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Beilinson–Bernstein Localization and Category O

1 · Prerequisites

2 · Summary

The weight parameter is complex; antidominance excludes positive integral positive-coroot pairings. The TDO has isotropy character κ+ρ, so D−ρ is ordinary differential operators. Global TDO sections are the exact central quotient for every parameter. Global sections is exact for antidominant parameters and gives the regular antidominant equivalence, including coherent modules. At singular antidominant parameters the proved replacement is the Serre quotient and the complete simple-parabolic kernel filtration under the stated full zero-subsystem condition.

Companion: beilinson-bernstein-localization-and-category-o-examples.

Reading context: category-o-klr-and-hecke-categorification-route. Its exact Category O conventions are compatible with the published BGG suppliers used here; no KLR or Hecke categorification theorem is a localization premise.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Flag-variety twisted differential operators and their modules

Definition

Assume the Axiom of Choice as inherited from the published group and sheaf suppliers. Let G be a connected simply connected complex semisimple affine algebraic group, B⊇T a Borel subgroup and maximal torus, X=G/B, g=Lie⁡G, h=Lie⁡T, and Φ+ the positive roots selected by B. Write ρ=12∑α∈Φ+α. All schemes are over C. For an integral weight η, OX(η) denotes the G-equivariant line bundle G×BCη with fiber character η at eB.

The infinitesimal G-action gives an anchor aX:LX:=OX⊗Cg⟶TX,f⊗x⟼fxX. Give LX the action-algebroid bracket [f⊗x,g⊗y]=fg⊗[x,y]+fxX(g)⊗y−gyX(f)⊗x. Its kernel bX=ker⁡aX is the isotropy Lie-algebra bundle; at gB its fiber is Ad⁡(g)b.

For any κ∈h∗, the character κ+ρ of b (zero on n+) transports to an OX-linear map χκ+ρX:bX→OX. The transport is independent of the representative g of gB, since a character is invariant under the adjoint action of B. The action-algebroid enveloping sheaf UX(g) is generated by OX and LX with the displayed bracket and [x,f]=xX(f),x∈LX, f∈OX. Define the sheaf of twisted differential operators Dκ:=UX(g)/(ξ−χκ+ρX(ξ):ξ∈bX). Its order filtration assigns order zero to OX and order at most one to the image of LX. A TDO means a filtered OX-ring with F0=OX, associated graded Sym⁡OXTX, and first-order commutator equal to the anchor; the well-definedness and PBW properties of Dκ are proved in PBW and integral line-bundle twisting for flag TDOs ↗. A left Dκ-module below is required to be quasi-coherent as an OX-module.

For z∈Z(U(g)), let pr⁡(z)∈U(h) be the Harish–Chandra projection along the chosen triangular decomposition, and put χκ(z)=pr⁡(z)(κ−ρ). This is the shifted central character: the Harish–Chandra isomorphism makes it W-invariant in κ. Define Aκ=U(g)/U(g)ker⁡χκ. The regularity convention is antidominant when ⟨κ,α∨⟩∉Z>0 for each positive root α, and regular when ⟨κ,α∨⟩≠0 for every root. For complex weights, Z>0 means the positive real integers; no order on arbitrary complex numbers is used.

Remarks

For integral κ, the proved identification is Dκ=Diff⁡(OX(κ+ρ)). In particular D−ρ=Diff⁡(OX). The construction uses the isotropy sheaf bX; quotienting U(g) by the fixed subalgebra b would not define an algebra. With the convention of The equivariant line bundle associated to a Borel character, OX(η)=L−η.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passOpen item page →

Complex-weight separation of Harish-Chandra characters

Statement

Let E be the real span of a finite reduced crystallographic root system Φ, with chosen positive roots Φ+, simple roots Δ={α1,…,αr}, Weyl group W and root lattice Q=∑iZαi. Extend the pairing complex linearly to EC. For κ∈EC, call κ antidominant if ⟨κ,α∨⟩∉Z>0 for every α∈Φ+, and regular if ⟨κ,α∨⟩≠0 for every root. Then κ−wκ∉Q+∖{0}(w∈W) for antidominant κ, and κ−wκ∉Q+(w≠1) when κ is also regular. Here Q+=∑iZ≥0αi.

Facts & Assumptions

Given: A finite reduced crystallographic root system, a positive system, its Weyl group and root lattice, and a complex weight κ=a+ib with a,b∈E.

[F1]

The simple roots form a basis of E and of Q over Z; positive roots have nonnegative simple-root coordinates, and the positive and negative root cones meet only at zero (Finite Weyl root system, lattice and chamber conventions, Finite Weyl positive roots and simple reflections).

[F2]

Move b by an element of W into the closed positive chamber and let I={i:(b,αi)=0}. Its stabilizer is the parabolic Weyl group WI generated by the reflections si with i∈I. The root subsystem ΦI generated by these simple roots has root lattice QI=∑i∈IZαi and span EI=span⁡R{αi:i∈I}. Then Q∩span⁡R{αi:i∈I}=∑i∈IZαi, because the simple roots are a Z-basis of Q. Every root of ΦI is perpendicular to b. These conclusions follow from Finite Weyl closed chambers and stabilizers and the simple-root basis.

[F3]

For the dual root system, the affine Weyl group is Q⋊W acting by translations and finite Weyl transformations. Its alcoves are simply transitive under this action, and the affine walls have equations ⟨x,α∨⟩=m with m∈Z (Coroot and dual root system, Root, coroot, weight, and coweight lattices, Alcove transitivity, the affine Coxeter presentation, and the length function).

[F4]

In a finite crystallographic root system, a reduced word w=si1⋯sim has positive prefix roots si1⋯sij−1αij for every j (Finite Weyl strong exchange and deletion, Finite Weyl positive roots and simple reflections).

Proof

1.1F1F2F3given

Suppose q=κ−wκ∈Q. Since q is real, b=wb, so w∈Wb. Move b into the closed positive chamber and conjugate a,b,κ,w,q by the same Weyl element; lattice membership is preserved. With I and EI as in [F2], w∈WI, and each generator of WI fixes EI⊥. Therefore a−wa∈EI; since q=a−wa∈Q, [F2] gives q∈QI=Q∩EI. The affine transformation tqw of the affine Weyl group QI⋊WI of the dual subsystem ΦI∨ fixes the orthogonal projection aI of a to EI.

2.1F2F3step 1.1construct

In any locally finite affine root-wall arrangement, the stabilizer of a point aI is generated by the reflections in walls through that point. To see this, choose a ball about aI meeting no wall not containing aI. Inside it, the finitely many hyperplanes through aI cut local chambers; generic line segments join any two local chambers by crossing one wall at a time and avoiding their codimension-two intersections. The corresponding wall reflections therefore act transitively on the local chambers. If an affine Weyl element fixes aI, choose a local chamber C and a product h of these reflections carrying C to its image. Then h−1g preserves the global alcove containing C, so it is the identity by the simple transitivity in [F3]. Hence g=h. Apply this to g=tqw from [step 1.1] in the arrangement for the dual subsystem ΦI∨. Every generating wall has a root α∈ΦI and ⟨a,α∨⟩∈Z; because α is in ΦI, [F2] gives ⟨b,α∨⟩=0, so ⟨κ,α∨⟩∈Z. Taking finite parts shows that w belongs to the subgroup Wint generated by the reflections sα for roots with integral κ-pairing. Undo now the temporary Weyl conjugation of step 1.1: if that conjugating element was u, a generating root α in the conjugated coordinates returns to u−1α, and ⟨uκ,α∨⟩=⟨κ,(u−1α)∨⟩. Thus the original w lies in the integral-root reflection subgroup for the original κ. From this point on κ,w,q,Φ+ and Q+ refer to the original data. No preservation of antidominance or of the positive cone by u is assumed.

3.1F1F4step 2.1algebra

The set Φint={α∈Φ:⟨κ,α∨⟩∈Z} is stable under its root reflections: if m=⟨κ,α∨⟩∈Z and β∈Φint, then ⟨κ,(sαβ)∨⟩=⟨sακ,β∨⟩=⟨κ,β∨⟩−m⟨α,β∨⟩∈Z, using crystallographic integrality. It is therefore a finite root system in its span, with positive system Φint∩Φ+ and its own simple roots Δint. For every δ∈Δint, antidominance makes the integer ⟨κ,δ∨⟩ nonpositive. If w=sδ1⋯sδm is reduced in Wint, telescoping gives κ−wκ=∑j=1m⟨κ,δj∨⟩sδ1⋯sδj−1δj. Every prefix root is positive in Φint by [F4], hence is positive in the ambient system; every term lies in −Q+. Thus q∈−Q+. If κ is regular, every integral pairing here is nonzero, so every coefficient is strictly negative.

4.1F1step 1.1step 3.1algebra∎

Combining [step 1.1] and [step 3.1], an assumed q∈Q+∖{0} also lies in −Q+, contradicting [F1]. This proves the antidominant assertion. If κ is regular, every integral root pairing in [step 3.1] is strictly negative. For any nonidentity w∈Wint, its reduced word has at least one term, and each term is a strictly negative integer multiple of a positive root; the sum is nonzero because Q+ is pointed. Hence q=0 forces w=1, proving the regular assertion.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passOpen item page →

Global sections on module sheaves have ordinary sheaf cohomology as derived functors

Statement

Assume the Axiom of Choice. Let (X,A) be a topological space with a sheaf of unital rings (not necessarily commutative), and let Mod⁡(A) be the category of sheaves of left A-modules. Then this category has enough injectives, every injective A-module sheaf is flasque as an underlying sheaf of abelian groups, and for every A-module sheaf M the right-derived functors of global sections in Mod⁡(A) satisfy RqΓMod⁡(A)(X,M)≅Hq(X,M)(q≥0), where the right side is ordinary sheaf cohomology of the underlying abelian sheaf.

Facts & Assumptions

Given: Axiom of Choice, a topological space X, a sheaf of unital rings A, and a sheaf M of left A-modules.

[F1]

For every unital ring R, every left R-module embeds in an injective left R-module (Module categories have enough injectives).

[F2]

Stalks are exact, and the stalk (Ax,Mx) is a ring-module pair (Modules on a ringed space, A sequence of abelian sheaves is exact exactly when it is exact on every stalk).

[F3]

For an open inclusion j:U↪X, extension by zero of an A∣U-module is defined by the same support condition as for abelian sheaves; restricting the A-action makes it an A-module, and its stalks are Mx on U and zero off U. The abelian-sheaf adjunction restricts to module morphisms, and stalkwise exactness makes this extension exact. The construction is proved in step 1.2 using Extension by zero for abelian sheaves on an open subspace, Extension by zero is left adjoint to restriction and is exact on abelian sheaves and A sequence of abelian sheaves is exact exactly when it is exact on every stalk.

[F4]

Flasque sheaves of abelian groups are acyclic for global sections (Flasque abelian sheaves are Γ-acyclic).

[F5]

Relative to a supplied injective resolution datum on a class D, the acyclic-resolution theorem applies when the resolved object, all resolution terms, and all cycles lie in D (An F-acyclic resolution, The acyclic-resolution theorem for right derived functors). For ordinary sheaf cohomology the datum is the one fixed on all of Ab(X) in Sheaf cohomology as right derived global sections.

Proof

1.1F1F2givenchoose

For each point x∈X, choose an embedding Mx↪Ix into an injective Ax-module by [F1]. The skyscraper sheaf ix∗Ix has sections Ix on opens containing x and zero on opens not containing x, with A(U) acting through Ax. The natural bijection Hom⁡A(N,ix∗Ix)≅Hom⁡Ax(Nx,Ix) shows ix∗Ix is injective, since taking stalks is exact by [F2]. The product of these injectives is injective: Hom into the product is the product of Hom functors, and products of exact sequences of abelian groups are exact under the stated Axiom of Choice. The diagonal map M→∏x∈Xix∗Ix is injective on each stalk by construction. Thus Mod⁡(A) has enough injectives.

1.2F2F3construct

Let j:U↪X be open and M an A∣U-module. Define (j!M)(V) as the sections of M(V∩U) whose support is closed in V, using Extension by zero for abelian sheaves on an open subspace. For a∈A(V) and such a section s, let as be the action of a∣V∩U; if s vanishes on W∩U near a point of V∖U, then so does as, so the support condition is preserved. The stalks are Mx for x∈U and zero otherwise by the underlying abelian construction. The abelian-sheaf adjunction extends a module map on U uniquely to an abelian-sheaf map on X; the extension is A-linear on stalks in U by the original module-linearity and off U because its source stalk is zero. Thus j! is left adjoint to restriction in module sheaves. The stalk description and [F2] show that it is exact.

2.1F2F3step 1.1step 1.2construct

Let I be an injective A-module sheaf and let U⊆V be open. A section s∈I(U) corresponds by evaluation at 1 to a morphism j!AU→I∣V. The natural map j!AU→AV is a monomorphism: on stalks it is the identity for points of U and the map 0→Ax outside U. Restriction preserves injectivity here because its exact left adjoint is extension by zero [F3, step 1.2]. Injectivity of I∣V extends the morphism across j!AU↪AV. The extension is determined by the image t of 1∈A(V), and t∣U=s. Every restriction I(V)→I(U) is therefore surjective, so I is flasque.

3.1F2F4F5givenstep 1.1step 2.1∎

Take an injective resolution 0→M→I0→I1→⋯ in Mod⁡(A), which exists by step 1.1. Its global-sections complex computes module-derived global sections by definition. Each underlying abelian sheaf Ip is flasque by step 2.1 and hence Γ-acyclic by [F4]. Use the supplied abelian-sheaf datum of [F5], whose domain is all of Ab(X): the underlying M, every Ip, and every cycle are abelian sheaves and therefore belong to that domain. Forgetting the module action preserves exactness by [F2], so this is a Γ-acyclic resolution relative to that datum. The acyclic-resolution theorem now identifies its global-sections cohomology with Hq(X,M); its Dependent Choice hypothesis follows from the assumed AC. Comparison of resolutions makes the identification natural in M, and it preserves degree zero.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passOpen item page →

Cech cohomology of line bundles on the projective line

Statement

Assume the Axiom of Choice, inherited from sheaf cohomology.

For d∈Z, let OP1(d) have standard frames e0,e1 on U0={x≠0} and U1={y≠0} with e1=zde0 on the overlap, where z=y/x and w=1/z. Then dim⁡H0(P1,O(d))=max⁡(d+1,0),dim⁡H1(P1,O(d))=max⁡(−d−1,0), and Hq=0 for q≥2. For d≥0, restrictions to U0 of global sections on P1, written in the frame e0, are precisely the polynomials of degree at most d; for d≤−2, H1 has Laurent basis zd+1,zd+2,…,z−1.

Facts & Assumptions

Given: The Axiom of Choice (The Axiom of Choice), P1 with the two standard affine charts, an integer d, the line-bundle transition e1=zde0, and sheaf cohomology with the supplied injective resolution datum.

[F1]

Under the assumed Axiom of Choice inherited from the definition of sheaf cohomology, the two-chart affine cover computes cohomology of a quasi-coherent sheaf on the separated scheme P1 (Cech cohomology computes quasi-coherent cohomology on a separated scheme).

[F2]

The sheaf O(d) is invertible, hence quasi-coherent, with the standard transition rule (Invertible sheaves).

Proof

1.1F1F2givenalgebra

The Cech complex for U0,U1 has C0=C[z]e0⊕C[w]e1,C1=C[z,z−1]e0, with differential (f0,f1)↦zdf1(1/z)−f0(z). Its kernel consists of polynomials f0(z) that also lie in zdC[z−1]. If d≥0, these are exactly the span of 1,z,…,zd; if d<0, the exponent ranges {0,1,…} and {d,d−1,…} are disjoint, so the kernel is zero. This proves the assertion for H0.

2.1F1step 1.1algebra∎

The degree-one cohomology is the Laurent-polynomial quotient C[z,z−1]/(C[z]+zdC[z−1]). The first summand spans exponents n≥0 and the second spans n≤d. If d≥−1, these ranges cover every integer, so the quotient is zero. If d≤−2, the missing exponents are exactly d+1,d+2,…,−1, which gives the stated basis and dimension −d−1. The Cech complex has no degree above one, so Hq=0 for q≥2.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passOpen item page →

The principal nilpotent Borel orbit by height elimination

Statement

Assume the Axiom of Choice and the setup of Complex semisimple algebraic group, Borel, and flag variety. For each simple root αi choose a nonzero root vector ei∈gαi and put e=∑iei. Write nj+=⨁ht⁡(α)=jgα. Then B⋅e={∑α∈Φ+cαeα∈n+:cαi≠0 for every simple root αi}, where one nonzero eα∈gα is fixed for each positive root. The right side is independent of the choices of those root vectors.

Facts & Assumptions

Given: A connected simply connected complex semisimple group G, Borel B=T⋉U, its positive root system, and nonzero simple-root vectors ei.

[F1]

The proof of The nilpotent central fiber is reduced and integral, step 1.2, constructs e=∑iei in a principal sl2 triple; the adjoint representation is a direct sum of strings of even highest weights 2mj>0, and ker⁡ad⁡e has dimension rank⁡G.

[F2]

B=T⋉U, U=exp⁡(n+), the positive root spaces are one-dimensional, and the simple roots form a basis of the root lattice (Complex semisimple algebraic group, Borel, and flag variety, Borel, opposite unipotent groups and root coordinates).

Proof

1.1F1F2algebra

On a principal sl2 string with highest weight 2m>0, ad⁡h has weights −2m,−2m+2,…,2m. For every j≥1, if weight 2j occurs then weight 2j−2 occurs, and the raising operator ad⁡e maps the latter one-dimensional weight space onto the former. Summing over the strings in [F1] gives [e,nj+]=nj+1+(j≥1), with zero spaces understood above the maximal root height.

2.1F1F2step 1.1chooseconstruct

Let x∈n+ have nonzero simple coefficients. The map T→(C×)r, t↦(αi(t))i, is an isogeny: its character-lattice map has image the full-rank root lattice. An isogeny of complex tori is surjective on complex points, so conjugation by one t∈T sets all simple coefficients of x to 1. Now suppose heights below j+1 already agree with those of e. Their height-(j+1) difference lies in nj+1+; by [step 1.1] choose uj∈nj+ whose bracket with e cancels that difference. The finite exponential exp⁡(ad⁡uj) changes no height at most j and changes height j+1 by [uj,e]; all its higher commutators have height at least j+2. Induction over the finitely many root heights conjugates x to e by U.

3.1F2step 2.1algebra∎

Conversely, conjugation by T scales each simple-root coefficient by a nonzero scalar. For u∈U, every commutator in exp⁡(ad⁡u)e−e has height at least two, because u has positive height and e has height one. Thus U fixes the simple-root coefficients, and B=TU preserves their nonvanishing. The inclusion in the right side and the reverse inclusion from step 2.1 prove the equality. The rank-zero case has n+=0, e=0 and both sides are the singleton {0}.

LemmaStatement: Literature-sourcedProof: AI-adaptedprecheck passOpen item page →

Quasicoherent modules are filtered unions of coherent subsheaves and cohomology commutes with these colimits

Statement

Assume the Axiom of Choice. Let X=G/B be the projective flag variety of Complex semisimple algebraic group, Borel, and flag variety, and let M be a quasi-coherent OX-module. Then M is the filtered union of its coherent OX-submodules. If M=lim→⁡jFj is any filtered colimit of quasi-coherent modules, then for every q≥0 the canonical map lim→⁡jHq(X,Fj)⟶Hq(X,M) is an isomorphism.

Facts & Assumptions

Given: The Axiom of Choice, the projective flag variety X, a quasi-coherent module M, and, for the second assertion, a filtered diagram Fj in QCoh⁡(X) with colimit M.

[F1]

X is a Noetherian, quasi-compact separated scheme; its highest-weight orbit construction embeds it as a closed subvariety of a projective space, so the restricted O(1) is very ample and its standard opens give a finite affine cover (A semisimple flag variety is smooth and projective, Projective orbit constructions for G/B and G/P_alpha, Relative very ampleness in the finite projective-space convention).

[F2]

On an affine open Spec⁡A, quasi-coherent modules are associated sheaves of A-modules; sections commute with filtered colimits under this equivalence (Affine quasi-coherent sheaves are modules, Quasi-coherent module on a scheme).

[F3]

On a locally Noetherian scheme, a quasi-coherent module of finite type is coherent (Coherent sheaves on a locally Noetherian scheme, Coherent module sheaves, Locally Noetherian and Noetherian schemes).

[F4]

The finite affine cover in [F1] computes quasi-coherent cohomology by its ordered Cech complex (Cech cohomology computes quasi-coherent cohomology on a separated scheme).

[F5]

Filtered colimits of abelian groups are exact and commute with the cohomology of a cochain complex (Filtered colimits of abelian groups are exact).

Proof

1.1F1F2chooseconstruct

Choose a very ample embedding X↪PN and its standard affine cover Ui=X∩D+(xi). For a section s∈Γ(Ui,M), each overlap Ui∩Uj is the principal open D(xi/xj) in the affine Uj. By [F2] write s∣Ui∩Uj=mj/(xi/xj)rj for some mj∈Γ(Uj,M). There are finitely many j, so choose a common r≥rj and replace each numerator mj by (xi/xj)r−rjmj, so its denominator is now (xi/xj)r. With xj as the frame of L=OX(1) on Uj, the section mj⊗xjr of M⊗Lr extends s⊗xir from Ui∩Uj to Uj. On an overlap Uj∩Uk, the two extensions agree after inverting xi, because both restrict to s⊗xir there. Their difference is therefore killed by some power of xi in the quasi-coherent module of sections on that affine overlap. There are finitely many overlaps, so one further common power kills all differences; multiplying every local extension by that power of xi makes them agree and they glue to a global section of M⊗Ln whose restriction to Ui is s⊗xin. Thus each local section on a standard chart is locally in the image of a global map L−n→M.

2.1F1F3step 1.1construct

Take the direct sum of the maps L−n→M produced by [step 1.1] for all standard charts and all their local sections. At every stalk this map is surjective because the standard charts cover X and their sections generate the associated modules. Hence M is the union of the images of finite subsums: the indexing set of finite subsums is filtered, their transition maps are inclusions, and their colimit is the image of the surjection. Each finite subsum is a finite direct sum of invertible sheaves, so its image is a finite-type quasi-coherent submodule of M; it is coherent by [F3]. This proves the first assertion.

3.1F1F2F4F5∎

Fix the finite affine cover from [F1]. Every finite intersection is affine, and [F2] identifies sections on it with module sections; these sections commute with the filtered colimit. Therefore the ordered Cech complex of M is the degreewise filtered colimit of the ordered Cech complexes of Fj. The cover computes sheaf cohomology by [F4], and exactness of filtered colimits in [F5] gives Hq(X,M)=Hq(lim→⁡jC∙(U,Fj))≅lim→⁡jHq(C∙(U,Fj))≅lim→⁡jHq(X,Fj) for every q≥0. The finite cover and degreewise finite sums are essential; no interchange with an infinite product is used.

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PBW and integral line-bundle twisting for flag TDOs

Statement

Use X, g, bX, and Dκ from Flag-variety twisted differential operators and their modules. For every κ∈h∗ the isotropy relations generate a two-sided ideal and define a TDO satisfying F0Dκ=OX,gr⁡Dκ≅Sym⁡OXTX. If η∈X∗(T) is integral, then Dκ≅Diff⁡(OX(κ+ρ))(κ+ρ integral),D−ρ=Diff⁡(OX), and tensoring by OX(η) defines an equivalence between left Dκ-modules and left Dκ+η-modules.

Facts & Assumptions

Given: The connected simply connected complex semisimple group G, its flag variety X=G/B, and a complex weight κ; for the line-bundle claims, an integral weight η.

[F1]

X is smooth and projective and G→X has Zariski-local sections; on each such chart the action algebroid is the transitive Lie algebroid OX⊗g with isotropy bX (A semisimple flag variety is smooth and projective, Zariski sections of Borel and minimal-parabolic orbit maps).

[F2]

The bracket and anchor in the action-algebroid definition satisfy the Jacobi, Leibniz and anchor identities because they are induced by the Lie algebra action on functions and vector fields (Flag-variety twisted differential operators and their modules).

[F3]

An integral weight defines the G-equivariant line bundle OX(η), and its infinitesimal G-action on sections has principal symbol the anchor vector field (G-linearizations of invertible sheaves on a complex G-variety, Invertible sheaves).

Proof

1.1F1F2algebraconstruct

Work on a Zariski open set where TX and bX are free and the anchor splits as an OX-module map. Combine tangent lifts x1,…,xd and a frame b1,…,bs of bX into one frame e1,…,en of the full action algebroid, ordered with the tangent lifts first and the isotropy frame last. For every frame generator use the relations eaf=fea+a(ea)(f) and, for b>a, ebea=eaeb+[eb,ea] to move functions left and order all generators; write each bracket in the chosen frame with its local function coefficients. Reordering terminates by lexicographic induction on generator degree, the number of generator/function inversions (a generator to the left of a coefficient), and the inversion count of the frame-generator word. A commutator correction lowers generator degree; the leading function move lowers the second count, and an out-of-order generator swap lowers the third. The only overlap types are ea(fg), ebeaf, and ecebea for arbitrary frame indices, including isotropy indices. Their reductions agree by the derivation rule for the anchor, the anchor identity a([eb,ea])=[a(eb),a(ea)], and Jacobi for the action-algebroid bracket [F2]. A terminating rewriting system with every such overlap resolved has unique normal forms: induction on maximum remaining reduction length joins any two first reductions at their common overlap, after which induction identifies the normal forms. Hence the ordered monomials in all ea, with coefficients on the left, form a local OX-basis, and the indicated ordering puts every tangent-lift monomial before isotropy monomials. Their leading symbols are the corresponding symmetric monomials, proving gr⁡UX(g)≅Sym⁡OX(OX⊗g).

2.1F1F2step 1.1algebraconstruct

On a chart pulled back to G, the isotropy character is the constant B-character κ+ρ. It kills [b,b] and is invariant under B-conjugation; equivariance therefore gives χX([x,ξ])=a(x)(χX(ξ)) for every local algebroid section x and isotropy section ξ. In the ordered forms of step 1.1, use ba=χX(ba) to eliminate each isotropy generator. The overlaps of this elimination with two isotropy generators agree because χX kills their bracket; the overlaps with a tangent lift agree by the displayed invariance identity; and overlaps with functions agree because a(ba)=0. Thus the quotient has the ordered tangent-lift monomials as a local basis, and its associated graded is Sym⁡OX(OX⊗g)/(bX)≅Sym⁡OXTX. The degree-zero part is OX, and the first-order commutator is the anchor inherited from UX(g). This proves the TDO axioms and the two-sidedness of the defining ideal.

3.1F3step 2.1algebra

Suppose κ+ρ is integral and put L=OX(κ+ρ). The infinitesimal G-linearization of L gives a filtered algebra map UX(g)→Diff⁡(L). Its isotropy action on each fiber is the character κ+ρ, so the map kills the ideal in step 2.1 and descends to Dκ→Diff⁡(L). On associated graded it is the identity map Sym⁡TX→Sym⁡TX because both maps send a vector field to its principal symbol. A filtered map with associated-graded isomorphism is an isomorphism: lift any section order by order for surjectivity, and take the leading symbol of a kernel section for injectivity. Thus Dκ≅Diff⁡(L). Taking κ=−ρ gives L=OX and the asserted untwisted identity.

4.1F3step 3.1algebra∎

For integral η, write Lη=OX(η). Locally choose a frame e of Lη. Tensoring a Dκ-module with e identifies its local differential-operator action with the action for the twist κ+η. If e′=ue on an overlap, with u an invertible regular function, the two local actions are related by conjugation D↦u−1Du; this is exactly the transition rule for the TDO parameter shifted by η. These local equivalences glue. Tensoring by L−η reverses the shift and composes with the first functor to the identity.

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Normality of the nilpotent cone and Springer functions

Statement

Assume the setup of Complex semisimple algebraic group, Borel, and flag variety and the Axiom of Choice. Let N⊆g be the nilpotent cone with its reduced coordinate ring from The nilpotent central fiber is reduced and integral, and let μ:T∗X→N be the Springer moment map. Then N is normal, μ is proper and birational, and pullback induces a graded algebra isomorphism C[N]→∼Γ(T∗X,OT∗X).

Facts & Assumptions

Given: A connected simply connected complex semisimple group G with Borel B, flag variety X=G/B, root system Φ, and the reduced nilpotent cone N.

[F1]

The nilpotent cone is irreducible and reduced of dimension 2∣Φ+∣ by The nilpotent central fiber is reduced and integral. Its proof establishes the additional facts used here: step 1.1 proves the complete-intersection and Cohen–Macaulay properties; step 1.2 constructs the principal element e=∑iei and computes dim⁡Zg(e)=rank⁡G; steps 3.2 and 4.2 show that every nilpotent element is conjugate into n+; and steps 6.1 and 7.1 prove full Jacobian rank and regularity at e.

[F2]

The Borel orbit of e consists exactly of the elements of n+ whose simple-root coefficients are nonzero (The principal nilpotent Borel orbit by height elimination).

[F3]

Bruhat decomposition writes every g∈G as b1nwb2 with b1,b2∈B and w∈W; a Weyl element carrying all positive simple roots to positive roots is the identity (Bruhat decomposition for a split reductive group).

[F4]

X is smooth projective, Lie⁡Pαi=b⊕g−αi and X=G/B→G/Pαi is a P1-bundle, so dim⁡G/Pαi=∣Φ+∣−1. The Killing form identifies T∗X≅G×Bn+, and projective morphisms are proper (Minimal parabolic from one negative simple root, A semisimple flag variety is smooth and projective, The Killing form is invariant and nondegenerate on a complex semisimple Lie algebra, A minimal-parabolic flag projection is a projective-line bundle, Projective morphisms are proper).

[F5]

Root-space brackets satisfy [gγ,gβ]⊆gγ+β (Brackets of root spaces), and the positive-root subgroups form the height-ordered unipotent group U (Borel, opposite unipotent groups and root coordinates). The simple roots form a Z-basis of the root lattice and positive roots have nonnegative simple-root coordinates (Simple roots form a signed integral basis); each root space is one-dimensional (Root spaces of a complex semisimple Lie algebra are one-dimensional).

[F6]

A finite-type morphism has constructible image (Chevalley: images of constructible sets are constructible).

[F7]

A complete intersection is S2, and an integral Noetherian scheme regular in codimension one is normal (serre normality criterion).

[F8]

A finite-type morphism with finite scheme-theoretic fibers is quasi-finite; a proper quasi-finite morphism is finite (Finite-fibre and pointwise characterizations of quasi-finiteness, A proper quasi-finite morphism is finite).

[F9]

A finite field extension in characteristic zero is separable, and every finite separable field extension is simple (A finite extension generated by elements all but possibly one of which are separable is simple).

[F10]

Proper pushforward of the structure sheaf is coherent; a finite module algebra over a ring is integral over that ring (Coherent higher direct images under proper morphisms).

Proof

1.1F1F6algebra

The orbit map G→N, g↦Ad⁡(g)e, has irreducible image closure. By [F1] its image has dimension dim⁡g−dim⁡Zg(e)=2∣Φ+∣=dim⁡N; by [F6] the constructible image is dense and therefore contains a nonempty open subset of the irreducible variety N. The orbit is G-stable, so its translates of this open subset cover the orbit; consequently G⋅e is open in N.

1.2F1F4

The Springer map is μ:G×Bn+⟶N,[g,x]⟼Ad⁡(g)x. Its graph is the incidence subvariety {(gB,y)∈X×N:y∈Ad⁡(g)n+}, which is closed because the spaces Ad⁡(g)n+ form a vector subbundle of X×g. The projection X×N→N is projective by [F4], so μ is proper by the projective-morphism theorem included in [F4]. Surjectivity follows from the last clause of [F1].

2.1F1F2F4F5F7step 1.1

If y∈N∖G⋅e, conjugate it into n+ by [F1]. At least one simple-root coefficient must vanish by [F2]. For each simple αi, set ni=⨁β∈Φ+, β≠αigβ. This is a nilpotent Lie subalgebra. It is an ideal in pαi=b⊕g−αi: brackets with h preserve each root space; brackets with positive root spaces have weights β+γ, which if nonzero remain positive and cannot equal αi because β≠αi has a positive coefficient at another simple root; and if β−αi is a root for β≠αi, it must be positive, since otherwise αi would be a sum of positive roots. These assertions use [F5] and the simple-root basis. The exponential/BCH coordinates in [F5] identify exp⁡:n+→U as a polynomial isomorphism, so Ni=exp⁡(ni) is a closed connected unipotent subgroup with Lie algebra ni. Order the positive-root coordinates with αi first. The product of the remaining root subgroups is then a closed subvariety of U of dimension ∣Φ+∣−1; it lies in Ni, which has the same dimension, so equals Ni. Hence U=UαiNi. Since ni is an ideal, its normalizer in the connected group Pαi has full Lie algebra and hence equals Pαi; thus Ni is normal in Pαi. The quotient Pαi/Ni is generated by T and the images of Uαi and U−αi. The rank-one homomorphism of Rank-one SL2 homomorphism and Weyl representative supplies the semisimple rank-one subgroup. The central subtorus (ker⁡αi)0⊆T centralizes it, and αi∘αi∨(t)=t2 shows that its quotient in T is covered by the coroot torus up to finite index. Hence Pαi/Ni is a central product of a torus and a semisimple rank-one group, so it is reductive and has no nontrivial connected normal unipotent subgroup. By Radical, unipotent radical, semisimple and reductive algebraic groups, Ni is the unipotent radical of Pαi. It is therefore Pαi-stable and has dimension ∣Φ+∣−1. Thus N∖G⋅e is contained in the finite union of the images of G×PαiNi⟶N,[g,u]⟼Ad⁡(g)log⁡u. Here log⁡:Ni→ni is the polynomial inverse of the exponential just constructed; it is Pαi-equivariant by conjugation, so the displayed map is well-defined. Each source has dimension (∣Φ+∣−1)+(∣Φ+∣−1)=2∣Φ+∣−2 by [F4]. Hence the complement of the open regular orbit has codimension at least two. The Jacobian rank at e is full by the proof of [F1]; G-equivariance makes every point of G⋅e regular. Thus N is regular in codimension one. Since it is an integral complete intersection, [F7] gives normality.

3.1F2F3F8F9step 1.1step 2.1step 1.2

The fiber over e is a single point. Indeed, if e∈Ad⁡(g)n+, write g=b1nwb2 by [F3]. The element x=Ad⁡(b1−1)e still has every simple coefficient nonzero by [F2]. Since Ad⁡(nw−1)x∈n+, each nonzero simple-root component of x must map to a positive root space; distinct root spaces cannot cancel. Therefore w−1 sends every positive simple root to a positive root, so w=1 by [F3], and gB=B. This algebraic argument holds after every algebraically closed extension of C as well. Equivariance gives a singleton geometric fiber over every point of O=G⋅e. The restriction μO:μ−1(O)→O is proper by base change. Its fibers are finite type and their geometric point sets are singletons, so each fiber point is isolated and has residue field finite over the base residue field; the finite-fiber criterion in [F8] makes μO quasi-finite, and proper quasi-finite finiteness in [F8] makes it finite. Both source and target are integral of dimension 2∣Φ+∣, so the induced function-field extension is finite. It is separable in characteristic zero, and by [F9] has a primitive element θ. After replacing an affine open Spec⁡A⊆O by a smaller nonempty principal open, its finite preimage is Spec⁡B with B finite over A, θ lies in B, and B=A[θ]≅A[T]/(f) for the monic minimal polynomial f of θ: first clear denominators to place θ in B, then localize to kill the finite torsion quotient B/A[θ] and to put the coefficients of f in A. The discriminant of f is nonzero by separability, so after inverting it this finite map is étale of rank d=[Frac⁡B:Frac⁡A]. Every geometric closed fiber in this open then has d distinct points, but every geometric fiber over O is a singleton; therefore d=1. This proves birationality without inferring degree from a closed-point count alone.

4.1F7F10step 2.1step 1.2step 3.1∎

Let R=C[N] and S=Γ(T∗X,O). Properness makes S=Γ(N,μ∗OT∗X) a finite R-algebra by [F10]. Birationality embeds S in Frac⁡(R) and contains R. Every element of a finite R-algebra is integral over R by the determinant trick. Since R is integrally closed by step 2.1, S=R. This proves the Springer-functions isomorphism without inferring regularity of a rational function from connected fibers.

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Partial-flag twist and local product decomposition

Statement

Let α be a simple root, Pα its minimal parabolic, Y=G/Pα, and pα:X=G/B→Y. Let κ∈h∗ satisfy ⟨κ,α∨⟩=0. The restriction of κ to pα that is zero on root spaces is a Lie algebra character. Define the partial-flag TDO Dκ−ρα on Y as the action-algebroid quotient whose isotropy character is this restriction of κ; the subscript κ−ρ uses the convention that a TDO parameter ν has isotropy character ν+ρ. For a quasicoherent left Dκ−ρα-module N, define pα†N on a Zariski product chart pα−1(U)≅U×P1 to be the ordinary inverse-image module OP1⊠N∣U: relative vector fields differentiate the first factor, and base operators act on the second. Its underlying sheaf is OX⊗pα−1OYpα−1N; the differential transition maps are induced by the chain rule under changes of the Pα-torsor section. Then these local modules glue to a quasicoherent left Dκ−ρ-module, and tensoring by OX(ρ) turns it into a left Dκ-module. The restriction of OX(ρ) to each pα-fiber is OP1(−1).

For a torsor section s:U→G, the product chart used below is the commutative square whose top arrow is Φs(u,qB)=s(u)qB:

U£P®=Bp¡1®(U)UU©spr1p®idU

The left vertical map is projection, and the bottom map is identity. The torsor section makes Φs an isomorphism; the equality pα∘Φs=pr1 verifies commutativity. The diagram records the local chart only; the PBW and gluing arguments below prove the TDO identifications.

Facts & Assumptions

Given: The simply connected complex semisimple group, its flag variety, a simple root α, the minimal-parabolic projection pα, and κ with ⟨κ,α∨⟩=0.

[F1]

ρ=12∑β∈Φ+β is an integral weight and ⟨ρ,α∨⟩=1 (The Weyl vector rho for a chosen positive system).

[F2]

G→Y is a Zariski-locally trivial right Pα-torsor and Pα/B≅P1; in the rank-one case Y is a point (Zariski sections of Borel and minimal-parabolic orbit maps, A minimal-parabolic flag projection is a projective-line bundle).

[F3]

The action-algebroid quotient construction has the ordered-basis PBW filtration with associated graded the symmetric tangent algebra, and tensoring by an integral line bundle changes the TDO parameter by its weight (Flag-variety twisted differential operators and their modules, PBW and integral line-bundle twisting for flag TDOs).

Proof

1.1F1F3givenalgebra

The derived algebra [pα,pα] is spanned by positive-root spaces and the rank-one subalgebra ⟨gα,g−α,α∨⟩. The functional κ vanishes on the root spaces by its definition and on α∨ by the assumed zero pairing. It therefore kills the derived algebra, so it is a Lie algebra character of pα. Its transport to the isotropy bundle on Y is well-defined because a character is invariant under conjugation by the connected group Pα. Applying the PBW quotient construction of [F3] to the action algebroid of G on Y defines Dκ−ρα with associated graded Sym⁡TY.

2.1F1F2F3step 1.1algebraconstruct

Choose a Zariski open U⊆Y with a section s:U→G of the Pα-torsor, as in [F2]. For a principal H-bundle Q→Z, write its Atiyah algebroid as TQ/H, the bundle of H-invariant vector fields with its anchor and bracket. The infinitesimal left G-action identifies the action algebroid of G on G/B with this Atiyah algebroid for G→X: on each fiber the left fundamental fields identify g with TgG, and the sign convention is the one in the displayed action-algebroid bracket. The section identifies G∣U with U×Pα, so the Borel torsor is U×Pα→U×(Pα/B). Its Atiyah algebroid splits as TU⊕pr⁡2∗At⁡(Pα→Pα/B), with zero cross-brackets because the two factors act on separate coordinates. The action algebroid of G on Y=G/Pα similarly becomes the Atiyah algebroid of G→Y, locally TU⊕(U×pα); quotienting its isotropy by κ∣pα leaves Diff⁡U, which is the local form of Dκ−ρα. In the vertical factor At⁡(Pα→Pα/B), the rank-one isotropy character is zero because κ vanishes on the root spaces and on α∨; the central isotropy acts trivially on Pα/B and its scalar relation adds no relative differential operator. Thus the vertical quotient is the rank-one TDO with parameter −ρsl2, which by [F3] is Diff⁡(OP1). The PBW normal forms of the direct-product algebroid therefore identify Dκ−ρ∣pα−1(U)≅DP1⊠Dκ−ρα∣U. The line bundle OX(ρ) restricts to degree −1 on the fiber because its associated character pairs to 1 with α∨; hence its restriction is OP1(−1).

3.1F1F2F3step 2.1construct∎

On overlaps, write the torsor sections as sj=sipij for a regular map pij:Ui∩Uj→Pα. The change of product trivialization is (u,qB)↦(u,pij(u)qB). On the Atiyah algebroid it is the gauge transformation of the product principal B-bundle: its base component includes the derivative of pij in pα, and its fiber component is the differential of left multiplication by pij(u) on Pα/B. The quotient of the base component by κ∣pα is exactly the transition of Dκ−ρα; the fiber component acts by the chain rule on relative operators. The isotropy character is preserved because it is a Lie-algebra character invariant under Ad⁡(Pα), and the equality pik=pijpjk makes the gauge maps compose, giving the cocycle identity. Thus the local product TDO identifications agree on overlaps. The local ordinary inverse-image modules OP1⊠N∣U glue to pα†N: in product coordinates a vertical field acts by ∂z(f⊗n)=∂z(f)⊗n, and a base operator acts by its derivative on f plus its given action on n. The chain rule is precisely the algebroid transition just checked, so this is a module for the pulled-back TDO, not its regular left module. Finally [F3] identifies OX(ρ)⊗pα†N as a Dκ-module because tensoring by OX(ρ) shifts the parameter from κ−ρ to κ.

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Global sections of twisted differential operators on the flag variety

Statement

Assume the setup of Flag-variety twisted differential operators and their modules and the Axiom of Choice. For every complex κ, the infinitesimal action on Dκ induces a filtered algebra isomorphism Aκ=U(g)/U(g)ker⁡χκ→∼Γ(X,Dκ), where χκ(z)=pr⁡(z)(κ−ρ). No dominance, regularity, or integrality condition is imposed on κ.

Facts & Assumptions

Given: A complex semisimple Lie algebra with chosen positive system, X=G/B, arbitrary κ∈h∗, and the action-algebroid TDO Dκ.

[F1]

Dκ is a TDO with gr⁡Dκ=Sym⁡TX and the infinitesimal action has its stated principal symbol (PBW and integral line-bundle twisting for flag TDOs).

[F2]

The PBW central quotient has associated graded the reduced coordinate ring C[N] of the nilpotent cone (The nilpotent central fiber is reduced and integral).

[F3]

The Springer map is proper birational and pullback identifies C[N]≅Γ(T∗X,O) (Normality of the nilpotent cone and Springer functions).

[F4]

The canonical bundle is ωX=OX(2ρ) in the associated-character convention of Flag-variety twisted differential operators and their modules (Canonical weight of a flag variety).

[F5]

For a cyclic highest-weight module of highest weight λ, a central element z acts by pr⁡(z)(λ) (The Harish-Chandra projection computes the highest-weight scalar).

Proof

1.1F1F4F5givenalgebra

Let ϕκ:U(g)→Γ(X,Dκ) be the infinitesimal-action map. Use the fiber Q=Dκ,eB/Dκ,eBmeB for the right OX-module structure, and write δ for the class of 1. This is a left U(g)-module. Choose local coordinates tj at eB and a local differential-operator trivialization. For b∈b, its operator is ∑jfj∂tj+cb, with fj(eB)=0 and cb(eB)=(κ+ρ)(b) by the isotropy relation. Moving coefficients to the right gives bδ=(cb(eB)−∑j∂tjfj(eB))δ. The anchor action on functions is the negative of the tangent action on points, so its linear trace on g/b is 2ρ(b), since the tangent weights are the negative roots; equivalently this is the canonical character in [F4]. Thus bδ=(κ−ρ)(b)δ, and n+δ=0. Negative-root vector fields span the tangent space at eB; PBW symbols [F1] show that their ordered monomials on δ span Q by induction on order. Hence Q is a cyclic highest-weight module of weight κ−ρ, so every central z acts by pr⁡(z)(κ−ρ)=χκ(z) by [F5]. Equivariance gives the same scalar on every closed right fiber. Only Lie algebra characters were used, so no nonintegral line bundle is required.

2.1F1F2step 1.1

Fix an order bound m. The space U(g)≤m is finite-dimensional by PBW, and FmDκ is locally free of finite rank as a right OX-module by the same PBW normal forms [F1]. For z∈ker⁡χκ, the right OX-linear multiplication map U(g)≤m⊗OX→Fm+d(z)Dκ given by u⊗f↦ϕκ(u(z−χκ(z)))f is zero on every closed fiber by step 1.1. In local frames this is a finite matrix of regular functions vanishing at every closed point; X is reduced and of finite type over C, so each entry is zero. Thus ϕκ kills the whole two-sided central ideal and factors through a filtered map ϕˉκ:Aκ→Γ(X,Dκ). This finite-rank argument does not apply Nakayama to an infinitely generated module.

3.1F1F2F3step 2.1

The associated-graded map fits into C[N]⟶gr⁡Aκ⟶gr⁡Γ(X,Dκ)↪Γ(X,gr⁡Dκ)=Γ(T∗X,O). The last inclusion follows by applying the left-exact functor Γ to each order-filtration sequence. The composite is pullback by the Springer moment map: for x∈g, its linear function on N pulls back to the principal symbol of the vector field xX, namely ξ↦ξ(xX) on T∗X. Linear functions generate C[N] as a quotient of S(g), so the two algebra maps agree on all generators. By [F3] the composite is an isomorphism.

4.1step 3.1algebra∎

Since the composite in [step 3.1] is an isomorphism and its right-hand map is injective, both intermediate associated-graded maps are isomorphisms. A filtered map with associated-graded isomorphism is an isomorphism: lift a target symbol and subtract a lift to lower the order until surjectivity holds; for injectivity, a nonzero kernel element would have a nonzero leading symbol in the graded kernel. Hence ϕˉκ is the asserted filtered algebra isomorphism. The argument uses no order condition on κ.

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Global sections and localization at a fixed infinitesimal character

Definition

Fix κ∈h∗ and Aκ, Dκ as in Flag-variety twisted differential operators and their modules. By Global sections of twisted differential operators on the flag variety, the sheaf Dκ is a right Aκ-module by multiplication by global sections, and Γ(X,−) takes values in left Aκ-modules through the infinitesimal action. Define Loc⁡κ(V):=Dκ⊗AκV,V∈Aκ-Mod, where the tensor product is the sheaf tensor product. Define Γκ(M):=Γ(X,M) for a quasi-coherent left Dκ-module M. Localization is right exact as a tensor functor. The next item proves the adjunction and verifies that these constructions land in the stated categories.

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Ample translation maps split by central-character separation

Statement

Let κ∈h∗ and let η be a sufficiently dominant integral weight, so that Lη=OX(−η) is ample. Put Vη=Γ(X,Lη)∗, the finite-dimensional irreducible representation of highest weight η. For any quasi-coherent left Dκ-module M, the natural coevaluation map M⟶M⊗OXLη⊗CVη is a split injection of sheaves of complex vector spaces when κ is antidominant. The natural evaluation map M⊗CVη∗⟶M⊗OXLη is a split surjection of such sheaves when κ is regular antidominant. The maps and their splittings commute with the diagonal U(g)-actions and are natural in M. The tensor factors Lη,Vη carry their specified G-linearizations; no B-action on arbitrary M is assumed. The splittings need not be OX-linear. These sheaf splittings suffice for the induced split maps on cohomology.

Facts & Assumptions

Given: The setup above, an arbitrary quasi-coherent M, and either the antidominance or the regular-antidominance hypothesis as appropriate.

[F1]

Lη is globally generated and ample; its space of sections is finite-dimensional, and Vη=Γ(Lη)∗ is irreducible with highest weight η (The Borel-Weil theorem, G-linearizations of invertible sheaves on a complex G-variety).

[F2]

Every weight ηj of Vη satisfies η−ηj∈Q+, with equality only for the unique highest-weight line; one can order its weight lines to give a B-stable filtration (The Borel-Weil theorem).

[F3]

Antidominant κ forbids κ−wκ∈Q+∖{0}, while regular antidominant κ forbids κ−wκ∈Q+ for w≠1 (Complex-weight separation of Harish-Chandra characters).

[F4]

Every quasi-coherent Dν-module has exact central action χν, and tensoring by an integral line bundle shifts the TDO parameter by its weight (Global sections of twisted differential operators on the flag variety, PBW and integral line-bundle twisting for flag TDOs).

[F5]

In a commutative ring, finitely many pairwise comaximal ideals give a surjection onto the product of their quotient rings; its kernel is their product (Chinese remainder theorem for pairwise comaximal ideals).

[F6]

Harish–Chandra identifies the center with Weyl-invariant polynomials in the shifted parameter, so two shifted characters are equal exactly when their parameters lie in the same Weyl orbit (Harish-Chandra isomorphism for the center). Indeed distinct finite orbits are separated by polynomial interpolation on their finite union, then averaging over the finite Weyl group makes the separator invariant.

Proof

1.1F1F2construct

Form the finite G-equivariant bundle E(Vη)=G×BVη. The map [g,v]↦(gB,gv) identifies it with the trivial bundle X×Vη with its diagonal G-action. Choose a weight basis in each weight space and order the weights with higher weights first. Positive root operators raise weights, so the resulting complete filtration is B-stable and its successive quotient lines have characters ηj as in [F2]. Association to G→X is exact on this finite filtration: on every torsor chart it is tensoring a sequence of complex vector spaces with OX. Its quotient line bundles are OX(ηj), with highest line OX(η). Tensoring this bundle filtration with arbitrary M remains exact, since each quotient is locally free.

2.1F1F2F4step 1.1construct

The coevaluation OX→Lη⊗E(Vη) is the highest line in this filtration; dually the evaluation E(Vη)∗→Lη is the quotient of weight −η. These are the duals of evaluation of the globally generated line bundle [F1], so they are respectively injective and surjective, locally split as vector-bundle maps. After tensoring with M they give the maps in the Statement, with the same exact filtration positions. Each associated quotient of the first target is M⊗OX(−η+ηj), with central character χκ−η+ηj by [F4]. The evaluation source has quotients M⊗OX(−ηj) with characters χκ−ηj; its target has character χκ−η. All these filtrations are preserved by the diagonal g-action because their finite bundle factors are G-equivariant.

3.1F2F3F6step 2.1algebra

For the coevaluation, every quotient other than its image has ηj≠η. If its character were χκ, equality of Harish–Chandra characters would give some w∈W with κ−wκ=η−ηj∈Q+∖{0}, contrary to [F3]. Thus the image is the sole filtration quotient with character χκ. This argument applies to the actual filtered module involving M, not to a supposed tensor-character identity for an unfiltered arbitrary tensor product.

3.2F2F3F6step 2.1algebra

For the evaluation, if ηj≠η had χκ−ηj=χκ−η, then κ−ηj=w(κ−η) for some w. Rearranging gives κ−w−1κ=η−w−1ηj∈Q+, since w−1ηj is again a weight of Vη. If the right side is nonzero, antidominance [F3] rules it out; if it is zero, regularity [F3] forces w=1 and hence ηj=η, a contradiction. Thus its target is the sole quotient with the distinguished character.

3.3F4F5step 2.1algebraconstruct

For a sheaf of complex vector spaces with a finite filtration of exact central-character quotients, a product of powers of their finitely many maximal ideals in Z(U(g)) annihilates the sheaf. Powers of distinct maximal ideals are comaximal: expand 1=(u+v)a+b−1 with u+v=1, u in the first ideal and v in the second. Thus [F5] gives central polynomial projectors onto the corresponding generalized-character summands. These polynomials act on sections by the diagonal differential U(g)-action, commute with restrictions and with U(g), and hence are morphisms of sheaves of complex vector spaces. They are natural in M. They are generally differential operators rather than OX-linear maps; that stronger linearity is neither asserted nor needed.

4.1step 3.1step 3.2step 3.3algebra∎

By step 3.1 the distinguished projector on the coevaluation target has image exactly the injected copy of M: it is identity on that copy, and its induced action on the filtered quotient is zero. Composing with the inverse of this identification gives a sheaf retraction. By step 3.2 the distinguished summand of the evaluation source maps isomorphically onto its target, since the kernel has no such character; invert that restriction to get its sheaf section. Step 3.3 supplies all asserted naturality and U(g)-linearity. Applying sheaf cohomology to either split pair preserves its retraction or section, proving the final assertion.

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Localization is left adjoint to global sections

Statement

For every κ∈h∗, Loc⁡κ:Aκ-Mod→QCoh⁡(X,Dκ) is left adjoint to Γκ:QCoh⁡(X,Dκ)→Aκ-Mod.

Facts & Assumptions

Given: The TDO sheaf Dκ, its global algebra Aκ≅Γ(X,Dκ), a left Aκ-module V, and a quasi-coherent left Dκ-module M.

[F1]

Aκ≅Γ(X,Dκ) as filtered algebras (Global sections of twisted differential operators on the flag variety).

[F2]

Localization is the sheafification of W↦Dκ(W)⊗AκV, with restrictions induced from Dκ (Global sections and localization at a fixed infinitesimal character); the tensor-Hom correspondence for this construction is checked in step 2.1.

[F3]

The local PBW basis makes Dκ quasi-coherent as a left OX-module (PBW and integral line-bundle twisting for flag TDOs, proof steps 1.1–2.1). On an affine chart U=Spec⁡R, it is therefore the associated sheaf of Q=Γ(U,Dκ); its sections on D(f) are Qf (Affine quasi-coherent sheaves are modules). The Axiom of Choice is inherited from these suppliers.

Proof

1.1F2F3givenalgebra

On an affine chart U=Spec⁡R, put Q=Γ(U,Dκ). Right multiplication by Aκ commutes with left multiplication by R. Thus Q⊗AκV is an R-module, and for every f∈R there is a natural isomorphism Qf⊗AκV≅(Q⊗AκV)f,(q/fm)⊗v⟼(q⊗v)/fm. The inverse sends (q⊗v)/fm to (q/fm)⊗v; additivity and the balancing relations make both maps well-defined. By [F2] and [F3], the tensor presheaf on the distinguished-open basis of U is therefore the associated sheaf of Q⊗AκV. Its sheafification has that restriction on U, proving that Loc⁡κV is quasi-coherent. Left multiplication on its first factor gives its left Dκ-action.

2.1F2step 1.1construct

The tensor-Hom correspondence here follows directly from balancing. Given an Aκ-linear map V→Hom⁡Dκ(Dκ,M), write its value at v as hv and send d⊗v over W to hv∣W(d). The Aκ-action on Hom is (ah)(d)=h(da), so the rule is balanced, respects restrictions, and extends through sheafification to a Dκ-linear map. Conversely such a sheaf map gives hv by d↦ϕ(d⊗v). These constructions are inverse and natural, and step 1.1 places their source in the required quasi-coherent category.

3.1F1step 2.1algebra∎

Evaluation at 1 identifies Hom⁡Dκ(Dκ,M) with Γ(X,M). A morphism is determined by the image of 1; conversely, each global section m defines the morphism d↦d m. Under this identification the Aκ-action is the one from [F1]. Substituting into step 2.1 gives the natural bijection Hom⁡Dκ(Loc⁡κV,M)≅Hom⁡Aκ(V,ΓκM), which is the asserted adjunction. Right exactness of localization follows because a left adjoint preserves cokernels.

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Antidominant twists are D-affine and regular ones are conservative

Statement

Assume the flag-variety setup of Flag-variety twisted differential operators and their modules. If κ is antidominant, then every quasi-coherent left Dκ-module M satisfies Hi(X,M)=0(i>0). Moreover, Γ(X,−) is exact on the category of quasi-coherent left Dκ-modules. If κ is also regular, then Γ(X,M)=0 implies M=0. The antidominance and regularity conditions are independent hypotheses; regularity alone does not imply the vanishing assertion.

Facts & Assumptions

Given: The Axiom of Choice, X=G/B, an ample line bundle OX(−η) for sufficiently dominant integral η, an antidominant (and, for conservativity, regular) κ, and a quasi-coherent left Dκ-module M.

[F1]

Every quasi-coherent OX-module is a filtered union of coherent submodules, and cohomology commutes with those filtered colimits (Quasicoherent modules are filtered unions of coherent subsheaves and cohomology commutes with these colimits).

[F2]

For coherent F and ample L, there is an integer n0 such that Hi(X,F⊗L⊗n)=0 for every i>0 and n≥n0 (Serre vanishing for coherent sheaves and ample twists).

[F3]

For coherent F and ample L, the twist F⊗L⊗n is globally generated for all sufficiently large n (Eventual generation of coherent projective twists, Global generation by the evaluation map).

[F4]

The natural injection M→M⊗L⊗V splits for antidominant κ, and the natural surjection M⊗V∗→M⊗L splits for regular antidominant κ, as sheaves of complex vector spaces; this is enough for the split maps on sheaf cohomology. Here L=OX(−η) and V=Γ(X,L)∗ (Ample translation maps split by central-character separation).

[F5]

For a sheaf of rings, the right-derived global sections on its module category agree with ordinary sheaf cohomology of the underlying module sheaf (Global sections on module sheaves have ordinary sheaf cohomology as derived functors).

Proof

1.1F1F2F4

Let i>0 and write M=lim→⁡jFj as the filtered union of coherent OX-submodules from [F1]. Fix one Fj. Choose a sufficiently dominant integral η so that Hi(X,Fj⊗L)=0 by [F2], with L=OX(−η). The composite Hi(X,Fj)→Hi(X,M)→Hi(X,M⊗L⊗V) factors through Hi(X,Fj⊗L⊗V) by naturality of the coevaluation map. This last group is Hi(X,Fj⊗L)⊗V=0 because V is finite-dimensional. By [F4], the map Hi(X,M)→Hi(X,M⊗L⊗V) is injective. Thus Hi(X,Fj)→Hi(X,M) is zero for every j. Taking the filtered colimit and using [F1] gives Hi(X,M)=0.

2.1F5step 1.1algebra

For every quasi-coherent left Dκ-module M, [F5] and step 1.1 give RqΓMod⁡(Dκ)(X,M)≅Hq(X,M)=0 for each q>0. Given a short exact sequence 0→M′→M→M′′→0 of quasi-coherent Dκ-modules, view it in the full module-sheaf category. Its derived-functor long exact sequence and the vanishing of R1Γ(M′) show that Γ(X,M)→Γ(X,M′′) is surjective; left exactness supplies exactness at the other terms. Hence Γ is exact on quasi-coherent Dκ-modules for antidominant κ.

3.1F1F3F4step 1.1algebra∎

Now assume κ is regular antidominant and Γ(X,M)=0. For any coherent Fj⊆M, choose a sufficiently dominant integral η so that Fj⊗L is globally generated by [F3]. By the split surjection in [F4], Γ(X,M⊗L) is a direct summand of Γ(X,M⊗V∗)=Γ(X,M)⊗V∗=0; hence Γ(X,M⊗L)=0. The inclusion Fj⊗L↪M⊗L remains injective on global sections because Γ is left exact, so Γ(X,Fj⊗L)=0. A globally generated sheaf with no global sections is zero, hence Fj=0. All coherent subsheaves in [F1] vanish, so M=0. This applies the splitting to M, not to the arbitrary coherent OX-submodule.

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The unit V to Gamma Loc_kappa(V) is an isomorphism for antidominant twists

Statement

For antidominant κ and every left Aκ-module V, the unit of the adjunction in Localization is left adjoint to global sections is an isomorphism V→∼Γ(X,Loc⁡κV).

Facts & Assumptions

Given: Antidominant κ and a left Aκ-module V.

[F1]

Γ(X,−) is exact on quasi-coherent Dκ-modules for antidominant κ (Antidominant twists are D-affine and regular ones are conservative).

[F2]

Γ(X,Dκ)=Aκ as a filtered algebra (Global sections of twisted differential operators on the flag variety).

[F3]

On this finite affine cover, global sections of quasi-coherent modules commute with filtered colimits, hence with arbitrary direct sums (Quasicoherent modules are filtered unions of coherent subsheaves and cohomology commutes with these colimits).

Proof

1.1F1given

Choose a free presentation Aκ(I)⟶Aκ(J)⟶V⟶0. Localization is a tensor functor, so it is right exact and gives Dκ(I)⟶Dκ(J)⟶Loc⁡κ(V)⟶0. Applying the exact global-sections functor [F1] preserves exactness.

2.1F2F3step 1.1algebra∎

By [F3], global sections commute with the direct sums in step 1.1; by [F2], each free term becomes the corresponding free Aκ-module. Under the adjunction unit, the maps on these free terms are the identity maps on Aκ(I) and Aκ(J). The cokernels of the two presentations are therefore identified by the induced unit map on V. Hence V→Γ(X,Loc⁡κV) is an isomorphism.

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The singular simple-parabolic kernel on the flag variety

Statement

Let κ be antidominant and let α be a simple root with ⟨κ,α∨⟩=0. Put pα:X=G/B→Xα=G/Pα, a Zariski-locally trivial P1-bundle, and let ρ=12∑β∈Φ+β. Use the partial TDO Dκ−ρα and pullback module pα†N defined in Partial-flag twist and local product decomposition. For every coherent Dκ-module M:

  1. Rqpα∗M=0 for every q>0;
  2. pα∗M=0 if and only if there is a coherent Dκ−ρα-module N with M≅OX(ρ)⊗pα†N, where N≅pα∗(OX(−ρ)⊗M); this determines N up to canonical isomorphism.

Facts & Assumptions

Given: Antidominant κ, a simple root α with zero pairing, the minimal parabolic projection pα, and a coherent Dκ-module M.

[F1]

The projection is a Zariski-locally trivial P1-bundle; on product charts its TDO has the singular rank-one relative factor. The ordinary inverse image of a base module has relative factor OP1, and OX(ρ) has relative factor OP1(−1) (A minimal-parabolic flag projection is a projective-line bundle, Partial-flag twist and local product decomposition).

[F2]

For a coherent product differential module on P1×U with singular relative factor D0=Diff⁡(O(−1)), all positive higher direct images to U vanish. Its direct image is zero if and only if it is O(−1)⊠N for a coherent base-TDO module N, recovered as the direct image after tensoring by O(1). The canonical evaluation is compatible with the differential transition maps and glues (Relative rank-one classification of the singular differential kernel).

Proof

1.1F1F2given

Cover Xα by the product charts of [F1]. On each chart [F2] proves Rqpα∗M=0 for every q>0, including arbitrary base affine opens. Higher direct image is a sheaf on the base, so vanishing on this open cover proves assertion (1). In particular the underlying sheaf direct-image functor is exact on coherent Dκ-modules: its long exact sequence has zero R1 term for every coherent kernel.

2.1F1F2step 1.1construct

Suppose pα∗M=0. On a product chart, [F2] gives the canonical differential-module isomorphism M=O(−1)⊠N, with N=pα∗(OX(−ρ)⊗M) in that chart's partial TDO convention. The inverse image in [F1] has relative structure-sheaf factor, so this is precisely the displayed form OX(ρ)⊗pα†N. The proof of [F2] makes its evaluation natural in all commuting base operators; on overlaps it is intertwined by the chain rule and the partial TDO cocycle in [F1]. Thus the base actions glue on the stated direct image and the local isomorphisms glue to the asserted global one. Coherence of N is part of [F2], not an inference from OX-coherence of M.

3.1F1F2step 2.1algebra∎

Conversely, the displayed form has local relative factor O(−1)⊠N by [F1], whose direct image is zero by [F2]; hence pα∗M=0 globally. Tensoring this form by OX(−ρ) and applying pα∗ recovers N, since pα∗pα†N=N. The same identity proves uniqueness up to the recovered canonical isomorphism. This proves both directions and all higher-image assertions; no rank-one classification is left as a source-only premise.

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The singular antidominant Serre quotient

Statement

Let κ be antidominant, not necessarily regular, and let Γ=Γκ:QCoh⁡(X,Dκ)⟶Aκ-Mod,K=ker⁡Γ. Then K is a Serre subcategory and the induced functors give an equivalence of abelian categories QCoh⁡(X,Dκ)/K≃Aκ-Mod. The quotient has representatives precisely among the quasicoherent Dκ-modules that are generated by global sections and have no nonzero quasicoherent Dκ-submodule with zero global sections. No equivalence with the whole Dκ-module category is asserted without regularity.

Facts & Assumptions

Given: Antidominant κ, the exact global-sections functor Γκ, the localization functor and their adjunction.

[F1]

Γκ is exact for antidominant κ (Antidominant twists are D-affine and regular ones are conservative).

[F2]

The adjunction unit V→ΓκLoc⁡κV is an isomorphism for every Aκ-module (The unit V to Gamma Loc_kappa(V) is an isomorphism for antidominant twists).

[F3]

Loc⁡κ is left adjoint to Γκ (Localization is left adjoint to global sections).

[F4]

Global sections on X commutes with filtered colimits of underlying quasicoherent sheaves, and therefore with arbitrary direct sums (Quasicoherent modules are filtered unions of coherent subsheaves and cohomology commutes with these colimits).

Proof

1.1F1given

Since Γκ is exact, its kernel K is closed under subobjects, quotients and extensions; hence K is a Serre subcategory. The functor Γκ therefore descends to the Serre quotient.

2.1F1F2step 1.1

Localization is right exact. For a short exact sequence 0→V′→V→V′′→0 of Aκ-modules, applying localization gives a right-exact sequence Loc⁡V′⟶Loc⁡V⟶Loc⁡V′′⟶0. Apply the exact functor Γκ and use [F2]. The resulting sequence is 0→V′→V→V′′→0. Therefore the kernel of Loc⁡V′→Loc⁡V has zero global sections and lies in K. Thus localization becomes exact after passage to the Serre quotient.

3.1F1F2F3step 2.1

The unit is an isomorphism by [F2], so it remains an isomorphism in the quotient. For any M, the triangular identity in [F3] shows that applying Γκ to the counit Loc⁡κΓκM→M gives an isomorphism. By exactness [F1], the kernel and cokernel of the counit lie in K; hence the counit is an isomorphism in the quotient. The descended unit and counit prove the claimed equivalence.

4.1F1F4step 3.1construct

For an arbitrary M, let E be the image of the counit Loc⁡κΓM→M. By step 3.1 its cokernel has zero global sections, so E and M define isomorphic objects of the Serre quotient. The source is generated by its global sections, hence so is E. This holds even for generation as an OX-module: PBW and the surjective action anchor show that Dκ is locally spanned over OX by products of the global g-operators; their actions on global sections remain global sections. Among the submodules of E with zero global sections, take their sum T. This is a set-indexed sum: a submodule sheaf is specified by a family of subsets of the sets E(U), one for each open U⊆X. The direct sum of any such family is again a quasicoherent Dκ-module, and Γ commutes with it by [F4]. Exactness of Γ [F1] then gives ΓT=0, so T is the largest submodule of E in K. The quotient E/T remains generated by global sections. If S⊆E/T has ΓS=0, its inverse image P⊆E fits into 0→T→P→S→0; exactness [F1] gives ΓP=0, so P⊆T by maximality and S=0. Thus E/T is a representative of the same quotient object, is generated by global sections, and has no nonzero submodule in K. Conversely, every module with those two properties is by definition such a representative.

5.1F1F2F3step 3.1step 4.1algebra∎

These representatives give an actual equivalence with the algebra-module category, not just a choice of quotient objects. If E,D are generated by global sections and have no nonzero subobject in K, any map with zero global sections has image in K and hence is zero. Given h:ΓE→ΓD, adjunction [F3] gives f:Loc⁡ΓE→D. The evaluation counit onto E is surjective because E is generated by global sections; its kernel is in K by step 3.1. Its image under f is therefore a K-subobject of D and is zero, so f factors uniquely through a map E→D inducing h. This proves full faithfulness of Γ on these representatives. For any algebra module V, apply the construction of step 4.1 to Loc⁡V; [F1]–[F2] give its representative global sections equal to V, proving essential surjectivity.

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Regular antidominant Beilinson–Bernstein localization

Statement

Assume the setup of Global sections and localization at a fixed infinitesimal character. If κ is regular antidominant, then Loc⁡κ:Aκ-Mod⇄QCoh⁡(X,Dκ):Γκ are inverse equivalences between all left Aκ-modules and all quasi-coherent left Dκ-modules. The equivalence restricts to finitely generated Aκ-modules and coherent Dκ-modules. It does not assert that Γ is faithful for a fixed non-antidominant representative of a regular central character. Here a coherent Dκ-module means a module locally finitely presented over the sheaf of rings Dκ; its local noetherianity is part of the proof below.

Facts & Assumptions

Given: Regular antidominant κ, the adjunction Loc⁡κ⊣Γκ, and the unit and conservativity results already proved.

[F1]

Loc⁡κ is left adjoint to Γκ (Localization is left adjoint to global sections).

[F2]

The unit V→ΓLoc⁡V is an isomorphism for every Aκ-module when κ is antidominant (The unit V to Gamma Loc_kappa(V) is an isomorphism for antidominant twists).

[F3]

Γ is exact and conservative when κ is regular antidominant (Antidominant twists are D-affine and regular ones are conservative).

Proof

1.1F1F2

The unit is an isomorphism by [F2]. For a quasi-coherent Dκ-module M, let ϵM:Loc⁡κΓκM→M be the counit. The triangular identity for the adjunction says Γκ(ϵM)∘ηΓκM=id⁡ΓκM, where η is the unit. Since η is an isomorphism, Γ(ϵM) is an isomorphism.

2.1F1F3step 1.1

Exactness of Γ in [F3] implies Γ(ker⁡ϵM)=0 and Γ(coker⁡ϵM)=0. Conservativity in [F3] makes both sheaves zero, so ϵM is an isomorphism. The unit and counit are isomorphisms, hence the adjoint functors are inverse equivalences.

3.1F1step 2.1algebra

By Noetherianity of the enveloping algebra, U(g) is left Noetherian, so its quotient Aκ is left Noetherian. On a smooth affine chart of X, Sym⁡TX is a polynomial algebra over a finite-type C-algebra and hence is Noetherian by If R is Noetherian then R[x1,…,xn] is Noetherian for every n∈N. If a filtered ring has Noetherian associated graded, every left ideal is finitely generated: choose finitely many lifts of homogeneous generators of its graded ideal, subtract their leading terms from an arbitrary ideal element, and induct on its finite filtration degree. This proves that Dκ is locally left Noetherian. A finitely generated Aκ-module has a finite presentation over the Noetherian ring Aκ; localization presents it locally as a quotient of a finite free Dκ-module, hence as a coherent Dκ-module.

4.1F1F3step 2.1step 3.1algebra∎

Conversely, let M be coherent over Dκ. A finite affine cover of X and local finite generation give finitely many local generators. The counit is an isomorphism by step 2.1, so each such generator is locally in the image of the evaluation map Dκ⊗CΓ(X,M)→M. These local image neighborhoods cover X; quasi-compactness gives a finite subcover, hence a finite set S⊂Γ(X,M) whose Dκ-span is all of M. Thus the map Dκ∣S∣→M is surjective. Exactness of Γ in [F3] gives a surjection Aκ∣S∣=Γ(X,Dκ∣S∣)→Γ(X,M), so Γ(X,M) is finitely generated over Aκ. This is coherence over Dκ, not coherence over OX.

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The integral regular localization equivalence restricts to Category O

Statement

Let κ be integral, regular and antidominant. Define the exact central-character subcategory Oχκexact={V∈O:(ker⁡χκ)V=0}. A strongly B-equivariant coherent Dκ-module means a coherent left Dκ-module with a rational B-linearization whose differential is the action-algebroid action and whose action is compatible with the Dκ-module structure. Then Loc⁡κ and Γκ restrict to inverse equivalences between Oχκexact and these strongly B-equivariant coherent modules.

The exact subcategory is distinct from the generalized-character block, where each vector is killed by some power of ker⁡χκ; the theorem does not identify the whole generalized block with B-equivariant coherent modules.

Facts & Assumptions

Given: Integral regular antidominant κ; the BGG category O of The classical BGG category O; its finite-length and simple-highest-weight structure; and the equivalence of Regular antidominant Beilinson–Bernstein localization.

[F1]

Every object of O has finite length, and its simple objects are exactly the highest-weight modules L(λ) (Every object of O has finite length, The simple objects of O).

[F2]

The center acts on a cyclic highest-weight module of highest weight λ by the Harish–Chandra character z↦pr⁡(z)(λ); the shifted Harish–Chandra map separates Weyl orbits (The Harish-Chandra projection computes the highest-weight scalar, Harish-Chandra isomorphism for the center).

[F3]

In BGG category O, h acts semisimply and U(n+)v is finite-dimensional for each vector; the module is finitely generated (The classical BGG category O).

[F4]

The regular antidominant equivalence restricts to finitely generated Aκ-modules and coherent Dκ-modules, and its unit and counit are natural isomorphisms (Regular antidominant Beilinson–Bernstein localization).

[F5]

The Borel has the semidirect-product decomposition B=T⋉U. Multiplication in U is given by the height-ordered positive-root coordinates, whose finite BCH law is compatible with the Lie brackets; conjugation by T acts on each root subgroup through its root character (Borel, opposite unipotent groups and root coordinates).

Proof

1.1F1F2givenalgebra

Let V∈Oχκexact. By [F1] it has a finite composition series with factors L(λ). Since the central ideal ker⁡χκ annihilates V, it annihilates every subquotient; thus each factor has central character χκ. By [F2], this means λ+ρ and κ have the same values on all Weyl-invariant polynomials. These invariants separate the finite W-orbits: for two disjoint finite orbits, polynomial interpolation separates their point sets, and averaging the separating polynomial over W makes it invariant. Therefore λ+ρ=wκ for some w∈W. Since κ is integral, λ is integral, and every weight of L(λ) differs from λ by an element of the root lattice. All weights of V are therefore integral.

2.1F2F3F5step 1.1construct

For a weight vector v∈V, the subspace U(n+)v is finite-dimensional by [F3] and is stable under h, since [h,n+]⊆n+. Its weights are integral by step 1.1. Define the rational T-action on each such finite-dimensional subspace by its integral weight characters. Each positive-root operator is nilpotent there because it strictly raises weights in a finite weight set; more generally, a real linear functional positive on all positive roots gives a finite weight filtration strictly raised by every element of n+, so π(X) is nilpotent for each X∈n+. The Lie representation of the nilpotent algebra n+ integrates by u=exp⁡(X)↦exp⁡(π(X)): the finite BCH polynomial is respected by the Lie representation, and the exponential coordinates n+→U and their multiplication law are those of [F5]. For t0∈T, the weight action satisfies ρT(t0)exp⁡(π(X))ρT(t0)−1=exp⁡(π(Ad⁡(t0)X)), so [F5] combines the T and U actions into a rational B=T⋉U-action differentiating to the given b-action. Any finite sum of these subspaces is again finite-dimensional and b-stable; uniqueness of the exponential U-action and the prescribed weight action makes the constructions compatible under inclusions. The subspaces form a directed cover of V, so their compatible actions define a rational B-action on V.

3.1F3F4step 2.1

The TDO Dκ is G-equivariant by its action-algebroid construction. The diagonal B-action therefore makes Loc⁡κ(V) strongly B-equivariant; it is coherent by [F4]. Conversely, if M is strongly B-equivariant and coherent, its global sections inherit a rational B-action. The torus action is a direct sum of integral weight spaces, and the unipotent action makes each U(n+)-orbit finite-dimensional. By [F4], ΓM is finitely generated over Aκ, hence over U(g), and its central ideal acts by zero because Aκ is the central quotient in Flag-variety twisted differential operators and their modules. Thus ΓM lies in Oχκexact.

4.1F4step 3.1∎

The unit and counit of the equivalence in [F4] are natural and B-equivariant, because all functors and maps in their construction commute with the diagonal B-action. Their restrictions are still isomorphisms, so the two restricted functors are inverse equivalences.

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Kashiwara's singular parabolic kernel filtration

Statement

Let κ be antidominant, let J={αi∈Δ:⟨κ,αi∨⟩=0}, and assume its full zero-root subsystem is generated by J. For each α∈J, write pα:X→Xα=G/Pα for the simple parabolic projection. Then there exists a finite sequence α1,…,αN∈J such that for every coherent Dκ-module M the following are equivalent:

  1. Γ(X,M)=0;
  2. there is a finite coherent filtration M=M0⊇M1⊇⋯⊇MN=0 with pαj∗(Mj−1/Mj)=0 for every j.

The sequence is one choice, not asserted to be unique; zero successive quotients are permitted.

Facts & Assumptions

Given: Antidominant κ, its zero simple-root set J, the stated zero-root subsystem condition, and coherent M.

[F1]

A reduced expression for wJ gives a fixed coherent chain EN⊆⋯⊆E0=E, where E=Dκ⊗OXOX(ρ), EN is generated by finitely many global differential sections, and Ej−1/Ej=OX(ρ)⊗pαj†Nj for coherent partial-TDO modules Nj. This includes the empty-word case (A fixed singular Verma chain with globally generated final bundle).

[F2]

The simple-parabolic direct-image functors have no positive higher images on coherent modules and are exact there; the displayed quotients in [F1] lie in their respective kernels (The singular simple-parabolic kernel on the flag variety).

[F3]

For antidominant κ, global sections is exact (The singular antidominant Serre quotient).

[F4]

The regular antidominant equivalence applies to all quasicoherent modules, restricts to coherent modules, and expresses any coherent module as a quotient of a finite sum of its TDO by finitely many global sections (Regular antidominant Beilinson–Bernstein localization). Tensoring by an integral line bundle is the TDO-shifting equivalence (PBW and integral line-bundle twisting for flag TDOs).

Proof

1.1F1F2choose

Choose once and for all the reduced expression and its simple-root sequence from [F1]. The explicit proof there constructs the Verma embeddings, their rational simple-parabolic descent, and the central-character projector proving global generation of the final term. Thus this finite chain is an actual local supplier, independent of M; it is not an unproved instruction to filter a localization functor. By [F2], each quotient belongs to ker⁡pαj∗.

1.2F3givenalgebra

Suppose the asserted filtration of M exists. Every factor Qj satisfies Γ(X,Qj)=Γ(Xαj,pαj∗Qj)=0. Applying exactness [F3] to 0→Mj→Mj−1→Qj→0 gives ΓMj−1=ΓMj. Starting with MN=0 proves ΓM=0.

1.3F1F4constructalgebra

Now suppose ΓM=0. The weight κ−ρ is regular antidominant. As proved by the simple-reflection and dual-positive-root calculation in [F1], for every positive root β, ⟨ρ,β∨⟩ is a positive integer: subtracting it from a nonintegral complex pairing leaves a nonintegral pairing, while subtracting it from a permitted integral pairing, which is nonpositive, gives a strictly negative integer. Thus no positive integral or zero pairing occurs. By the integral twisting equivalence and [F4], OX(−ρ)⊗M is generated by finitely many global differential sections over Dκ−ρ. Tensor back with OX(ρ); the twist bimodule identity gives a surjection En↠M for some finite n, with E as in [F1]. Locally this identity is the equality of line-twisted differential operators from the PBW/twist construction in [F4].

2.1F1F2step 1.3construct

Put T=DκΓ(X,E)⊆E and Q=E/T. The submodule T is the image of the global-section evaluation map and is quasi-coherent; the local filtered-noetherian PBW argument for a TDO makes it coherent as a submodule of the coherent module E. Every component E→M in step 1.3 kills Γ(X,E) because ΓM=0, hence kills T, giving a surjection Qn↠M. The globally generated submodule EN⊆E from [F1] is contained in T: each of its global generators is a section of E. Therefore the images Qj of Ej in Q give Q=Q0⊇⋯⊇QN=0. Their factors are coherent quotients of Ej−1/Ej. Exactness of the corresponding pαj∗ in [F2] puts each factor in its kernel.

3.1F1F2step 1.2step 2.1algebra∎

Take the direct sum of this chain n times and its image under Qn↠M. This gives the required finite coherent filtration of M with the same root sequence; every factor is a coherent quotient of a finite sum of factors from step 2.1, and hence has zero corresponding direct image by [F2]. If the sequence is empty, [F1] gives E=EN globally generated, so T=E, Q=0 and M=0, exactly the length-zero filtration. The argument and step 1.2 prove both directions for all the stated complex parameters, with no unproved singular-kernel or derived-localization premise.

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Relative rank-one classification of the singular differential kernel

Statement

Assume the complex flag-variety setup, including the Axiom of Choice, of Flag-variety twisted differential operators and their modules. On Z=P1 put L=OZ(−1), D=Diff⁡(OZ) and D0=Diff⁡(L). Form E=D0⊗OZL, using the right OZ-action on D0. Evaluation gives E/D0Γ(Z,E)≅L. Every quasi-coherent D0-module Q with Γ(Z,Q)=0 has the canonical form Q≅L⊗CΓ(Z,L−1⊗Q), with trivial sl2-action on the second factor.

For any commutative C-algebra R, the same classification holds for quasi-coherent modules over the vertical ring D0,R on PR1: its kernel modules are exactly LR⊗RN for R-modules N. This form commutes with every scalar extension R→R′. If R is noetherian, coherence over D0,R is equivalent to finite generation of N over R. Scalar extension here concerns only the vertical ring and a central base ring; it makes no claim about transporting arbitrary base derivations.

More generally let U be a smooth affine complex variety and let A be a TDO on U. For the projection r:Z×U→U, a coherent (D0⊠A)-module Q satisfies Rqr∗Q=0 for q>0; moreover r∗Q=0 if and only if the evaluation isomorphism is Q≅L⊠N,N=r∗(L−1⊗Q), where N is a unique coherent A-module. Here the ordinary differential inverse image has underlying sheaf OZ⊠N and relative vector fields differentiate its OZ factor. These isomorphisms are natural in all commuting base differential operators. Consequently they glue over locally trivial P1-bundles with compatible product TDO charts and line bundle restricting to L, as in Partial-flag twist and local product decomposition.

Facts & Assumptions

Given: The complex objects and modules in the statement; the relative coherence assertion assumes coherence over the product differential ring, not coherence over D0 after forgetting the base.

[F1]

Tensoring by L identifies D-modules and D0-modules; filtered local differential operators have the PBW basis (PBW and integral line-bundle twisting for flag TDOs).

[F2]

For Z, both singular parameter 0 and regular parameter −ρ are antidominant. Global sections is exact on their quasi-coherent D-modules, and at −ρ localization and global sections are inverse (Antidominant twists are D-affine and regular ones are conservative, Regular antidominant Beilinson–Bernstein localization).

[F3]

H0(Z,L)=H1(Z,L)=0, H0(Z,OZ)=C, and L⊗TZ=OZ(1) is generated by its two standard global sections (Cech cohomology of line bundles on the projective line).

[F4]

An affine morphism has no positive higher direct images of quasi-coherent sheaves (Higher direct images of quasi-coherent modules vanish along affine morphisms). The product charts and their TDO transitions are those of Partial-flag twist and local product decomposition, with ordinary differential inverse image OZ⊠N.

Proof

1.1F1F3algebra

Morita untwisting identifies E with L⊗D. Its evaluation map ϵ:E→L sends ℓ⊗P to ℓP(1). In an affine coordinate x, the unique normal form P=∑j≥0aj∂xj shows that K=ker⁡ϵ is locally L⊗D∂x. Its order-one part is canonically L⊗TZ: a vector field intrinsically annihilates 1, so this identification does not choose a connection or coordinate. PBW shows K=D0K≤1. By [F3] the two global sections of K≤1=OZ(1) generate K. Conversely every global section of E maps to zero because ΓL=0. Thus D0ΓE=K, proving the universal quotient.

1.2F2F4algebra

Let q:Z×U→Z be the other projection. It is affine, so q∗Q is quasi-coherent, carries the relative D0-action, and has no positive higher direct images by [F4]. Leray and singular vanishing [F2] give Hi(Z×U,Q)=0 for i>0. Apply the same argument over every affine open subset of U; the sheafification of these cohomology groups is Rir∗Q, proving its vanishing. In particular r∗ is exact on quasi-coherent product differential modules.

2.1F1F2F3step 1.1algebra

Put T=L−1⊗Q. By the regular equivalence in [F2], T is generated over D by its global sections, so E(I)↠Q for some set I. Since ΓQ=0, each summand kills ΓE and hence D0ΓE. Step 1.1 gives L(I)↠Q, or OZ(I)↠T. The kernel H is a quasi-coherent D-module. Exactness of Γ embeds ΓH into C(I); its sl2-action is trivial. The natural map OZ⊗CΓH→H sends a constant horizontal section to that same section, and is D-linear because H⊆OZ(I). Its map on global sections is the identity of ΓH. Exactness and regular conservativity in [F2] kill its kernel and cokernel, so it is an isomorphism. Thus H=OZ⊗ΓH and T=OZ⊗V, with V=ΓT. Untwisting gives the claimed canonical evaluation isomorphism and trivial action. The converse follows from ΓL=0.

3.1F1F3F4step 2.1algebra

For any central base ring R, push a module on ZR=Z×Spec⁡R along the affine map to Z and apply step 2.1. Multiplication by R commutes with all vertical operators, so its natural evaluation is R-linear and reconstructs the sheaf as LR⊗RN. Conversely this form has zero direct image by the Čech complex for L tensored over C with N. Tensoring this form over R with R′ proves the asserted scalar-extension compatibility without assuming flatness. If R is noetherian, finite relative differential generators involve finitely many coefficients in N; these coefficients generate N since vertical operators create no new coefficients. Conversely finitely generated N gives a finite relative differential generating set, and PBW over the noetherian ring R makes the relative differential ring left noetherian, proving coherence.

3.2F3F4step 2.1step 1.2algebra

Suppose r∗Q=0. Then Γ(Z,q∗Q)=Γ(Z×U,Q)=0. Step 2.1 applied to q∗Q yields its canonical form L⊗V. Multiplication by Γ(U,OU) and every operator in Γ(U,A) commute with the relative D0 action, so naturality of step 2.1 makes V a module over that base differential ring. Affine quasi-coherent sheafification identifies its sheaf with N=r∗(L−1⊗Q) and the obtained isomorphism with Q=L⊠N. No tensor product is taken over a noncommutative ring: the exterior product is over C with the two commuting actions. Conversely r∗(L⊠N)=0 follows by the two-affine-open Čech calculation for L tensored over C with N.

4.1F1step 3.2algebra

The A-module N of step 3.2 is coherent. On each of the two affine fiber charts choose finitely many product-differential generators of Q. This is possible for a coherent differential module on an affine smooth chart: its quasi-coherent underlying module is determined by sections; local finite generators on a finite principal-open cover become global generators after clearing denominators, and differential operators localize by the Leibniz rule. Trivialize L there and express each chosen generator as a finite sum of polynomials in the fiber coordinate times sections of N. Let N0 be the base differential submodule generated by the finitely many coefficients from both charts. Product differential operators preserve L⊠N0, so the chosen generators imply L⊠N0=L⊠N. Evaluation at any fiber point gives N0=N, proving finite generation. A TDO on a smooth affine chart is left noetherian: PBW gives the noetherian graded algebra Sym⁡TU; lift finitely many graded generators and induct on order to generate any left ideal. Thus finite generation implies coherence.

5.1F3F4step 3.2step 4.1algebra∎

Finally the map p†p∗(L−1⊗Q)→L−1⊗Q is the intrinsic differential evaluation map. On each product chart it is the isomorphism of step 3.2. A change of torsor section acts on the fiber coordinate by its transition, and the chain rule intertwines relative differentiation; the base differential action transforms by the given TDO cocycle. Evaluation therefore agrees on overlaps and glues. Moreover p∗p†N=N, since p∗O=O on a P1-bundle, so N is unique up to its canonical isomorphism. The argument uses choice only for the permitted bases and generating sets in [F2] and the inherited suppliers.

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Exact twisted associated bundles and simple-parabolic descent

Statement

Assume the complex simply connected semisimple setup, including the Axiom of Choice, of Flag-variety twisted differential operators and their modules. Let S be B or a minimal parabolic Pα, put Y=G/S, and let τ be an Ad⁡(S)-invariant character of s. A twisted (g,S)-module of twist τ means a vector space H with a Lie representation π:g→End⁡H and a rational S-representation r, such that dr(x)=π(x)+τ(x)id⁡H(x∈s),r(s)π(A)r(s)−1=π(Ad⁡(s)A). The weight τ can be complex; no rational character s↦sτ is presumed. Define AτS by the action-algebroid quotient on Y with isotropy character τ, and define EτS(H)=G×S(H,r). For infinite-dimensional rational modules, this is the associated quasi-coherent sheaf, locally OY⊗CH. Then EτS is an exact functor to quasi-coherent AτS-modules. For S=B, Aκ+ρB=Dκ.

If V is a finite-dimensional rational G-module, use the diagonal Lie and S actions on H⊗V. Then EτS(H⊗V)≅EτS(H)⊗CV, where the differential action on the right acts only on the first factor: constant vectors in V are horizontal. In particular, with M(λ)=U(g)⊗U(b)Cλ, Eκ+ρB(M(−κ−ρ))≅Dκ,Eκ+ρB(M(−κ))≅Dκ⊗OXOX(ρ). In these formulas the rational B-action is the adjoint action on the induced module with its highest vector of twisted weight 0 or ρ, respectively; the tensor product on the last right-hand side uses the right OX-action on Dκ.

Finally suppose ⟨κ,α∨⟩=0 and H is twisted (g,Pα) of twist κ. Let N=EκPα(H), a module over the partial TDO Dκ−ρα of Partial-flag twist and local product decomposition. Restrict its rational action to B and tensor that rational action by the integral character ρ; with unchanged π this makes H twisted of twist κ+ρ. For this latter structure, Eκ+ρB(H)≅OX(ρ)⊗pα†N. Here pα† is ordinary differential inverse image, with local underlying sheaf OP1⊠N.

Facts & Assumptions

Given: The group, subgroups, character, twisted module and finite G-module in the statement; morphisms of twisted modules intertwine both the Lie and rational group actions.

[F1]

G→G/S has Zariski-local sections and their transition maps lie in S; associated sheaves are locally O⊗H (Zariski sections of Borel and minimal-parabolic orbit maps).

[F2]

The action-algebroid PBW basis identifies its isotropy-character quotient with a TDO. Integral line-bundle tensoring shifts the character by its weight (PBW and integral line-bundle twisting for flag TDOs).

[F3]

Ordered PBW monomials identify a Verma module with U(n−)⊗Cλ (Verma modules, PBW gives an ordered monomial basis for the enveloping algebra).

[F4]

The partial TDO has isotropy character κ and its pullback has parameter κ−ρ; ordinary inverse image has the local relative OP1 factor (Partial-flag twist and local product decomposition).

Proof

1.1F1givenconstruct

The relation [gs,h]=[g,r(s)h] defines the associated sheaf by [F1]; rationality means every vector belongs to a finite-dimensional rational S-submodule, so the construction is the filtered union of the usual finite-rank associated bundles. On a torsor section it is precisely OY⊗H. A short exact sequence of twisted modules therefore becomes a short exact sequence of sheaves, since tensoring over C is exact. Equivariant morphisms give the same local maps on all charts.

2.1F1F2step 1.1algebra

Let β(A) be the infinitesimal G-action on the associated sheaf. Define an OY-linear action by γ(A)[g,h]=[g,π(Ad⁡(g−1)A)h]. The covariance hypothesis makes this independent of replacing g by gs. Differentiating covariance gives [β(A),γ(A′)]=γ([A,A′]); the representation property gives [γ(A),γ(A′)]=γ([A,A′]). Consequently a(A)=β(A)−γ(A) satisfies [a(A),f]=AY(f),[a(A),a(A′)]=a([A,A′]). At the base point, an isotropy element x∈s acts by dr(x)−π(x)=τ(x); transport gives the same isotropy relation at every point. Thus a factors through AτS. The displayed identities also show that maps in step 1.1 are differential-module maps, proving exactness of the differential functor.

3.1step 2.1algebra

The associated-bundle map for a finite G-module is [g,h⊗v]⟼[g,h]⊗gv. It respects the S relation; its inverse sends [g,h]⊗w to [g,h⊗g−1w]. Under this map β becomes βH⊗1+1⊗dV, because the G-equivariant structure on the trivial bundle has the diagonal G-action. Likewise γ becomes γH⊗1+1⊗dV: the identity g dV(Ad⁡(g−1)A) g−1=dV(A) gives its second summand. Subtraction cancels these finite-representation terms exactly. Thus a=aH⊗1, with the Leibniz rule on function coefficients, and constant vectors of V are horizontal. This proves the asserted identity as a differential-module identity, not merely as an equivariant bundle identity.

3.2F1F2F3step 2.1algebra

More generally fix an integral B-weight η and put τ=κ+ρ. On M(−τ+η) define the rational B-action by conjugating the U(g) factor and letting the highest vector have weight η. The infinitesimal action is π+τ: commuting x∈b past the enveloping factor leaves the scalar (−τ+η)(x) on the highest vector, whereas the rational action leaves η(x). Its rationality follows from the finite-dimensional adjoint filtration of U(g) and the rational character η. The highest line gives a line subbundle OX(η) of the associated sheaf. Apply the differential action to obtain Dκ⊗OXOX(η)→EτB(M(−τ+η)). Locally on a torsor section, filter both sides by the degree of the negative-root PBW monomials. On the right, γ supplies those monomials with sign −1 and β preserves the associated filtration; hence the leading map sends a degree-d tangent monomial to (−1)d times the corresponding Verma monomial. By [F2]–[F3] this is an isomorphism of symmetric tangent modules. Induction on degree therefore proves the filtered map is an isomorphism. The cases η=0,ρ are the claimed formulas.

3.3F1F4step 2.1algebra

For twisted (g,Pα)-module H of twist κ, the character κ is defined on pα because its α-coroot pairing is zero. The construction of steps 1.1 and 2.1 on Y=G/Pα gives N over AκPα=Dκ−ρα. Restriction from Pα to B identifies associated underlying sheaves G×BH=pα∗(G×PαH). In a product chart its underlying module is OP1⊠N. For a vertical vector field, its β and fiberwise γ terms on the transported H cancel, leaving only differentiation of the relative function coefficient. For base fields the same formula is the original β−γ action on N. These are precisely the ordinary inverse image action in [F4]. They also prove agreement on overlaps, since both sides use the same Pα transition and chain rule. Thus EκB(H)=pα†N.

4.1F2step 3.3algebra∎

Multiplying the restricted rational B-action by the integral character ρ adds ρ to its differential while leaving π unchanged. The associated bundle is therefore tensored by OX(ρ). By [F2] its differential twist becomes κ+ρ, so its TDO is Dκ. Combine this with step 3.3 to obtain the displayed parabolic-descent identity. Choices of bases and of local torsor sections use only the inherited Axiom of Choice; all resulting constructions and isomorphisms are canonical.

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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.

5 · Examples, counterexamples and false statements

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