolic descent.

[F6]

Positive root subgroups, their product factorization, and the minimal-parabolic root subgroup are those of Borel, opposite unipotent groups and root coordinates and Minimal parabolic from one negative simple root. Finite-dimensional sl2 modules of highest weight m−1 integrate to their polynomial SL2 representations (Finite-dimensional representations of sl_2).

[F7]

The enveloping algebra has primitive coproduct Δ(A)=A⊗1+1⊗A and antipode S(A)=−A, with both antipode convolution identities proved on all words (Hopf-algebra structure on U(g)).

Proof

1.1F1givenalgebra

Write κ=a+ib in the real root space. Choose a real number t outside the following finite exceptional set: for each root, exclude a value making ⟨a+tb,β∨⟩=0 unless both pairings already vanish; for each Weyl element, exclude a value making w(a+tb)=a+tb unless wa=a and wb=b. Each nonidentical linear equation excludes at most one value. Then the real vector c=a+tb has stabilizer Wc=Wa∩Wb=Wκ, and its perpendicular roots are exactly Φκ. The real closed-chamber stabilizer theorem [F1] therefore identifies Wκ with the group generated by these root reflections. The assumed simple system gives Wκ=WJ. Reduced-word positivity in [F1] gives mj=⟨μj−1,αj∨⟩∈Z>0: the inverse prefix sends αj to a positive root. For completeness, si permutes the positive roots other than αi, so siρ=ρ−αi and ⟨ρ,αi∨⟩=1. Each positive coroot is a nonzero nonnegative integral sum of simple coroots (apply the positive-root statement to the dual root system), giving the asserted positive integral pairing. The final μN=wJρ pairs strictly negatively with every positive coroot of Φκ.

2.1F4step 1.1algebra

Choose root generators eα,fα,hα with [eα,fα]=hα. In Hj−1 its highest vector v has αj-weight mj−1, because ⟨κ,αj∨⟩=0 and ⟨ρ,αj∨⟩=1. The identity eαfαmv=m(a−m+1)fαm−1v for a highest vector of weight a, proved by commuting eα past the m factors, shows that fαjmjv is killed by eαj. Every other simple positive generator commutes with fαj and kills v. Thus this is a highest vector of weight −κ−ρ+μj, defining Hj→Hj−1. On the negative-root PBW model it is multiplication on the right by fαjmj. The associated graded is multiplication by a nonzero monomial in the polynomial algebra S(n−), hence injective; taking the highest nonzero degree proves injectivity of the original map. Twisting the rational highest weight adds κ+ρ, so the same map is B-equivariant. This gives the fixed chain.

2.2F3step 1.1algebra

In the highest-weight module V of [F3] put V′=⨁μN−ξ∉Q+Vξ,V′′=V/V′. This is a B-submodule: raising a weight outside the downset of μN cannot enter that downset, since subtracting a positive root from an element of Q+ stays incompatible with the assumed outside condition in the reverse direction. More explicitly, if μN−(ξ+β)∈Q+ for β>0, then μN−ξ∈Q+, a contradiction. All weights of V′′ satisfy μN−ξ∈Q+. Its one-dimensional extremal weight line VμN is a B-submodule because raising it leaves this downset.

3.1F4F6step 2.1algebra

Put α=αj, m=mj and Cj=Hj−1/Hj. Let uα− be the sum of negative root spaces other than g−α. It is a Lie subalgebra stable under the α-Levi. Ordering its basis before fα in PBW gives Cj≅U(uα−)⊗span⁡(v,fαv,…,fαm−1v). Indeed im⁡Hj has exactly the basis with final fα exponent at least m. The last factor is the m-dimensional simple α-module. Positive root spaces other than gα kill this factor: commute them past powers of fα; all resulting roots stay positive and different from α, or vanish. Therefore this basis identifies Cj with the parabolic induction from that finite-dimensional pα-module. In particular π(eα) and π(fα) are locally nilpotent on Cj: the adjoint α-action on each finite PBW degree of U(uα−) is locally finite, and its tensor with the last factor is a sum of finite-dimensional sl2 modules.

3.2F1F2F3F4step 1.1step 2.2algebra

Suppose a weight ξ of V′′ has χ−κ+ξ=χ−κ+μN. By [F4] and the W-invariance of the sign change, κ−ξ∈W(κ−μN)=W(κ−ρ), where the last equality uses wJκ=κ. Choose w with w(κ−ξ)=κ−ρ. Then κ−wκ=ρ−wξ∈Q+, since wξ is a weight of V and lies below ρ by [F3]. By [F2] the difference is zero, so wκ=κ and w∈Wκ=WJ. Thus ξ=w−1ρ∈WJμN. For a strictly antidominant weight μN in this subsystem, vμN−μN∈Q+ for every v∈WJ: telescope a reduced word, whose simple-root pairings with μN are negative and whose prefix roots are positive by [F1]. Consequently ξ−μN∈Q+, whereas μN−ξ∈Q+ by step 2.2. The pointed root cone forces ξ=μN. Thus all other weights of V′′ have central characters different from the distinguished one. This is separation for arbitrary complex antidominant κ, using no real-chamber restriction.

4.1F4F6step 3.1algebra

Remove the integral character ρ from the rational B-action on Cj. Its infinitesimal action becomes π+κ, and all torus weights are integral, beginning with μj−1−ρ. This action extends to a rational Pα-action. Explicitly keep the torus weight action and the existing positive root groups, and define the additional negative root group by x−α(t)=exp⁡(tπ(fα)). This exponential is a finite sum on each vector by step 3.1. On finite PBW-degree subspaces, the Levi SL2 relations hold by [F6]; the torus action agrees because its α-weight is that of π, as κ(hα)=0. The other torus characters are integral and hence rational. The non-Levi positive nilradical acts locally nilpotently and its conjugation relations with the Levi follow by exponentiating the Lie brackets; the finite Baker–Campbell–Hausdorff sums agree with its root-group factorization [F6]. These actions are locally finite: commuting a positive non-Levi root generator through a PBW word never increases its uα− degree, and the Levi preserves that degree. Each bounded-degree tensor the last finite factor is finite-dimensional and stable under pα. Hence all the displayed matrix coefficients are regular and glue to the rational parabolic action. Covariance with π(g) follows on the root generators by the same bracket/exponential calculation. This is a twisted (g,Pα)-module of twist κ.

4.2F4step 2.2step 3.2algebra

Induce C−κ−ρ⊗V′′ from b. By exactness of induction, its distinguished weight line induces the submodule HN. The quotient has a finite Verma filtration with one factor M(−κ−ρ+ξ) for each other weight, counted with multiplicity: order the finitely many weight spaces from higher to lower and refine within each torus weight space; the positive nilradical raises weights and the torus acts diagonally. Choose a central element z whose value c0 on the distinguished character differs from its values ci on all the other characters. Such z exists: each forbidden equality is a proper linear hyperplane in the center, and a finite union of proper linear subspaces cannot cover a complex vector space (restrict to the finite span of elements individually separating the finitely many pairs). Let g(t)=∏i(t−ci) with repetition along the quotient filtration. The product g(z) annihilates that quotient, because each factor kills its corresponding successive Verma factor; all factors commute. On HN it is the nonzero scalar g(c0). Therefore g(z)/g(c0) maps the induced module onto HN and is the identity on HN, giving a projection. It intertwines the rational twisted B-action because z is invariant under the adjoint action of connected B. This is an actual module projection; no OX-linearity is asserted for central operators on arbitrary differential modules.

5.1F4F5step 4.1algebra

Apply [F5] to the exact chain in step 2.1. The PBW identity gives E0=Dκ⊗OX(ρ). Descent of step 4.1 gives Ej−1/Ej=OX(ρ)⊗pα†Nj, with Nj=EκPα(Cj). These modules are coherent: E0 is locally a rank-one free differential module, and the PBW filtered-noetherian argument makes its differential submodules Ej and quotients coherent. Locally the quotient has the form O(−1)⊠Nj; finite differential generators on the two affine fiber charts involve finitely many coefficients in Nj. Their base-differential span must be Nj, since vertical differentiation creates no new coefficients. The partial TDO is locally noetherian by the same PBW argument, so Nj is coherent.

6.1F4F5F7step 4.2algebra∎

Composing induction of V↠V′′ with the projection of step 4.2 gives a surjection of twisted modules M(−κ−ρ)⊗V↠HN. Here the tensor identity is the map u⊗(c⊗v)↦∑(u(1)⊗c)⊗u(2)v, with inverse obtained by inserting the antipode in the second enveloping factor. The coproduct and antipode from [F7] check on generators that both maps respect the b relations, are mutual inverses, and commute with the twisted rational B-actions. Apply the exact functor [F5]. Its PBW and tensor identities give Dκ⊗CV↠EN with differential action only on Dκ. The sections 1⊗vi for a finite basis of V are global differential generators. This proves finite global generation and completes all chain assertions, including the empty-word case. Choice enters through the inherited highest-weight and Weyl suppliers and the permitted bases.

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