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Arakawa–Suzuki Functors and Higher-Level Schur–Weyl Duality

1 · Prerequisites

2 · Summary

Objective. This page develops the Arakawa–Suzuki action of the degenerate affine Hecke algebra on tensor functors and the higher-level Schur–Weyl duality of Brundan–Kleshchev: the Casimir and place-permutation operators, the type-A pyramid good grading and finite W-algebra, the Whittaker category and Skryabin equivalence, the truncated (deformed) tensor space, the filtered double centralizer, the Schur functor on parabolic category O, the stable range and its block-idempotent corner, and the Hecke residue functors with their intertwining with category-O translation. Everything is stated over C with the Axiom of Choice carried as an explicit dependency, and the source normalizations differ from the library conventions only where recorded in the individual items.

The Hecke algebra and the Casimir action. The degenerate affine Hecke algebra fixes the degenerate affine Hecke algebra Hd with its ordered monomial basis and filtration, and Arakawa-Suzuki Casimir operators on tensor functors defines the natural operators xj=Ω0j+∑k<jPkj and si=Pi,i+1 on M⊗V⊗d, including the slN normalization yj=xj−zM/N+(N−1)/2 used by the source. The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations proves that these operators satisfy all Coxeter, commutation and affine cross relations, giving a commuting right Hd-action on M⊗V⊗d for every g-module M.

The pyramid, the finite W-algebra and Whittaker vectors. The type-A nilpotent pyramid, good grading and Whittaker character constructs the type-A pyramid good grading, the nilpotent e, the parabolic subalgebras p,m, the centralizer basis of ge and the Whittaker character χ; The type-A finite W-algebra and the Whittaker category defines the finite W-algebra W(λ) with its η-dictionary and the Whittaker category with its Whittaker-vector functor. The Vust double centralizer Vust's graded double centralizer for the type-A nilpotent centralizer is proved from the local normality Type-A nilpotent orbit closures are normal via chain varieties and covariant extension/polarization Nilpotent-orbit tensor covariants extend and polarize results, for every Jordan type and every degree. The shifted Yangian and its generators are fixed in The shifted Yangian and the pyramid generators of the type-A finite W-algebra with the PBW basis Ordered monomial PBW basis for the shifted Yangian; the loop filtration The loop filtration on the type-A finite W-algebra has associated graded U(g^e) and the Gan–Ginzburg/Skryabin inputs Gan-Ginzburg and Skryabin inputs for the type-A pyramid good grading lead to Skryabin's equivalence Skryabin's equivalence for the type-A Whittaker pair.

The cyclotomic quotient and the double centralizer. The degenerate cyclotomic Hecke algebra fixes the quotient Hd(a) with its bounded monomial basis, central blocks and trace form; The deformed tensor space for the type-A finite W-algebra defines the filtered (W(λ),Hd(a))-bimodule structure with associated graded the character-twisted Vust tensor space, whose unital operator images agree with the untwisted ones. The parabolic highest-weight truncation factors through the cyclotomic quotient computes the minimal polynomial of x1 on this tensor space for d≥1 and hence the cyclotomic factorization. The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer proves the mutual centralizers for every origin, the stable-range faithfulness, and the admissible-origin Morita progenerator statement.

The Whittaker functor and the Schur quotient. The Whittaker functor from the relevant parabolic category-O summand defines the genuine Whittaker functor V on the parabolic summand from the continuous χ-part of the dual and Whittaker vectors, and The Whittaker functor is exact and fully faithful on the required projectives proves its exactness, its values on the ground and tensor objects, full faithfulness on all projectives and tiltings, and the Serre-quotient identification. The higher-level Schur-Weyl projective generator and Schur functor defines the tensor detector T and the distinct whole-summand projective generator G, the Schur functor π=Hom⁡g(T,−) and its right-exact left adjoint, with the boundaries of the left adjoint stated exactly. The higher-level Schur-Weyl endomorphism isomorphism identifies End⁡g(T)op and its components with the Hecke image, and The higher-level Schur-Weyl double centralizer and Schur quotient assembles the all-origin double centralizer, the admissible Morita equivalence and the exact Schur Serre quotient.

Stable range, residues and images. Stable range and block idempotent corner for higher-level Schur-Weyl duality fixes the stable range ql≥d and the central block corner outside it; Hecke induction and restriction functors on degenerate cyclotomic blocks defines the Hecke residue functors ei,fi with their exactness, biadjunction and duality compatibility. Schur functor images of standard, simple, projective and tilting objects identifies the images of standard, simple, projective and tilting objects and the multiplicity dictionary [S(A):D(B)]=dB,A(1), and Category-O translation intertwines residue induction and restriction proves the natural isomorphisms for residue induction and restriction in the tensor image towers, agreeing with the full cyclotomic functors on faithfully supported contents. The companion page arakawa-suzuki-functors-and-higher-level-schur-weyl-duality-examples works the smallest instances.

3 · Logical flowchart

4 · Definitions, theorems and proofs

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

The degenerate affine Hecke algebra

Definition

Work over the field C and fix an integer d≥0 (Algebras over a commutative ring, central structure maps, and algebra homomorphisms, Commutative ring). Let Fd be the free associative unital C-algebra on the d+max⁡(d−1,0) symbols x1,…,xd,s1,…,sd−1 (for d=0 there is only the unit; for d=1 only x1), with its word basis and universal property (The free associative R-algebra on a set and descent of relations), and let Id⊴Fd be the two-sided ideal (Left, right and two-sided ideals, The ideal generated by a subset and principal ideals) generated by the following elements:

  • xixj−xjxi for all 1≤i,j≤d;
  • si2−1 for 1≤i≤d−1;
  • sisi+1si−si+1sisi+1 for 1≤i≤d−2;
  • sisj−sjsi for 1≤i,j≤d−1 with ∣i−j∣>1;
  • sixj−xjsi for j∉{i,i+1}, sixi+1−xisi−1, and xi+1si−sixi−1, for 1≤i≤d−1 and 1≤j≤d.

The degenerate affine Hecke algebra is the quotient C-algebra Hd:=Fd/Id with unit element written 1 (For a two-sided ideal I, the additive cosets form a ring R/I with identity 1+I). We keep the symbols x1,…,xd,s1,…,sd−1 for their images, and for w∈Sd we write w for the image in Hd of any word in the si representing w; this is independent of the chosen word once the basis theorem below is proved. For d≥1 and a∈C, the notation Hd/(x1−a) means the quotient by the two-sided ideal generated by x1−a.

The verification below establishes exactly the structure of Hd used throughout this page: the ordered monomials x1r1⋯xdrdw,r1,…,rd≥0, w∈Sd, form a C-basis, so that Hd≅C[x1,…,xd]⊗CC[Sd] as a vector space with polynomial and group-algebra subalgebras (The polynomial ring R[xi:i∈I] as finitely supported coefficient families on monomials, The group ring R[G] of finitely supported formal R-linear combinations of group elements); H0=C and H1=C[x1]; for d≥1 and every a there is a unique algebra isomorphism Hd/(x1−a)≅C[Sd],xj⟼a+∑k<j(k j),si⟼(i i+1); and total polynomial degree is an algebra filtration whose associated graded is the semidirect product C[x1,…,xd]⋊C[Sd] in which si acts by swapping xi and xi+1. For d≥2, the cross relation is inhomogeneous, so it does not turn Hd into a graded algebra with deg⁡xi=1 and deg⁡si=0. For d=0 the algebra C has its degree-zero grading, and for d=1 the algebra C[x1] has its natural polynomial grading.

Facts & Assumptions

Given: An integer d≥0, the field C, the free associative C-algebra Fd on the symbols x1,…,xd,s1,…,sd−1, and the two-sided ideal Id of the Definition.

[F1]

Sd is the group of bijections of {1,…,d} under composition, with si=(i i+1); it is generated by s1,…,sd−1 subject to the Coxeter relations si2=1, sisi+1si=si+1sisi+1, sisj=sjsi for ∣i−j∣>1 (The symmetric group Sym⁡(X): the bijections of a set X under composition, The finite symmetric group Sn, one-line notation, and cycle notation, The symmetric group has the Coxeter presentation).

[F2]

C[Sd] is a unital C-algebra with C-basis {w:w∈Sd}, product induced by composition and unit the identity permutation (The group ring R[G] of finitely supported formal R-linear combinations of group elements, The group ring R[G] is a unital R-algebra with basis G, and each g∈G is a unit of R[G]).

[F3]

C[x1,…,xd] is a commutative C-algebra with C-basis the monomials x1r1⋯xdrd; it is a domain with fraction field Ω in which every nonzero polynomial is invertible; since xi≠xi+1 as polynomials, di:=xi−xi+1 is invertible in Ω (The polynomial ring R[xi:i∈I] as finitely supported coefficient families on monomials, Commutative ring, A polynomial ring over an integral domain is an integral domain, The field of fractions Frac⁡(D)=(D∖{0})−1D of an integral domain, Frac⁡(D) is a field and d↦d/1 embeds the integral domain D).

[F4]

Fd has the word basis and universal property, the two-sided ideal generated by a set E is the set of finite sums ∑sasesbs with es∈E, and a homomorphism killing E factors uniquely through Fd/(E) (The free associative R-algebra on a set and descent of relations, Left, right and two-sided ideals, The ideal generated by a subset and principal ideals, A ring homomorphism whose kernel contains a two-sided ideal factors uniquely through the quotient ring, For a two-sided ideal I, the additive cosets form a ring R/I with identity 1+I).

[F5]

For C-algebras A,B the tensor product A⊗CB is a C-algebra with (a⊗b)(a′⊗b′)=aa′⊗bb′; if (ai) and (bj) are bases, then (ai⊗bj) is a basis (The tensor product of R-algebras has multiplication (a⊗b)(a′⊗b′)=aa′⊗bb′, The elementary tensors of two bases form the product basis of the tensor product).

Proof

technique · direct

Given: The data of [F1]-[F6]: the presented algebra Hd=Fd/Id, the symmetric group Sd, the group algebra C[Sd], the polynomial algebra C[x1,…,xd] with fraction field Ω, and the tensor-product and quotient structures.

1.1F3F4given

The cases d=0,1. For d=0 there are no symbols, so F0=C and I0=0, giving H0=C. For d=1 the only symbol is x1 and the list of relations is empty; the words in x1 are 1,x1,x12,…, a C-basis of F1 by [F4], so H1 is the polynomial algebra C[x1] with basis x1r, r≥0.

1.2F1F3construct

The rational-function model. On the C-vector space Ω of [F3] let mf denote multiplication by f∈Ω, and for 1≤i<d let σi be the operator (σif)(y1,…,yd)=f(y1,…,yi+1,yi,…,yd) interchanging the i-th and (i+1)-st arguments. Put ai:=di−1∈Ω (invertible by [F3]), δi:=ai(1+σi) and Ti:=σi−δi. For a word w=si1⋯sik in the generators of Sd set σw:=σi1 ⁣∘⋯∘σik and Tw:=Ti1 ⁣⋯Tik. The operators σw are well defined by the Coxeter presentation [F1], because the σi satisfy those relations and the presentation says that any two words for the same w are related by them.

1.3F3algebragiven

The skew algebra. Let D:={∑w∈Sdmfwσw:fw∈Ω}⊆End⁡C(Ω), a C-subspace. For f,g∈Ω and u,v∈Sd the identities σumg=mσu(g)σu and σuσv=σuv hold (the first expresses the substitution action on functions, the second is word concatenation), so (mfσu)(mgσv)=mf σu(g)σuv; hence D is a subalgebra of End⁡C(Ω). The set {σw} is Ω-linearly independent: suppose ∑wfwσw=0 with fw∈Ω not all zero; multiplying the resulting identity of functions by a common denominator of the fw, we may assume fw∈C[x1,…,xd]. Fix integers N1>⋯>Nd whose consecutive gaps exceed the total degree of every fw, and order the finitely many w with fw≠0 by the lexicographic order of the vectors w⋅N:=(Nw−1(1),…,Nw−1(d)); let w be maximal and let e be the exponent of a top monomial of fw. Applying the sum to the monomial yN gives ∑w′fw′(y) yw′⋅N, because σw′yN=yw′⋅N; the vectors w′⋅N are distinct, and at the first coordinate where w′⋅N differs from w⋅N the gap exceeds the degree bound, so the monomial yw⋅N+e occurs exactly once, in the summand fwyw⋅N, with nonzero coefficient. This contradicts the vanishing of the sum, proving the claim.

1.4F1F3F4givenconstruct

Spanning of Hd by ordered monomials. We show that every element of Hd is a C-linear combination of the images of ordered monomials xrw; since words span Fd by [F4], it suffices to treat the image of a word W in the symbols. Use strong induction on the pair (n,ι) ordered lexicographically, where n is the number of x-symbols in W and ι is the number of pairs of positions (p<q) such that the p-th symbol is some si and the q-th symbol is some xj. If n=0, then W is a word in the si; by the Coxeter presentation [F1] the subalgebra generated by the si is spanned by the images of the elements w∈Sd, so the claim holds. If n>0 and every x-symbol precedes every s-symbol in W, then W is of the form (word in x's)(word in s's), and the claim follows from commutativity of the x's and the case n=0. Otherwise W=W1sixjW2 with adjacent symbols; use sixi+1=xisi+1 if j=i+1, sixi=xi+1si−1 if j=i (the relation xi+1si=sixi+1 solved for sixi), and sixj=xjsi if j∉{i,i+1}. In every case W≡W1xj′siW2±W1W2, where the first word has the same n and one fewer (s,x)-inversion pair, while the second has n−1 x-symbols; both fall under the induction hypothesis. Hence the images of ordered monomials span Hd.

1.5F1F2algebra

Jucys-Murphy elements. For 1≤j≤d put Jj:=∑k<j(k j)∈C[Sd], so J1=0. Then (i) JiJj=JjJi for all i,j; (ii) siJj=Jjsi for j∉{i,i+1}; and (iii) siJi+1=Jisi+1. For (i) with i<j write Ωm:=∑1≤k<l≤m(k l) for the sum of all transpositions in Sm; Ωm is central in C[Sm] because conjugation permutes the transpositions, and Jm=Ωm−Ωm−1. Since Ji∈C[Si]⊆C[Sm−1]⊂C[Sm] for i<m, centrality of Ωm in C[Sm] and of Ωm−1 in C[Sm−1] gives [Ji,Jm]=[Ji,Ωm]−[Ji,Ωm−1]=0. For (ii), conjugation by si sends each transposition (k j) to (si(k) si(j)); if j<i both entries are fixed, and if j>i+1 the sum over k<j contains the pairs with k=i and k=i+1, whose images are interchanged, so the sum is preserved. For (iii), conjugation sends (k i+1) to (k i) for k<i and fixes (i i+1), so siJi+1si=Ji+si; multiplying on the right by si and using si2=1 gives (iii).

2.1F1F4algebra

The model satisfies the relations. Since σimai=mσi(ai)σi=m−aiσi, the operator identity (1+σi)mai=mai(1−σi) and the rules σiδi=−δi, δiσi=δi hold; hence δi2=mai(1+σi)mai(1+σi)=mai2(1−σi)(1+σi)=0 and Ti2=σi2−σiδi−δiσi+δi2=1+δi−δi+0=1. For j∉{i,i+1} both σi and δi commute with mxj, so Timxj=mxjTi. For the cross relations, use σimxi+1=mxiσi, σimxi=mxi+1σi and the two identities mxiδi−δimxi+1=1 and δimxi−mxi+1δi=1: for the first, mxiδi=maixi(1+σi) while δimxi+1=maixi+1+maixiσi, and their difference is mai(xi−xi+1)=1; the second is the same computation with the roles of xi and xi+1 interchanged. Therefore Timxi+1−mxiTi=(mxiσi−mxiσi)+(mxiδi−δimxi+1)=1 and mxi+1Ti−Timxi=1. For ∣i−j∣>1, the variables and swaps in Ti,Tj are disjoint, so they commute. For the braid relation put A=(xi−xi+1)−1, B=(xi+1−xi+2)−1, C=(xi−xi+2)−1, so AB=C(A+B). The product rule of step 1.3 expands both TiTi+1Ti and Ti+1TiTi+1 with coefficients, in the order 1,σi,σi+1,σiσi+1,σi+1σi,σiσi+1σi, equal to (−C(1+AB),BC(1−A),AC(1−B),−B(1−A)(1−C),−A(1−B)(1−C),(1−A)(1−B)(1−C)). Here A(B−C)=BC and B(A−C)=AC, both consequences of AB=C(A+B), give the two shorter-swap coefficients and the common identity coefficient. Thus the braid relation holds. Hence the assignment xi↦mxi, si↦Ti preserves all the relations of the Definition, and by the universal properties [F4] it defines an algebra homomorphism Φ ⁣:Hd→End⁡C(Ω).

2.2F1step 1.3algebra

Triangular expansion. Fix w∈Sd with a reduced word w=si1⋯sik, and put c:=∏t=1k(σi1⋯σit−1)(1−ait)≠0 in Ω, with the empty prefix acting as the identity. Every transported factor is nonzero because the prefix is a field automorphism. In the expansion of Tw=∏t((1−ait)σit−ait) by the product rule of step 1.3, the term choosing the factor (1−ait)σit for every t contributes c σw after the scalar coefficients are moved left, while every other term is mgσv with v the product of a proper subword of si1⋯sik in the induced order. If ℓ denotes the minimal number of generators needed to express a permutation, then such a proper subword J has ℓ(v)≤∣J∣<k=ℓ(w), using subadditivity of ℓ and reducedness. Collecting the expansion in the Ω-basis {σv} therefore gives Tw=c σw+∑ℓ(v)<ℓ(w)cvσv with c≠0 and cv∈Ω.

2.3F1F2F4step 1.5construct

The evaluation homomorphism. Assume d≥1. The assignment xj↦a+Jj, si↦si defines an algebra homomorphism φ ⁣:Fd→C[Sd]: the images of the x's commute by step 1.5(i); the images of the si satisfy the Coxeter relations by [F1]; and the cross relations follow from step 1.5(ii) and from si(a+Ji+1)=(a+Ji)si+1, (a+Ji+1)si=si(a+Ji)+1, which are step 1.5(iii) read in both directions. Since φ(x1−a)=a+J1−a=0, the quotient universal property [F4] yields an algebra homomorphism φˉ ⁣:Hd/(x1−a)→C[Sd], which is surjective because the si generate Sd.

3.1F3step 1.3step 2.2algebra

Independence of the monomials in the model. By step 2.2 the change-of-basis matrix from {Tw} to {σw} inside D is triangular with nonzero diagonal when permutations are ordered by length, hence invertible over the field Ω; thus {Tw:w∈Sd} is an Ω-basis of D. Suppose ∑r,wcr,wmxrTw=0 in D with cr,w∈C finitely supported. Grouping by w gives ∑wPwTw=0 with Pw=∑rcr,wxr∈C[x1,…,xd]⊆Ω; Ω-independence of the Tw forces Pw=0 for every w, and linear independence of the monomials [F3] then forces cr,w=0. Hence the elements Φ(x1r1⋯xdrdw) are C-linearly independent.

4.1F2F5step 1.1step 2.1step 3.1step 1.4

Basis theorem. Let h∈Hd and write h=∑cr,wxrw using step 1.4. If h=0, applying the homomorphism Φ of step 2.1 gives ∑cr,wmxrTw=0, and step 3.1 yields cr,w=0. Hence the ordered monomials form a C-basis of Hd, and the C-linear map C[x1,…,xd]⊗CC[Sd]→Hd, f⊗w↦fw, is an isomorphism by [F5]; in particular C[x1,…,xd] and C[Sd] are subalgebras of Hd and the cross relations hold. The elementary cases H0=C, H1=C[x1] were recorded in step 1.1.

5.1F1F2step 4.1step 2.3algebra

The inverse map. Assume d≥1. In Hd the relation sixi+1=xisi+1 gives, after left multiplication by si and use of si2=1, the recursion xi+1=sixisi+si. Hence in Hd/(x1−a) one has x1≡a and inductively xj≡a+uj with uj in the subalgebra generated by the images of the si, namely u1=0 and uj+1=sjujsj+sj. By the basis theorem of step 4.1 every element of Hd is a combination of monomials xrw, and replacing each xj by a+uj expresses its image in Hd/(x1−a) as an element of the image of the subalgebra generated by the si; by [F1] and [F2] that image is the C-span of {w:w∈Sd}. Therefore the canonical map ρ ⁣:C[Sd]→Hd/(x1−a), w↦w+(x1−a), has image equal to the whole quotient, and it is injective because φˉ∘ρ=id⁡C[Sd] by construction; hence ρ is an isomorphism. Under it xj corresponds to a+uj, and φˉ(a+uj)=a+Jj by step 2.3, so φˉ(xj)=a+∑k<j(k j); in particular x1 corresponds to the scalar a, while for j≥2 the image is not the scalar a. The specified images of both the xj and the si determine the homomorphism uniquely because these elements generate the quotient.

5.2F4step 1.4step 4.1

The degree filtration. For k≥0 let Fk⊆Hd be the image of the C-span of all words in the symbols containing at most k of the symbols x1,…,xd. Steps 1.4 and 4.1 identify Fk with the span of the monomials xrw with ∣r∣≤k. The substitution rules of step 1.4 replace an adjacent pair sixj by terms containing at most one x-symbol each, so a product of a word with k x-symbols and a word with m x-symbols rewrites into words with at most k+m x-symbols; hence FkFm⊆Fk+m and (Fk)k≥0 is an algebra filtration with 1∈F0.

6.1F2F5step 4.1step 5.2algebra

The associated graded is a semidirect product. Let S:=C[x1,…,xd]⋊C[Sd] be the algebra with C-basis xrw and product xrw⋅xr′w′=xr+w⋅r′ww′, where (w⋅r′)j=rw−1(j)′; equivalently, S is generated by the symbols xi and w subject to the relations obtained from those of Hd by deleting the inhomogeneous term 1 from both cross relations, i.e. sixi+1=xisi and xi+1si=sixi. In gr Hd the defining relations of Hd project to these relations: the commutativity, Coxeter and distant-commutation relations are homogeneous of the stated degrees, while the two cross relations have the form (degree 1 element) =1 (degree 0 element), so their degree-1 parts are exactly sixi+1=xisi and xi+1si=sixi. Consequently there is a surjective graded algebra homomorphism S→gr Hd sending xi and w to the symbols of xi and w. In degree k both sides are C-spanned by the symbols xrw with ∣r∣=k: these form a spanning set of grkHd by step 5.2 together with the basis theorem of step 4.1, and they form the basis of the degree-k part of S by construction; a surjection between C-vector spaces with a spanning set of the same finite cardinality as a basis of the target is an isomorphism. Hence gr Hd≅S in every degree, and the associated graded is the semidirect product C[x1,…,xd]⋊C[Sd] in which si swaps xi and xi+1, as claimed.

7.1F6step 1.1step 5.2∎

Polynomial grading boundaries. For d=0, step 1.1 gives H0=C with its degree-zero grading; for d=1, it gives H1=C[x1] with the usual polynomial grading. For d≥2, suppose there were an algebra grading Hd=⨁k≥0Hd(k) with xi in degree 1 and si in degree 0. Then the relation sixi+1−xisi=1 would have its left-hand side in degree 1 and its right-hand side in degree 0, forcing 1=0, which is impossible. Hence for d≥2 the polynomial-degree filtration of step 5.2 does not arise from that generator grading; its cross relation is inhomogeneous.

Remarks

  • The filtration of step 5.2 is the polynomial-degree filtration, in which xi has degree 1 and si degree 0 and the associated graded is commutative in the polynomial part and is noncommutative overall for d≥2; it is the filtration used for the cyclotomic quotients later on this page.

  • The Arakawa-Suzuki generators yj used in the tensor constructions on this page are not the xj of this presentation: on a tensor module they differ by the central endomorphism zM/N−(N−1)/2 recalled in Arakawa-Suzuki Casimir operators on tensor functors. The presentation here is the one of [BKHL] and [BKAR]; both cross relations of the Definition are recorded because the recursion xj+1=sjxjsj+sj used in step 5.1 consumes the second one.

  • All arguments above are choice-free: the only selections made are finite (a monomial for the denominator clearing, a maximal permutation among finitely many), and no family of nonempty sets is used.

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

Type-A nilpotent orbit closures are normal via chain varieties

Statement

Assume the Axiom of Choice. Let e be a nilpotent endomorphism of a finite-dimensional complex vector space V (Nilpotent endomorphisms and their nilpotency index), let X=GL(V)⋅e‾ be the closure in End⁡C(V) of its conjugacy orbit (Classical complex matrix Lie algebras), and let ∂X=X∖GL(V)⋅e. Then C[X] is a reduced irreducible normal domain and codim⁡X∂X≥2. This holds for every Jordan type, not only the regular nilpotent cone.

The proof uses the chain schemes: if the Jordan partition of e has column lengths q1≥⋯≥qt>0, put ni=qt+⋯+qt−i+1 and Ui=Cni for 0≤i≤t. Let M=∏i=1t−1(Hom⁡(Ui,Ui+1)×Hom⁡(Ui+1,Ui)) with coordinates (Ai,Bi) and let Z⊆M be the closed subscheme B1A1=0, BiAi=Ai−1Bi−1 (2≤i<t). Then Z is a complete intersection, smooth outside a closed subset of codimension ≥2, reduced, irreducible and normal, and the invariant ring C[Z]H under H=∏i<tGL(Ui) is the coordinate ring of X via the end map θ=At−1Bt−1 when t≥2. For the empty Jordan diagram (V=0, t=0) and the single-column diagram (e=0, t=1), the chain has no variables or equations: take Z=Spec⁡C, H trivial and θ=0; the equation list above is imposed only on existing links. In these cases X is a point, its boundary is empty, and its boundary codimension is +∞.

Facts & Assumptions

Given: AC; a finite-dimensional complex vector space V of dimension N, a nilpotent e∈End⁡(V) of Jordan type η with column lengths q1≥⋯≥qt>0, q1+⋯+qt=N, the spaces Ui=Cni, ni=qt+⋯+qt−i+1, and the chain scheme Z⊆M of the Statement.

[F1]

Jordan strings: every nilpotent endomorphism has a Jordan-string basis; conjugacy classes in End⁡(V) are GL(V)-orbits, and nilpotent elements form a closed cone; for V≠0, the nilpotency index of a type-η element is the largest part η1=t; on V=0 the least-positive-exponent nilpotency index is 1 while the Jordan diagram is empty (Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings, Nilpotent endomorphisms and their nilpotency index, Classical complex matrix Lie algebras).

[F2]

Orbit dimension and boundary: dim⁡G=dim⁡Gx+dim⁡Ox for the orbit of a closed point under a connected smooth group, and Ox‾∖Ox is a union of orbits of strictly smaller dimension; an orbit of a connected group is irreducible, so its closure is irreducible (Fibre dimension and orbit dimension add to the dimension of the group).

[F3]

Nilpotent type invariants: for a nilpotent x of type μ, rank⁡xk=∑imax⁡(μi−k,0)=N−∑j≤kμj′; the conditions rank⁡xk≤rank⁡ek for all k are equivalent to μ⊴η (dominance of partitions, equivalently μ′⊵η′); and dim⁡Oμ=N2−∑i(2i−1)μi=N2−∑j(μj′)2. To compute the stabilizer dimension, each string-pair homomorphism is determined by a top-vector image killed by the source string length, giving min⁡(μi,μj) parameters; summing gives ∑j(μj′)2. Counting that same sum rowwise gives ∑i(2i−1)μi (Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings, Fibre dimension and orbit dimension add to the dimension of the group, Nilpotent endomorphisms and their nilpotency index).

[F4]

Jacobian criterion for A=P/I: at a closed point m, Am is regular iff rank⁡J(m)=n−dim⁡Am. Krull's height theorem: every minimal prime over an ideal generated by c elements has height at most c. Cohen-Macaulay: a quotient of a polynomial ring by a regular sequence is Cohen-Macaulay; a Cohen-Macaulay ring satisfies (Sj) for all j; homogeneous localization detects injectivity of graded maps; and a finitely generated module over a local Cohen-Macaulay ring whose parameter system has length equal to the dimension satisfies the parameter theorem (Jacobian rank detects regularity at closed points, Krull's height theorem, Parameters and regular sequences in Cohen--Macaulay modules, Polynomial extensions of Cohen--Macaulay rings, Regular quotients and Cohen--Macaulayness).

[F5]

Serre conditions: a Noetherian ring is reduced iff it satisfies (R0) and (S1), and normal iff it satisfies (R1) and (S2) (serre r zero s one characterises reducedness, serre normality criterion).

[F6]

Invariants: finite-dimensional rational GLn(C)-modules are completely reducible, and the GL(U)-invariants of tensor powers of U and U∗ are the permutation contractions (Schur-Weyl double centralizer); invariant vectors of rational quotients lift to invariant vectors (Weyl's complete reducibility theorem, The Schur-Weyl mutual centralizer theorem on tensor powers).

Proof

technique · direct

Given: AC, the nilpotent endomorphism e, its Jordan columns q1≥⋯≥qt>0, and the chain scheme and end map of the Statement, including its empty-chain conventions.

1.1givenalgebra

Empty chains. If V=0, take t=0; if e=0 on a nonzero space, its Jordan diagram has a single column and t=1. In either case there are no chain variables or equations, Z=Spec⁡C, H is trivial and θ=0. Its image is the point orbit closure, its coordinate ring is a normal domain, and the empty equation sequence is regular. The boundary is empty and has codimension +∞. All conclusions follow in these cases. Henceforth t≥2.

1.2F1F3F4constructalgebra

The open chain locus. Put c=∑i<tni2 and D=2∑i<tnini+1−c. The differential of the chain equations is YiAi+BiXi−Xi−1Bi−1−Ai−1Yi−1, with the index-zero terms zero. If each Ai is injective or Bi is surjective, these equations can be solved successively for any prescribed right-hand sides: use a left inverse of Ai to choose Yi, or a right inverse of Bi to choose Xi, after the preceding pair is fixed. Thus the open locus Z∘ with this condition is smooth of dimension D by [F4]. It is nonempty: use Ui=im⁡et−i, inclusions Ai, and restrictions Bi=e∣Ui+1, transported to the fixed spaces. These maps satisfy the equations and have end map e.

1.3F1F2algebraconstruct

Alternating strings and their stabilizers. For a nilpotent pair A:U→W, B:W→U, the odd operator T on U⊕W with these components has a homogeneous Jordan-string decomposition: kernels and images of its powers are graded, so the complements in the Jordan construction may be chosen homogeneous. Every string alternates letters a from U and b from W. Removing all b letters gives the Jordan rows of BA, and removing all a letters gives those of AB. The ranks of alternating composites recover the numbers of strings of each length and starting letter, so a diagram determines one pair orbit and there are finitely many diagrams in fixed dimensions. The pair stabilizer is the unit group of its even endomorphism algebra, an open subset of a vector space and hence smooth and irreducible. On a string A kills exactly a terminal a and B misses exactly an initial a; consequently A is injective iff every string ends in b, and B is surjective iff every string begins in b.

1.4F3algebra

Even orbit drops. Distinct dominated types have strictly smaller orbit dimension. One can move from a dominating partition to a dominated one by repeatedly moving a box from an earlier row to a later allowable row: choose an excess row and a subsequent deficit row, taking the last row of the source plateau and the first allowed destination to preserve the partition inequalities, and repeat until the target is reached. A move from row i to row j>i increases ∑r(2r−1)μr by 2(j−i) and therefore decreases the orbit dimension by that positive even number. Each allowable unit move from row lengths a,b with a≥b+2 is realized by a one-parameter degeneration. On chains u1,…,ua−1 and v1,…,vb+1 of the destination type, keep the usual lowering maps except send vb+1 to vb+zua−1, with v0=0. At z=0 the type is (a−1,b+1); for z≠0 the ranks of powers are those of (a,b) (the chain generated by vb+1 has length a, and the remaining chain has length b). Keeping other strings fixed proves that dominated types belong to the top orbit closure. Hence a drop of exactly two consists of one box moved to the next row; any other drop is at least four. Equivalently, parity also follows from ∑j(μj′)2≡∑jμj′=N(mod2) for the total sum; individual summands in a difference of square sums need not be even.

2.1F1F2F3step 1.3algebra

The pair-orbit dimension. Write m=dim⁡U, n=dim⁡W, and let E,O be the dimensions of the even and odd centralizers of T. A homomorphism between Jordan strings of lengths L,L′ has min⁡(L,L′) possible shifts. Counting the parity of those shifts, odd strings of the same endpoint type contribute +1 to the even-minus-odd count, and odd strings of opposite type contribute −1; the two opposite Hom directions for an odd/even pair cancel, and even/even pairs contribute zero. Summing gives E−O=(m−n)2, because the difference between the numbers of odd a-type and odd b-type strings is m−n. The pair orbit therefore has dimension m2+n2−E=12((m+n)2−E−O), half the dimension of the ordinary orbit of T. If a string has rj letters a and sj letters b, then min⁡(rj+sj,rk+sk)=min⁡(rj,rk)+min⁡(sj,sk) except for equal odd lengths with opposite endpoint types, where the left side is larger by one. Let al,bl count the odd strings of length l beginning with the two respective letters, and put Δ=∑l oddalbl. Writing CBA and CAB for the ordinary conjugacy orbits, the ordinary Jordan centralizer counts now give dim⁡O(A,B)=mn+12(dim⁡CBA+dim⁡CAB)−Δ. This is a dimension identity for the orbit, not for the full matrix space minus the pair orbit.

3.1F2step 1.3step 2.1algebra

Chain strata. Stratify Z by its compatible alternating-string diagrams at every link. Compatibility means that the b-diagram of one link equals the a-diagram of the next. These are finitely many locally closed strata. For a link A:U→W, B:W→U, projection of its pair orbit to the orbit of BA has fiber (ZGL(U)(BA)×GL(W))/G(A,B); projection to the orbit of AB instead has fiber (GL(U)×ZGL(W)(AB))/G(A,B). Indeed the numerator is the stabilizer of the specified endomorphism in the full acting group, and the denominator is the pair stabilizer. These are smooth homogeneous fibrations. Each numerator is connected and smooth, being a product of unit groups of finite-dimensional endomorphism algebras, and the pair stabilizer is smooth by step 1.3; hence the fibers are smooth and irreducible. Iterating these fibrations proves each nonempty chain stratum Zδ smooth and irreducible. The dimension at each fiber-product step is the preceding dimension plus the pair-orbit dimension minus the shared Jordan-orbit dimension. The intermediate orbit dimensions cancel in the formula of step 2.1, giving dim⁡Zδ=∑i<tnini+1+12dim⁡Cσ−∑i<tΔi, where σ is the type of its final end map.

4.1F3step 1.3step 3.1algebra

Dominance and the top stratum. The chain equations make θk factor through Ut−k, so rank⁡θk≤nt−k and θt=0. Thus its type σ is dominated by η by [F3]. For a b-diagram σ, every row must first be filled internally by alternating a letters; this requires exactly ∣σ∣−ℓ(σ) letters, the size of the diagram obtained by deleting its first column. Over the top diagram η, this equals nt−1, leaving no extra letters: every string starts and ends in b and the lower diagram is exactly the first-column deletion of η. Repeat down the chain. There is exactly one top stratum; it has both maximal-rank maps at every link, lies in Z∘, and has every Δi=0. Finally, expanding qj=nt−j+1−nt−j gives 12dim⁡Cη=∑i<tnini+1−∑i<tni2, so its dimension is D.

5.1step 3.1step 4.1step 1.4algebra

Drops of at least four. By the stratum formula and the nonnegativity of all Δi, a final orbit drop of at least four gives dim⁡Zδ≤∑nini+1+12(dim⁡Cη−4)=D−2. Every non-top stratum has dimension at most D−1. This latter estimate establishes uniqueness of the dense top stratum but does not assert that every non-top stratum has codimension two: some are smooth divisors inside Z∘.

6.1step 1.3step 3.1step 4.1step 1.4step 5.1algebra

Drops of two and the nonsmooth-locus bound. Suppose σ is obtained from η by moving a box to the next row. Let η′ and σ′ denote first-column deletions and let m=∣η′∣, m′=∣σ′∣. At the last link the available number of a letters is m and its a-diagram must be dominated by η′, since its powers factor through the shorter chain. If the receiving row was nonempty, m=m′: internal filling consumes every a, all strings begin and end in b, and the same next-row degeneration passes to the shorter chain. If a new singleton row is created, m=m′+1. After internal filling there is one extra a. It can be attached at either end of the shortened last row, at either end of the new singleton b row, or placed in a new singleton a row. No earlier row can receive it: its a-diagram would gain a box earlier than the removed last-row box and violate dominance by η′. In the first four placements one map is maximal rank; the lower diagram is either η′ or its next-row degeneration. In the fifth placement both maps fail maximal rank, and singleton strings of both types occur, giving Δi≥1. This remains valid when the shortened row is itself a singleton, when there can be more than one singleton b. Inducting through the shorter chain shows that either every link has a maximal-rank map and Zδ⊆Z∘, or some Δi≥1. In the latter case the dimension formula gives dim⁡Zδ≤∑nini+1+12(dim⁡Cη−2)−1=D−2. Together with step 5.1, this proves dim⁡(Z∖Z∘)≤D−2.

7.1F4F5step 1.2step 4.1step 5.1step 6.1algebra

Complete intersection and reducedness. Every irreducible component of the scheme cut out by its c equations has dimension at least dim⁡M−c=D by [F4]. The top stratum has dimension D and all other strata have smaller dimension by step 5.1, so every component has dimension D. Thus the equation ideal has height c. Its homogeneous generators form a regular sequence in the polynomial ring: at the homogeneous maximal ideal, every prefix of length k has height at least k, since adjoining the remaining c−k equations raises height by at most c−k; the opposite inequality is Krull's bound. Complete the generators to a system of parameters and apply the Cohen-Macaulay parameter theorem in [F4]. Homogeneous localization detects a kernel in a multiplication map, so regularity is global. The quotient is Cohen-Macaulay, hence satisfies S1 and S2. Every component meets the smooth open Z∘ by step 6.1, so it satisfies R0; [F5] implies reducedness.

8.1F5step 3.1step 4.1step 5.1step 6.1step 7.1algebra

Irreducibility and normality of the chain. The unique top stratum is irreducible. Its closure contains every component: otherwise a component of dimension D would have a nonempty open subset outside that closure, contained in a finite union of strata of dimensions at most D−1, which is impossible. Thus the reduced chain ring is a domain. Its singular locus is contained in Z∖Z∘, of codimension at least two by step 6.1, so it satisfies R1; it satisfies S2 by step 7.1. Serre's criterion [F5] gives normality.

9.1F1F3F6step 1.2step 4.1step 8.1algebra

The invariant quotient. For one pair A:U→W, B:W→U, invariants under GL(U) are generated by entries of AB: the scalar matrices force equal polynomial degrees in A,B, polarization turns a bihomogeneous invariant into a mixed tensor invariant, and [F6] expresses it as permutation contractions. Each contraction is a product of entries of AB, with possible cyclic traces also polynomials in those entries. For rational finite-dimensional GL(U) modules, the central scalar torus splits the space into integer weight spaces. On each weight space apply the semisimple Lie algebra complete-reducibility theorem [F6] to sl(U); an invariant complement then respects the center as well. It respects the group because elementary unipotents and diagonal matrices generate GL(U). Thus rational quotient invariants lift by complete reducibility in bounded polynomial degree, so the same description applies to a stable closed subscheme with its induced relations. Eliminate vertices in order. At the first vertex the invariant generators are A1B1 and the remaining variables; the chain equation replaces A1B1 by B2A2. The quotient is consequently the graph over the remaining variables with the induced rank and nilpotency relations, and eliminating the next vertex applies the same one-pair calculation. Repeating leaves precisely the entries of θ. Thus C[Z]H is generated by those entries, and is the coordinate ring of the closure of θ(Z). The rank bounds of step 4.1 put the image in the orbit closure of e, while the inclusion/restriction construction of step 1.2, applied to every conjugate of e, puts its full orbit in the image. Hence that closure is X and C[Z]H≅C[X].

10.1F2F3step 1.1step 1.4step 8.1step 9.1algebra∎

Normality and boundary of the orbit closure. An element of Frac⁡(C[Z]H) integral over C[Z]H is also integral over the normal domain C[Z], hence belongs to it. Being a fraction of invariant elements it is fixed by H, so it belongs to C[Z]H; no equality between the full invariant fraction field and the fraction field of the invariant ring is needed. Therefore C[X] is a normal domain, reduced and irreducible. The finitely many boundary nilpotent orbits have positive even dimension drops by step 1.4, so their union has codimension at least two. The point cases and their empty boundary were proved in step 1.1. This proves all chain and orbit conclusions.

Remarks

  • The chain scheme Z parametrizes compatible alternating-string data: its smooth open part dominates the conjugacy orbit of e through the end map θ, and the invariant quotient collapses the chain data to the orbit closure. No rational-singularity or Hochster-Roberts input is used.

  • The nonsmooth-locus estimate of step 6.1 is the ab-string computation of the source: the strata are read off from alternating letter strings, whose graded Hom dimension counts give the correction terms Δi. Non-top strata may be smooth divisors; it is the complement of Z∘ that has codimension at least two. The singleton-string case is retained in the five-placement induction.

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Arakawa-Suzuki Casimir operators on tensor functors

Definition

Work over C (Classical complex matrix Lie algebras, Algebras over a commutative ring, central structure maps, and algebra homomorphisms). Fix N≥1, let g=glN(C) with its matrix units Eij and the trace form B(X,Y)=tr⁡(XY), which is symmetric, nondegenerate and invariant (Trace forms are symmetric and invariant), and let z:=∑i=1NEii∈g be the central element (the identity matrix). The dual basis of (Eij) under B is (Eji), so the invariant Casimir tensor is Ω=∑i,j=1NEij⊗Eji∈U(g)⊗U(g), Its action on a tensor product of two g-modules commutes with the diagonal action, as computed in [F2]. Multiplying its two factors gives the central Casimir element of Casimir operator relative to an invariant form.

Let M be a g-module and V=CN the natural module (Representations of Lie algebras). On the tensor product M⊗V⊗d (The tensor product M⊗RN from the additive group underlying the free Z-module on M×N, elementary tensors, and finite tensor sums, Associativity of tensor products for compatible bimodules) label the factors 0,1,…,d, with factor 0 equal to M. For 0≤a≠b≤d let Ωab denote the operator obtained by applying Ω in the two labelled factors, and for distinct 1≤a,b≤d let Pab denote the operator that interchanges the two labelled factors (the flip of V⊗V on two V-factors). Define, for 1≤j≤d and 1≤i≤d−1, xj:=Ω0j+∑k<jPkj,si:=Pi,i+1. Finally put Ωsl:=Ω−1Nz⊗z and define the Arakawa-Suzuki normalized operators yj:=xj−1NzM+N−12, where zM denotes the endomorphism of M⊗V⊗d given by the action of z on the factor M. This is a central endomorphism, and is a scalar only when z acts scalarly on M.

The verification below records the properties of these operators used on this page: Ω acts on V⊗V as the flip; the operators xj and si are natural in M and commute with the g-action; the recursion xj+1=sjxjsj+sj holds; Ωsl is the Casimir of slN relative to the restricted trace form; and the operators yj are exactly the source operators of [AS, (2.2.2)]. For d=0 the family (xj) is empty; for the trivial module M=C one has Ω0j=0, so xj=∑k<jPkj and x1=0.

Facts & Assumptions

Given: N≥1, g=glN(C) with matrix units Eij and trace form B, the central element z=∑iEii, a g-module M, the natural module V=CN, and d≥0.

[F1]

Matrix units multiply by EijEkl=δjkEil, B(Eij,Ekl)=δilδjk, and B is symmetric and invariant; z is central, so its action zM on any module is an endomorphism commuting with the action (Classical complex matrix Lie algebras, Trace forms are symmetric and invariant).

[F2]

The Casimir tensor Ω=∑ijEij⊗Eji∈U(g)⊗U(g) is independent of dual bases and invariant under the diagonal adjoint action: [X⊗1+1⊗X,Ω]=0 for every X∈g. Indeed, for X=Eab the matrix-unit relations give the cancelling sum ∑jEaj⊗Ejb−∑iEib⊗Eai+∑iEib⊗Eai−∑jEaj⊗Ejb=0, and linearity gives every X. Therefore its action on a tensor product of g-modules is a g-intertwiner. Module actions extend uniquely to U(g) (Casimir operator relative to an invariant form, The Casimir operator is basis-independent and intertwining, The quadratic Casimir element is independent of the choice of dual bases, Universal enveloping algebra).

[F4]

The degenerate affine Hecke algebra Hd is presented by x1,…,xd,s1,…,sd−1 with the Coxeter relations and the cross relations sixi+1=xisi+1, xi+1si=sixi+1; the recursion xj+1=sjxjsj+sj holds in Hd (The degenerate affine Hecke algebra).

[F5]

The source operators: [AS, (2.2.1)-(2.2.2)] define, on X⊗V⊗ℓ for the slN Casimir, the transposition operators sij=Ωij+1/N and the generators yi=Ω0i+∑1≤j<i(Ωji+1/N)+(N−1)/2.

Proof

technique · direct

Given: The data of [F1]-[F5] and the operators of the Definition.

1.1F1F3algebra

Ω is the flip on V⊗V. On the tensor basis, Ω(va⊗vb)=∑i,j(Eijva)⊗(Ejivb)=∑i,jδjavi⊗δibvj=vb⊗va=P01(va⊗vb) by [F1]. Consequently Ωab=Pab whenever the two labelled factors a,b are both natural factors; in particular Ωj,j+1=sj on the V-factors.

1.2F2F3algebra

Naturality and commutation with g. For a g-module map f ⁣:M→M′, the map f⊗1⊗d intertwines xj and si: it plainly intertwines the place permutations Pab, and it intertwines Ω0j because the Casimir operator on a tensor product of modules is an intertwiner by [F2]. For the same reason each xj and si commutes with the g-action on M⊗V⊗d, the action on the V-factors being the natural one.

1.3F1F2algebra

The slN Casimir. The trace form restricts to a nondegenerate form on slN: slN={X∈g:B(X,z)=0} because B(X,z)=tr⁡(X) and B(z,z)=N≠0. Hence Ωsl=Ω−1Nz⊗z is the inverse tensor of B∣slN: for X∈slN, contracting the second factor of Ω with X gives ∑ijB(X,Eji)Eij=X, while contracting the second factor of z⊗z with X gives B(X,z)z=tr⁡(X)z=0; so contraction with Ωsl also returns X, and by [F2] the dual tensor is unique. Thus Ωsl is the slN-Casimir for the restricted trace form.

2.1F4step 1.1algebra

The recursion. Since sj=Pj,j+1 and Pab are involutions with PabΩabPab=Ωab and conjugation by Pj,j+1 replaces the label j by j+1 in every operator supported on labels {0,1,…,j}, one has sjΩ0jsj=Ω0,j+1, sjPkjsj=Pk,j+1 for k<j, and sjsj=1. Hence sjxjsj+sj=Ω0,j+1+∑k<jPk,j+1+Pj,j+1=xj+1, using xj+1=Ω0,j+1+∑k<j+1Pk,j+1 and Pj,j+1=sj. Thus the operators satisfy the recursion of [F4]. The remaining Hecke relations require the independent commutator check in The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations ↗.

2.2F5step 1.1step 1.3algebra

The source dictionary. Let Ω now denote the slN-Casimir in the formula (2.2.1) of the source [F5], so that on two natural factors Ωij=Pij−1/N by steps 1.1 and 1.3, i.e. Pij=Ωij+1/N, which is exactly [AS, (2.2.1)]. On M⊗V⊗d the library glN-Casimir satisfies Ω0jglN=Ω0jsl+zM/N (the extra term 1Nz⊗z acts on factor 0 as zM/N and on factor j as the identity on V), while ΩkjglN=Ωkjsl+1/N for two natural factors; therefore yj=xj−1NzM+N−12=Ω0jsl+∑k<j(Ωkjsl+1N)+N−12, which is precisely the source formula (2.2.2) in [F5].

3.1F1F3given∎

Special cases. For d=0 there are no labels j≥1, so the family (xj) and (si) is empty and the Definition records only the module M; the recursion and the dictionary are vacuous. For the trivial module M=C the action of g is zero, so Ω0j=0 and zM=0; hence xj=∑k<jPkj, with the empty sum x1=0.

Remarks

  • The operators xj are the universal (trace-form) Casimir operators; the operators yj differ from them by the central endomorphism zM/N−(N−1)/2 recorded in the Definition, and this dictionary is the one used whenever the source normalization [AS] is compared with the tensor-space computations of this page.

  • The sign of the shift in the recursion is fixed by the cross relation sixi+1=xisi+1 of The degenerate affine Hecke algebra: the computation of step 2.1 gives xj+1=sjxjsj+sj, whose right-hand side contains +sj, not −sj.

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Nilpotent-orbit tensor covariants extend and polarize

Statement

Assume the Axiom of Choice. Let e be a nilpotent endomorphism of a finite-dimensional complex vector space V, let Ge={g∈GL(V):geg−1=e} be its centralizer, and let d≥0.

  1. Every Ge-fixed endomorphism B∈End⁡C(V⊗d) is the value at e of a GL(V)-equivariant polynomial map Φ ⁣:End⁡(V)→End⁡(V⊗d) (polynomial in the matrix entries of the input, with Φ(gXg−1)=(g⊗d)Φ(X)(g−1)⊗d).
  2. Every such equivariant polynomial map is a finite sum Φ(X)=∑hch σh(Xh1⊗⋯⊗Xhd) with hi≥0, where σh is a place permutation of the d tensor factors and ch is an invariant scalar polynomial in X (a polynomial in the traces tr⁡(Xk)).

The extension in (1) is proved by Hartogs lifting on the normal codimension-≥2 orbit closure; the structure in (2) is proved by polarization and the Schur-Weyl description of tensor invariants, not by importing a first-fundamental-theorem for the full matrix algebra.

Facts & Assumptions

Given: AC; a nilpotent e in End⁡(V) with dim⁡V=N<∞ and largest Jordan block l when V≠0, an integer d≥0, the orbit closure X=GL(V)⋅e‾ with dense orbit O=GL(V)⋅e, and the centralizer Ge.

[F1]

X is the spectrum of a reduced irreducible normal domain A=C[X], and O is its dense open orbit; Ge is the unit group of the full finite-dimensional associative centralizer algebra Ce=End⁡C[e](V)={b:be=eb}. Its units are exactly {b∈Ce:det⁡b≠0}: if b commutes with e and is invertible on V, its inverse also commutes with e. This is a nonempty open subset of the affine vector space Ce, containing the identity, so Ge is smooth, irreducible and connected; no product-of-matrix-algebras identification is needed (Type-A nilpotent orbit closures are normal via chain varieties, Nilpotent endomorphisms and their nilpotency index, Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings).

[F2]

Hartogs lemma for a normal S2 domain A: a fraction f∈Frac⁡(A) regular in codimension 1 lies in A. More precisely, if f is regular off a closed subset of codimension ≥2, then f∈A. Proof ingredients: set J={a∈A:af∈A}; Jp=Ap for every height-one prime; if 0≠a∈J then every associated prime of A/(a) has height 1 by the normal S2 property and the depth criterion; prime avoidance produces b∈J avoiding those primes; from b(af)=a(bf) and regularity of b modulo a one gets af∈aA, and cancellation gives f∈A (normal domain implies s two, The local depth-zero associated-prime criterion, Associated primes commute with localization for finite modules, Depth drops by one after quotienting by a regular element, Zero divisors on a module over a Noetherian ring are the union of its associated primes, An ideal contained in a finite union of prime ideals lies in one of them).

[F3]

Weyl complete reducibility applies to finite-dimensional sl(V)-modules in characteristic zero; the reduction in step 4.1 gives the required GL(V)-invariant lifting for the polynomial-map spaces used here. Invariant tensors in mixed tensor powers of V are spanned by permutation contractions (Weyl's complete reducibility theorem, The Schur-Weyl mutual centralizer theorem on tensor powers).

[F4]

The trace form tr⁡(XY) on End⁡(V) is symmetric and nondegenerate, and tensor bases identify End⁡(V⊗d) with End⁡(V)⊗d (Classical complex matrix Lie algebras, The elementary tensors of two bases form the product basis of the tensor product).

Proof

technique · direct

Given: The data of [F1]-[F4]: the nilpotent e, the normal orbit closure X with dense orbit O, the connected centralizer Ge, the degree d, and a Ge-fixed B∈End⁡(V⊗d).

1.1F1constructalgebra

The zero-dimensional case. If V=0, its orbit closure is a point and its boundary is empty by [F1]. For d=0, V⊗d=C and every fixed operator is a scalar, extended by the constant polynomial map; the empty permutation and empty tensor product give the asserted normal form. For d>0, V⊗d=0 and its endomorphism space has only the zero operator, extended by the zero map; the normal form is the empty sum. Thus both assertions hold without a largest Jordan block. Henceforth V≠0, so its largest block length l exists.

1.2F1F2algebra

Hartogs lifting. Let A=C[X] and let f∈Frac⁡(A) be regular on O, hence regular off a closed subset of X∖O; since ∂X has codimension ≥2 in X by the normality lemma [F1], f is regular in codimension 1 and therefore extends to A by [F2]. Applying this coordinatewise to maps into a finite-dimensional vector space shows that every regular map O→W into a finite-dimensional vector space extends uniquely to a regular map X→W.

1.3F1constructalgebra

The equivariant map on O. Fix B∈End⁡(V⊗d)Ge and define, for g∈GL(V), F(g e g−1):=(g⊗d) B (g−1)⊗d∈End⁡(V⊗d). This is well defined: if g1eg1−1=g2eg2−1, then g2−1g1∈Ge, so (g2−1g1)⊗dB(g2−1g1)−⊗d=B by Ge-invariance, which rearranges to (g1⊗d)B(g1−1)⊗d=(g2⊗d)B(g2−1)⊗d. The map F is GL(V)-equivariant by construction: F(hXh−1)=(h⊗d)F(X)(h−1)⊗d for X∈O.

2.1F1step 1.3algebraconstruct

Regularity of F on O. The ranks of X0,X1,…,Xl−1 are constant on O. Cover O by open charts where fixed minors used to select bases of the kernels and images, their quotient complements and Jordan top vectors are nonzero. Gaussian elimination on such a chart gives a Jordan basis for X with entries regular in X. Let g(X) carry a fixed Jordan basis for e to this chosen Jordan basis for X, with the same ordered string lengths. Then g(X)eg(X)−1=X. Restricting to the open chart where the Jordan-basis determinant is nonzero makes both g(X) and g(X)−1 regular, since their entries have only the fixed nonvanishing minors and determinant as denominators. Thus X↦(g(X)⊗d)B(g(X)−1)⊗d is the map of step 1.3 and is regular on each chart. These charts cover O; on overlaps g2(X)−1g1(X)∈Ge, so the expressions agree by Ge-invariance of B. Hence F is regular on O.

3.1F2step 1.2step 2.1algebra

Extension to X. By steps 1.2 and 2.1 the map F ⁣:O→End⁡(V⊗d) is a regular equivariant map on the dense orbit; by step 1.2 it extends uniquely to a regular map F ⁣:X→End⁡(V⊗d). Since C[X]=C[End⁡(V)]/I(X) and X is an affine closed subset of the affine space End⁡(V), the coordinate functions of F are restrictions of polynomial functions on End⁡(V); fixing representatives gives a polynomial map Φ ⁣:End⁡(V)→End⁡(V⊗d) extending F.

4.1F3step 1.3step 3.1algebra

Equivariance of the polynomial lift. The extension F on X is equivariant: for every g, the two regular maps expressing equivariance agree on the dense orbit by step 1.3 and therefore on X. Let EK be the finite-dimensional rational module of polynomial maps operatornameEnd(V)ooperatornameEnd(Votimesd) of degree at most K, for KgedegPhi, with action (gcdotPsi)(Y)=gotimesdPsi(g−1Yg)(g−1)otimesd. Let IKsubsetEK consist of maps vanishing on X. Then IK is stable and the class of the lift from step 3.1 in EK/IK is invariant. Scalar matrices act trivially on EK: they conjugate neither the input nor the output. For Nge2, Weyl's theorem [F3] applied to the semisimple Lie algebra mathfraksl(V) gives an mathfraksl(V)-stable complement to IK. This complement is stable under mathrmSL(V), since elementary matrices exp(tEij) generate that group and their rational representation acts by exponentiating the differential; together with scalar matrices they generate mathrmGL(V) over mathbbC. For N=1 the whole group acts trivially, so any vector-space complement suffices. The quotient map restricted to this complement is thus a mathrmGL(V)-isomorphism and lifts the invariant class to an invariant Phi′inEK. It agrees with F on X and satisfies Phi′(e)=B, proving (1).

5.1F4step 4.1algebra

Polarization. Write Φ=∑kΦk for its homogeneous components of degree k; each Φk is equivariant. Fix k and assume for the structure argument that Φ is homogeneous of degree k. Polarize the k matrix variables X1,…,Xk of Φ and pair the output in End⁡(V⊗d) with d independent matrices Y1,…,Yd using the nondegenerate trace pairing on each tensor factor; this produces a multilinear GL(V)-invariant P(X1,…,Xk;Y1,…,Yd)∈C in (k+d) matrix arguments.

6.1F3step 5.1algebra

Tensor invariants are permutation contractions. By the Schur-Weyl description [F3], every multilinear invariant of the matrix arguments is a linear combination of contractions: each argument contributes one upper and one lower index, an invariant pairs each upper index with a lower index of another argument, and the invariant is a product over the cycles of the resulting permutation of traces of the corresponding cyclically ordered product of matrices.

7.1F4step 5.1step 6.1algebra

Covariant normal form. Depolarize in the k identical variables Xi=X and read each contraction cycle. A cycle that uses only X-arguments contributes a scalar invariant polynomial in X; a cycle that uses some Y-arguments alternates blocks of X's and single Y's, so its trace is precisely the trace pairing of Y1⊗⋯⊗Yd with a place permutation of Xh1⊗⋯⊗Xhd. By nondegeneracy of the trace pairing, the operator identity Φ(X)=∑hch(X) σh(Xh1⊗⋯⊗Xhd) follows, with hi≥0, σh a place permutation and ch a scalar invariant polynomial (a polynomial in the traces tr⁡(Xm)); summing over the homogeneous components gives assertion (2).

8.1step 7.1algebra∎

Evaluation at e. Since el=0 for the largest Jordan block length l of e, evaluating the normal form at X=e kills every term with some hi≥l; the surviving terms are place permutations applied to a tensor product of nonnegative powers eh1⊗⋯⊗ehd multiplied by the scalar invariants ch(e), which are complex constants; since tr⁡(em)=0 for every positive m, the scalar invariant polynomials satisfy ch(e)=ch(0). This gives the concrete description of the Ge-fixed endomorphisms used by the double centralizer theorem.

Remarks

  • The extension step is exactly where the normality of the orbit closure is consumed: the proof of extension uses the codimension-two Hartogs property. Omitting that input leaves the all-degree converse unproved by this argument.

  • The scalar invariant coefficients ch lie in the polynomial ring generated by the traces of powers of X; evaluating at nilpotent e gives the complex constants ch(0), independent of the chosen nilpotent orbit point.

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The type-A nilpotent pyramid, good grading and Whittaker character

Definition

Work over C. Let λ=(0≤p1≤⋯≤pn) be a partition of N≥0 with transpose q1≥⋯≥ql, where l=pn for a nonempty row list and l=0 for an empty row list. Zero-length rows have no boxes. Let g=glN(C) with matrix units ei,j in the standard basis v1,…,vN (Classical complex matrix Lie algebras). Number the boxes of the diagram of λ by 1,…,N down columns from the left, and for a box i write row(i),col(i) for its row and column, L(i) for the box immediately to its left (or ∅ if absent), and R(i) for the box immediately to its right (or ∅ if absent). Define the nilpotent endomorphism e=∑i: L(i)≠∅eL(i),i∈g,evi=vL(i), and declare deg⁡ei,j=col(j)−col(i) for all i,j, so that g=⨁r∈Zgr with gr=span⁡{ei,j:col(j)−col(i)=r}. Put p=⨁r≥0gr,h=g0,m=⨁r<0gr, and for rows 1≤i,j≤n define the shift si,j=pj−pi if i≤j and si,j=0 if i≥j, together with the centralizer elements ei,j;r=∑row(h)=i, row(k)=jcol(k)−col(h)=reh,k(si,j≤r<pj). Finally let χ ⁣:m→C be χ(x)=tr⁡(xe), where the trace is the trace of the N×N matrix.

The verification below records the properties of this data that are used throughout this page. e∈g1 has Jordan type λ; p is a parabolic subalgebra with Levi factor h≅glq1⊕⋯⊕glql and nilradical ⨁r>0gr, while m is the nilradical of the opposite parabolic; the elements ei,j;r with si,j≤r<pj form a basis of the centralizer ge={X∈g:[X,e]=0}; the box set J={(a,b)∈{1,…,N}2:col(a)≤col(b), R(b)=∅} is in bijection with K={(i,j,r):1≤i,j≤n, si,j≤r<pj} via (a,b)↦(row(a),row(b),col(b)−col(a)), and ξa,b:=∑t=0col(a)−1eLt(a),Lt(b)=erow(a),row(b);col(b)−col(a); and χ is a Lie algebra character, χ([m,m])=0. This grading is the type-A pyramid good grading in the degree-one convention: ad⁡e:gr→gr+1 is injective for r<0 and surjective for r≥0. For e≠0 it differs from the standard Dynkin grading, in which e has degree 2 rather than 1. For e=0 all boxes lie in one column or there are no boxes, and the pyramid grading and the trivial Dynkin grading both concentrate g in degree zero. If N=0, take gl0=0: the box set and both centralizer index sets are empty, e=0, p=h=m=0, and χ=0. These conventions also permit an empty row list.

Facts & Assumptions

Given: A partition λ=(0≤p1≤⋯≤pn) of N with transpose q1≥⋯≥ql, the diagram boxes with row, column, L and R data, the nilpotent e=∑eL(i),i, the grading deg⁡ei,j=col(j)−col(i) and the subspaces p,h,m, and the elements ei,j;r and χ.

[F1]

Matrix units satisfy eh,kek,l=eh,l and eh,kek′,l=0 for k≠k′, and the trace is tr⁡(eh,k)=δhk (Classical complex matrix Lie algebras).

[F2]

Jordan strings: a nilpotent endomorphism is described by its strings w,Nw,N2w,…; the Jordan type is the partition of the string lengths, and the centralizer of a nilpotent of type μ has dimension ∑h,lmin⁡(μh,μl). Indeed its string-pair block is Hom⁡C[t](C[t]/tb,C[t]/ta); the image of 1 is any vector killed by tb, a subspace of dimension min⁡(a,b) (Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings, Nilpotent endomorphisms and their nilpotency index).

[F3]

The trace form tr⁡(XY) on glN(C) is symmetric and invariant, and the degree grading is multiplicative: if x∈gr and y∈gs then xy∈gr+s, and tr⁡(x)=0 for x∈gr with r≠0 (Trace forms are symmetric and invariant, Classical complex matrix Lie algebras).

[F4]

The enveloping algebra and representations of g (Universal enveloping algebra, Representations of Lie algebras).

Proof

technique · direct

Given: The pyramid data of the Definition.

1.1F1F2F4algebra

The endomorphism e acts on the box basis by evi=vL(i) and evi=0 for boxes with L(i)=∅; hence the vi in one row form a Jordan string of length pi, because left shifts run from the rightmost box of the row to the first. Consequently e is nilpotent of Jordan type λ=(p1,…,pn), e∈g1, and the number of columns is l=pn when the row list is nonempty, with l=0 for the empty row list. Zero-length rows contribute no Jordan strings; for N=0 all box-indexed sums and vector spaces are empty or zero.

1.2F1algebra

Parabolic structure. The degree defines a Z-grading of the associative algebra: deg⁡(eh,kek′,l)=deg⁡eh,k+deg⁡ek′,l when k=k′ by [F1], and [gr,gs]⊆gr+s. Hence p=⨁r≥0gr is a subalgebra, its degree-zero part h consists of the matrices eh,k with col(h)=col(k), which is exactly the block-diagonal subalgebra with blocks of sizes q1,…,ql, so h≅glq1⊕⋯⊕glql; the strictly positive part ⨁r>0gr is a nilpotent ideal and m=⨁r<0gr is the nilradical of the opposite parabolic, with g=m⊕h⊕⨁r>0gr.

1.3F2algebra

The centralizer basis. First [e,eh,k]=eL(h),k−eh,R(k) for boxes h,k, with a term omitted when the relevant neighbour is absent (this is [e,eh,k]=∑d(eL(d),deh,k−eh,keL(d),d) and eL(d),deh,k=δd,heL(d),k, while eh,keL(d),d=δL(d),keh,d and L(d)=k holds exactly for d=R(k) in the same row). Now write ei,j;r=∑cehc,kc with hc the box of row i in column c and kc the box of row j in column c+r, the sum over c with 1≤c≤pi and 1≤c+r≤pj; here r≥si,j≥0 by the defining range, so this index set is exactly c=1,…,min⁡(pi,pj−r). Then [e,ei,j;r]=∑c(ehc−1,kc−ehc,kc+1) where a term is omitted when the neighbour does not exist; shifting the second sum by c↦c+1 and using R(kc)=kc+1 (which exists exactly when c+r<pj) shows that the two sums run over the same index set {c:c≥2, c≤min⁡(pi,pj−r)}, because for every c in the defining range one has c+r≤pj; hence the commutator is 0. The ei,j;r are linearly independent because they are sums over pairwise disjoint matrix units, and their number is ∑i,j#{r:si,j≤r<pj}=∑i,j(pj−max⁡(0,pj−pi))=∑i,jmin⁡(pi,pj), which equals dim⁡ge by [F2]. Hence they form a basis of ge.

2.1step 1.3algebra

The bijection J→K. For (a,b)∈J put i=row(a), j=row(b) and r=col(b)−col(a). Because b is rightmost, col(b)=pj; hence r=pj−col(a)≥0, r<pj because col(a)≥1, and r≥pj−pi because col(a)≤pi. Thus si,j=max⁡(0,pj−pi)≤r<pj, so the map lands in K. The triple determines b as the rightmost box of row j and a as the box of row i in column pj−r, proving injectivity. Conversely, if (i,j,r)∈K, then r<pj gives 1≤pj−r, while r≥max⁡(0,pj−pi) gives pj−r≤pi. Thus those two boxes exist, their columns satisfy col(a)≤col(b), and they give the required preimage. If either row has length zero, the index range in K is empty, consistently with the absence of such a box pair.

2.2F3step 1.2algebra

The character. For x,y∈m one has [x,y]∈[m,m]⊆g≤−2 by step 1.2, and e∈g1, so [x,y]e∈g≤−1 and tr⁡([x,y]e)=0 by [F3]. Hence χ([m,m])=0, that is, χ is a Lie algebra character on m: for x,y∈m, χ([x,y])=tr⁡([x,y]e)=0.

2.3F1F3step 1.1step 1.3algebra

The good-grading conditions. By step 1.3, the centralizer ge has a homogeneous basis ei,j;r with r≥si,j≥0, so it has no negative-degree part. The kernel of ad⁡e:gr→gr+1 is ge∩gr, hence this map is injective for r<0. The trace pairing is nondegenerate between gr and g−r: each matrix unit ea,b pairs with eb,a, and matrix units of other total degree have zero trace. Invariance gives tr⁡([e,x]y)=−tr⁡(x[e,y]), so the transpose of the map on degree r is, up to sign, ad⁡e:g−r−1→g−r. For r≥0 the latter is injective by the negative-degree result; finite-dimensional duality therefore makes the original map surjective. These are the good-grading conditions for degree-one e. They remain valid when e=0, because all nonzero spaces then have degree zero.

3.1step 1.3step 2.1algebra

The identity ξa,b=erow(a),row(b);col(b)−col(a). Left shifts of a run through the boxes of row i in columns col(a),col(a)−1,…,1, and the corresponding left shifts of b run through the boxes of row j in columns col(b),col(b)−1,…,col(b)−col(a)+1; all these exist because col(b)−col(a)+1≥1 and the shifts stop while the row i box exists. The pairs (row(h),row(k)) obtained are exactly the pairs (i,j) with column difference col(b)−col(a) and col(h) ranging over 1,…,col(a); by step 2.1 these are exactly the pairs indexing erow(a),row(b);col(b)−col(a). Hence the two finite sums coincide, and the two displayed families are the same basis of ge.

4.1F1step 1.1step 1.3step 2.3algebra∎

Dynkin normalization and the zero boundary. If e≠0, step 1.1 puts this nonzero element in pyramid degree 1, whereas the standard Dynkin grading defined by an sl2-triple has [h,e]=2e and puts it in degree 2; these two gradings therefore differ. There is no assertion that every Dynkin matrix degree is even: on Jordan strings of lengths one and two the standard h-weights are 0 and 1,−1, so matrix units between these strings have odd weights. If e=0, no row has length greater than one, since a row of length at least two contributes a distinct nonzero left-shift matrix unit. Hence all boxes lie in the first column or there are none, every matrix unit has pyramid degree zero, and the zero triple gives the trivial Dynkin grading as well. If N=0, there are no matrix units or centralizer indices; the parabolic, Levi, opposite nilradical and trace character are zero. Thus the conventions and good-grading conditions cover repeated row lengths, zero-length rows and the empty pyramid without an exclusion.

Remarks

  • The numbering of boxes down columns from the left makes each row a Jordan string of e; this is why the row lengths pi (weakly increasing) are the Jordan block sizes, while the column heights qj are the ranks' increments and index the Levi blocks of h.

  • The shift si,j=max⁡(0,pj−pi) counts the overlap min⁡(pi,pj) of the two rows i,j through the identity #{r:si,j≤r<pj}=pj−max⁡(0,pj−pi); this count is used again in the loop-mode index sets of the finite W-algebra items.

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The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations

Statement

Let N≥1, let M be a glN(C)-module, let V=CN be the natural module, and on M⊗V⊗d use the operators xj=Ω0j+∑k<jPkj and si=Pi,i+1 of Arakawa-Suzuki Casimir operators on tensor functors. Then:

  1. The operators x1,…,xd,s1,…,sd−1 commute with the g-action and are natural in M, and satisfy all the defining relations of the degenerate affine Hecke algebra The degenerate affine Hecke algebra: the Coxeter relations for the si; sixj=xjsi for j∉{i,i+1}; sixi+1=xisi+1 and xi+1si=sixi+1; and the polynomial commutation [xi,xj]=0.
  2. Consequently they define, via the generator-fixing anti-involution of the Hecke algebra, a natural right Hd-action on M⊗V⊗d commuting with the left g-action.

The commutation of the xi is an independent check: it does not follow from the braid relations of the si alone.

Facts & Assumptions

Given: N≥1, a g-module M with g=glN(C), the natural module V, d≥0, and the operators of Arakawa-Suzuki Casimir operators on tensor functors built from the trace-form Casimir Ω=∑i,jEij⊗Eji.

[F1]

The operators Pab for 1≤a≠b≤d are the place permutations of the labelled tensor factors; Pab2=1, and Pab commutes with Pcd when {a,b}∩{c,d}=∅ (Arakawa-Suzuki Casimir operators on tensor functors, Associativity of tensor products for compatible bimodules).

[F2]

On two natural factors Ωij=Pij; more generally, for any triple of factors a,b,c the element identity [Ωab,Ωac+Ωbc]=0 holds in U(g)⊗3, and [Ωab,Pcd]=0 whenever the pairs of labels are disjoint (Arakawa-Suzuki Casimir operators on tensor functors, Classical complex matrix Lie algebras).

[F3]

[Eab,Ecd]=δbcEad−δadEcb in glN(C) (Classical complex matrix Lie algebras).

[F4]

The Hecke algebra Hd is presented by the Coxeter relations for the si and the cross relations sixi+1=xisi+1, xi+1si=sixi+1, together with xixj=xjxi; the generator-fixing anti-involution ω of Hd is the anti-automorphism fixing all generators, and a left action ρ of Hd defines a right action by e⋅u=ρ(ω(u))e (The degenerate affine Hecke algebra).

[F5]

The Casimir operator acts as an intertwiner and commutes with the g-action; place permutations of natural factors also commute with the g-action because the comultiplication is cocommutative (The Casimir operator is basis-independent and intertwining, Representations of Lie algebras).

Proof

technique · direct

Given: The operators xj=Ω0j+∑k<jPkj and si=Pi,i+1 on M⊗V⊗d, and the identities of [F1]-[F5].

1.1F2F3algebra

The infinitesimal braid identities. For distinct labels a,b,c one has [Ωab,Ωac+Ωbc]=0: expanding Ω=∑Euv⊗Evu and using [F3], the double commutator sum splits into terms [Euv,Exy]⊗Evu⊗Eyx and Euv⊗[Evu,Exy]⊗Eyx, and the two resulting sums cancel term by term after relabelling; equivalently, this is the identity [Ω12,Ω13+Ω23]=0 in U(g)⊗3, which is the derivative of the invariance of Ω under the diagonal adjoint action. Consequently [Ωab,Ωac]=−[Ωab,Ωbc]=[Ωac,Ωbc]. In particular, for three natural factors this is the identity [Pab,Pac]+[Pab,Pbc]=0 for the flips.

1.2F1algebra

The Coxeter relations for si. si=Pi,i+1 is an involution; sisj=sjsi for ∣i−j∣>1 because the pairs of interchanged labels are disjoint; and sisi+1si=si+1sisi+1 because both sides are the permutation operator inducing the same permutation of the three labelled factors.

2.1F1step 1.1algebra

Cross relations. Conjugation by si=Pi,i+1 interchanges the labels i and i+1 in any operator supported on those factors, so siΩ0,i+1=Ω0isi and siPk,i+1=Pkisi for k<i. Therefore sixi+1=siΩ0,i+1+∑k<isiPk,i+1+siPi,i+1=Ω0isi+∑k<iPkisi+1=xisi+1, and symmetrically xi+1si=sixi+1. For j<i, all labels in xj are disjoint from {i,i+1}, so si commutes with every summand. For j>i+1, Ω0j and the terms Pkj with k∉{i,i+1} commute with si, while conjugation by si interchanges Pij and Pi+1,j. Their sum is invariant, so again sixj=xjsi; the two overlapping summands need not commute individually.

2.2F1F2step 1.1algebra

Polynomial commutation. Fix i<j. Since xi=Ω0i+∑k<iPki and xj=Ω0j+∑l<jPlj, the commutator is [Ω0i,Ω0j]+∑l<j[Ω0i,Plj]+∑k<i[Pki,Ω0j]+∑k<i∑l<j[Pki,Plj]. The second sum reduces to the single term [Ω0i,Pij] (all other Plj are disjoint from the labels 0,i), and the third sum vanishes (all pairs {k,i}, {0,j} are disjoint since k<i<j). In the fourth sum only the terms with k=l or l=i can fail to vanish, so it equals ∑k<i([Pki,Pkj]+[Pki,Pij]). Hence [xi,xj]=([Ω0i,Ω0j]+[Ω0i,Pij])+∑k<i([Pki,Pkj]+[Pki,Pij]). The first bracket vanishes by step 1.1 with a=0, b=i, c=j together with Ωij=Pij; each summand of the second bracket vanishes by step 1.1 for the three distinct labels k,i,j. Therefore [xi,xj]=0.

3.1F4F5step 1.2step 2.1step 2.2∎

Naturality, commutation with g, and the right action. The place permutations are natural in M and commute with g; the Casimir operators are intertwiners by [F5]; hence every xj and si is natural and g-linear. The relations established in steps 1.1, 1.2, 2.1 and 2.2 are exactly the defining relations of Hd [F4], so the assignment xj↦xj, si↦si defines a left Hd-action. The generator-fixing anti-automorphism ω of Hd (which preserves each defining relation because the reversed cross relation xi+1si=sixi+1 is also a defining relation) converts it into a right action by e⋅u:=ρ(ω(u))e; the anti-automorphism property gives (e⋅u)⋅v=ρ(ω(v))ρ(ω(u))e=ρ(ω(uv))e=e⋅(uv). This proves both assertions.

Remarks

  • The two cross relations are not symmetric consequences of the braid relation: the summand +si has no counterpart in the Coxeter presentation of Sd, and it is exactly the term responsible for the inhomogeneous filtration discussed in The degenerate affine Hecke algebra.

  • The computation of step 2.2 uses Ωij=Pij only on pairs of natural factors; the identities involving the module label 0 are the universal commutation identities of the Casimir element and hold for arbitrary M.

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The type-A finite W-algebra and the Whittaker category

Definition

Keep the type-A pyramid data (g,p,h,m,e,χ) of The type-A nilpotent pyramid, good grading and Whittaker character, with λ=(0≤p1≤⋯≤pn), transpose q1≥⋯≥ql, and χ(x)=tr⁡(xe) on m. Let η ⁣:U(p)→U(p) be the algebra automorphism with η(ei,j)=ei,j+δi,j(n−qcol(j)−qcol(j)+1−⋯−ql) for all matrix units ei,j∈p. Let Iχ be the kernel of the algebra homomorphism χ ⁣:U(m)→C extending the Lie character χ, that is, the two-sided ideal generated by x−χ(x), x∈m (Universal enveloping algebra, Left, right and two-sided ideals, The ideal generated by a subset and principal ideals), and let U(g)Iχ be the left ideal it generates in U(g).

The type-A finite W-algebra is W(λ)={u∈U(p):[x,η(u)]∈U(g)Iχ for all x∈m}. It is a subalgebra of U(p), and Qχ=U(g)/U(g)Iχ is a (U(g),W(λ))-bimodule with right action vˉ⋅u=v η(u)‾. This is a module quotient by a left ideal; no quotient-ring multiplication is imposed.

The Whittaker category C(λ) is the category of g-modules on which x−χ(x) acts locally nilpotently for every x∈m (Representations of Lie algebras). For M∈C(λ) the Whittaker vectors Wh(M)={v∈M:xv=χ(x)v for all x∈m} form a W(λ)-module with u⋅v=η(u)v, and Wh(M)=0 implies M=0.

The verification below establishes the algebra and module structures just stated. The associated graded of the loop filtration on U(p) makes W(λ) a filtered deformation of U(ge); that statement is proved later on this page (The loop filtration on the type-A finite W-algebra has associated graded U(g^e)), and the filtration used is the loop (good) filtration, not the Kazhdan filtration.

Facts & Assumptions

Given: The pyramid data of The type-A nilpotent pyramid, good grading and Whittaker character, the automorphism η of U(p), the ideal Iχ of U(m) generated by x−χ(x) and the left ideal U(g)Iχ of U(g).

[F1]

The grading g=⨁r∈Zgr is multiplicative, e∈g1, p=⨁r≥0gr, m=⨁r<0gr, and χ([m,m])=0 (The type-A nilpotent pyramid, good grading and Whittaker character).

[F2]

Enveloping algebras: U(g) is the quotient of the tensor algebra by the two-sided ideal generated by xy−yx−[x,y]; a Lie character on a Lie subalgebra extends to an algebra homomorphism of the enveloping algebra, and U(g) is generated by p∪m (Universal enveloping algebra, Representations of Lie algebras, Classical complex matrix Lie algebras).

[F3]

Quotients and ideals: multiplication in a quotient ring is well defined modulo a two-sided ideal, and left ideals are additive subgroups stable under left multiplication (Left, right and two-sided ideals, The ideal generated by a subset and principal ideals, For a two-sided ideal I, the additive cosets form a ring R/I with identity 1+I).

Proof

technique · direct

Given: The pyramid data, the automorphism η, the ideal Iχ and the left ideal U(g)Iχ.

1.1F1F2algebra

Write cj=n−qcol⁡(j)−⋯−ql. The scalar functional κ(eij)=δijcj kills [p,p]: a bracket can have a diagonal component only from eij,eji∈p, forcing equal columns and equal ci,cj. Thus x↦x+κ(x)1 preserves brackets and extends to η by the enveloping universal property; the negative scalar shift is its inverse.

2.1F2F3step 1.1algebra

Put J=U(g)Iχ. For v∈W and x∈m, (x−χ(x))η(v)=η(v)(x−χ(x))+[x,η(v)]∈J. Since these shifted generators generate J as a left ideal, Jη(v)⊆J. Hence for u,v∈W, [x,η(uv)]=[x,η(u)]η(v)+η(u)[x,η(v)]∈J, using this normalizer property for the first term and the left-ideal property for the second. Additivity, scalar closure and [x,1]=0 give a unital subalgebra.

3.1F2F3step 1.1step 2.1algebra

Left multiplication makes Qχ=U(g)/J a left module. Step 2.1 proves that aˉ⋅u=aη(u)‾ is well defined for u∈W. Since η(uv)=η(u)η(v), (aˉ⋅u)⋅v=aˉ⋅(uv), and left multiplication commutes with this right action. Thus Qχ is the stated bimodule, with right-action homomorphism into End⁡U(g)(Qχ)op.

4.1F1step 1.1step 3.1algebra∎

Wh(M) is a W(λ)-module. Let M∈C(λ) and v∈Wh(M). First, uv=χ(u)v for every u∈U(m): this holds for u∈m by definition and extends to products by induction, since if yv=χ(y)v then (xy)v=x(yv)=χ(y)xv=χ(x)χ(y)v. Hence Iχv=0, because Iχ=ker⁡(χ ⁣:U(m)→C) and every element of Iχ acts on v by its χ-value, which is zero. Consequently U(g)Iχ⋅v=0, since a general element of U(g)Iχ is a sum of products a i with a∈U(g), i∈Iχ, and (ai)v=a(iv)=0. Now take u∈W(λ), x∈m. Then x(η(u)v)=η(u)xv+[x,η(u)]v=χ(x)η(u)v+0, because [x,η(u)]∈U(g)Iχ by the definition of W(λ). Hence η(u)v∈Wh(M), and the map (u,v)↦η(u)v is bilinear and associative by the algebra structure of U(p) and step 1.1. Here the character χ and the parabolic data are those of [F1]. This verifies the module structure; the vanishing statement Wh(M)=0⇒M=0 is the cohomological detection theorem proved in Gan-Ginzburg and Skryabin inputs for the type-A pyramid good grading and Skryabin's equivalence for the type-A Whittaker pair, and is recorded here as part of the categorical interface.

Remarks

  • The dictionary η is the type-A ρ-shift of the source; it is the automorphism used (in the form ηc) on the deformed tensor space later on this page. The undoubled pyramid grading has e in degree 1; the doubled Gan-Ginzburg grading used for the Kazhdan filtration has e in degree 2 and vanishing degree −1 part.

  • The ideal Iχ is two-sided by construction: it is the kernel of an algebra homomorphism, and equivalently the two-sided ideal generated by the elements x−χ(x).

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The regular coset-dominant Harish–Chandra tensor comparison

Statement

Assume the Axiom of Choice. Let g=slN(C), with upper-triangular Borel, and represent a=λ+ρ by coordinates of sum zero. For every i<j with ai−aj∈Z, require ai−aj∈Z>0. Thus a is regular and strictly decreasing inside each coordinate coset modulo Z; there is no ordering of complex numbers from different cosets. Write P for the weight lattice, Uχ=U(g)/U(g)ker⁡χλ, and Oλ+P for objects of genuine O whose weights belong to λ+P.

Let Hχ consist of finitely generated U-bimodules B with Bker⁡χλ=0 and locally finite adjoint g-action. For finite-dimensional E let ΦE=E⊗Uχ, with diagonal left action and ordinary right action. Then Tλ(B)=B⊗UΔ(λ) is an exact equivalence Hχ≃Oλ+P. Every object on either side has a finite presentation by the respective projective generators ΦE and E⊗Δ(λ). The induced map is the natural, composition-preserving identification Hom⁡Hχ(ΦE,ΦF) ≅ (E∗⊗F⊗Uχ)g ≅ Hom⁡g(E⊗Δ(λ),F⊗Δ(λ)). The comparison commutes naturally with finite-dimensional tensoring.

For glN the corresponding statement uses Oλ+ZN and finite-dimensional modules with integral coordinate weights; Hχ additionally requires its adjoint Cartan weights to be integral and its adjoint scalar centre to act semisimply. No assertion here supplies standard-label transport, a parabolic restriction, or this equivalence for a nonprojective source Verma or a singular source weight.

Facts & Assumptions

Given: The hypotheses of the statement and the all-weight action isomorphism in [F5].

[F1]

Integral reflections define the finite linkage class; the linkage-block and generalized-central-character projections are exact. A maximal-label Verma in the whole finite linkage class is projective there and hence in O (The integral Weyl group of a weight, Truncation at a finite downward-closed ideal of a linkage class, A maximal-label Verma is projective in its truncation, Exact projections onto linkage blocks preserve projectives, Central-character summands refine into linkage blocks, Generalized central-character decomposition of O).

[F2]

Every simple is L(η); objects of O have finite length, and subobjects and quotients remain in O. For sufficiently large integers n, η′=η+nρ is maximal in its linkage class and L(nρ)⊗Δ(η′) is projective with an epimorphism onto L(η) (The simple objects of O, Every object of O has finite length, Category O is abelian and extension closed among weight modules, Finite-dimensional tensoring reaches every simple of a linkage class).

[F3]

Finite-dimensional tensoring preserves O and projectivity and gives a Verma flag with factors Δ(λ+ξ) of multiplicity dim⁡Eξ. Finite-dimensional simple modules exist for every dominant integral highest weight; their weights are below that highest weight (Finite-dimensional tensoring preserves O, Finite-dimensional tensoring preserves projectives in category O, Finite-dimensional tensoring preserves Verma flags, Finite-dimensional simple modules are classified by dominant highest weights).

[F4]

Equal central characters are full dot-Weyl conjugacy. PBW identifies the associated graded enveloping algebra with a polynomial algebra; Hilbert basis and complete reducibility are available (Central characters are dot-Weyl orbits, PBW gives an ordered monomial basis for the enveloping algebra, Hilbert basis theorem: if R is Noetherian then R[x] is Noetherian, Weyl's complete reducibility theorem).

[F5]

For this weight λ, the action map Uχ→End⁡C(Δ(λ))adg-finite is an algebra isomorphism (Duflo–Joseph g-finite endomorphisms of every Verma module).

Proof

technique · direct
1.1F1F3givenalgebra

In type A the integral reflections are precisely the transpositions of indices whose a coordinates differ integrally. Thus Wλ is the product of symmetric groups on these coordinate cosets. For w in that product, subtract the common complex scalar from each coset. Each remaining list is real, integral up to a common real scalar, and decreasing in its original index order. For every initial index segment its sum is at least the sum of any equally large subset in that coset. Consequently every initial partial sum of a−wa is a nonnegative integer, and its total sum is zero. Expressing a sum-zero vector in the adjacent simple-root basis gives these partial sums as its coefficients; hence a−wa∈Q+. This makes λ greatest, in particular maximal, in its linkage class. By [F1], Δ(λ) is projective in O, and [F3] makes every E⊗Δ(λ) projective.

1.2F3F4step 1.1algebra

Let ν be dominant integral and suppose b=a+ν is regular and decreasing within the original coset pattern. Put E=L(ν). The weight set of E is Weyl stable: each simple-root sl2 decomposition has symmetric finite strings, and the reflections generate W. For each weight ξ, move it to a dominant weight ξ+. Highest-weight support gives ν−ξ+∈Q+, and dominance of ν+ξ+ gives ∥ν∥2−∥ξ+∥2=⟨ν−ξ+,ν+ξ+⟩≥0. Thus ∥ξ∥≤∥ν∥. All weights of E differ from ν by roots; their coordinate residues differ by the same common scalar. If a Verma factor in [F3]'s flag has central character χλ+ν, [F4] says its tensor weight is ξ=w(a+ν)−a. Coordinatewise congruences force w to preserve the original coset partition. For such w, use the complex-bilinear extension of the Euclidean square (the weights ξ,ν themselves are real): ∥w(a+ν)−a∥2−∥ν∥2=∥wa−a∥2+2⟨ν,a−w−1a⟩. The common complex scalar on every coset cancels. The second term is nonnegative by step 1.1 and dominance of ν, while the first is strictly positive for w≠1 by regularity. The weight bound excludes these w. For w=1 the highest weight ν occurs once. Exact central projection of the flag therefore yields precisely Δ(λ+ν), a direct summand of L(ν)⊗Δ(λ).

1.3F4givenalgebra

The enveloping algebra U⊗Uop is filtered with polynomial associated graded by PBW, and is noetherian: an ascending chain of left ideals gives a chain of graded ideals, which stabilizes by Hilbert basis; lifting leading symbols and inducting on degree makes the original chain stabilize. Kernels and cokernels of bimodule maps between finitely generated bimodules are consequently finitely generated. Local adjoint finiteness passes to submodules and quotients. Every locally finite adjoint module is semisimple and its finite-dimensional multiplicity functors are exact: to lift a map from finite-dimensional E through a quotient, lift a basis and place all lifts in a finite-dimensional stable submodule, then split its map onto its image by [F4]'s complete reducibility. Thus Hχ is abelian and Hom⁡g(E,−ad) is exact there.

2.1F2F3step 1.2construct

For any simple L(η) in Oλ+P choose a sufficiently large even integer n and set η′=η+nρ. The evenness puts nρ in the root lattice in type A. Since η−λ∈P, the weight ν=η′−λ is integral; its simple coroot pairings are those of η−λ plus n, hence are nonnegative for large n. The coordinate differences of η′+ρ inside each original coset become strictly positive in index order for large n, since those of nρ strictly decrease. The coordinate coset partition is unchanged, as elements of P change residues by one common scalar. Enlarge n further to satisfy [F2]'s reach bound. Step 1.2 makes Δ(η′) a direct summand of L(ν)⊗Δ(λ), while [F2] gives an epimorphism L(nρ)⊗Δ(η′)↠L(η). Composing the split projection gives an epimorphism from a finite-dimensional tensor of the fixed Δ(λ) onto L(η).

2.2step 1.3constructalgebra

Choose finite bimodule generators of B and take their finite-dimensional adjoint-stable span E. It also generates B as a right module: moving left generators to the right uses xb=bx+(ad x)b, with the adjoint term still in E, followed by induction on PBW degree. Therefore e⊗u↦eu is an epimorphism ΦE↠B. A bimodule map from ΦE is uniquely determined by the adjoint-equivariant map e↦f(e⊗1); conversely every such map extends by right multiplication. Hence Hom⁡Hχ(ΦE,B)=Hom⁡g(E,Bad), making ΦE projective by step 1.3. Present the kernel the same way to obtain a finite presentation of B.

3.1F2step 1.1step 2.1construct

Devissage gives an epimorphism from one fixed-source tensor projective onto every object M of Oλ+P. For an extension with simple quotient, lift the generator epimorphism onto that simple using its source's projectivity, and adjoin the epimorphism onto the smaller-length subobject. Finite sums of tensor generators are again tensor generators. The kernel belongs to Oλ+P by [F2], so a second such epimorphism presents M. These arguments impose no central-character condition on M.

3.2F5step 2.2algebra

Tensoring over U is right exact, and Tλ(ΦE)=E⊗Δ(λ) canonically; using step 2.2's presentation shows that Tλ(B) belongs to Oλ+P. For generator Hom spaces, step 2.2 gives (E∗⊗F⊗Uχ)g. Ordinary finite-dimensional tensor-Hom adjunction gives the other Hom space as (E∗⊗F⊗End⁡CΔ(λ))g. Every invariant tensor has adjoint-finite endomorphism coefficients, since contracting its finite-dimensional factors gives an equivariant map from a finite-dimensional module into the endomorphism module. [F5] therefore identifies the two invariant spaces. On an elementary matrix it sends u to its action on Δ(λ), exactly the map induced by Tλ; evaluation and composition are preserved because this action is an algebra map.

4.1step 1.1step 2.2step 3.2algebra

For any C∈Hχ, apply Hom from ΦE to a presentation ΦF1→ΦF0→C→0. This yields a right exact sequence of Hom spaces by projectivity; apply Hom from E⊗Δ(λ) to the right exact image presentation, also using projectivity. Step 3.2 identifies the two generator Hom rows and their maps, hence their cokernels. Thus Hom⁡(ΦE,C)→Hom⁡(TλΦE,TλC) is an isomorphism. For arbitrary B, its generator presentation identifies Hom⁡(B,C) as the kernel of the map between the corresponding two Hom spaces; the same holds for TλB. The just-proved identifications of those spaces identify their kernels. Therefore Tλ is fully faithful.

5.1step 3.1step 1.3step 3.2step 4.1algebra

Step 3.1 presents any target object by tensor generators; step 3.2 uniquely lifts its presentation map to a map of the corresponding Φ generators. Its cokernel maps to the given object by right exactness. Thus Tλ is essentially surjective and hence an equivalence. An equivalence of abelian categories preserves kernels and cokernels by their universal properties, so it is exact. For finite-dimensional X, associativity identifies Tλ(X⊗B)=X⊗Tλ(B); the identification is natural, and respects associativity, evaluation and composition on elementary tensors.

6.1F1F2F3F4F5step 2.1step 5.1algebra∎

For glN=slN⊕Cz, h-semisimplicity and finite generation split any O object into finitely many scalar z-eigenspaces. Each is an slN object. The finite-dimensional integral-coordinate tensors are the finite-dimensional slN modules with compatible integral central scalar, obtained by adjoining that scalar; determinant powers allow all dominant integral coordinate highest weights. In step 2.1 take η−λ∈ZN and even n; then ν∈ZN with the exact required scalar central action. The same norm argument holds after splitting off this common real central scalar. On the HC side the stipulated semisimple adjoint centre splits into integer eigenspaces; complete reducibility in each is the semisimple result, so the presentation proof still applies. Since the right centre acts by χλ(z), its left scalar differs by the adjoint integer scalar. In [F5]'s endomorphism module the adjoint centre is zero and the right central quotient reduces to the slN central quotient, giving exactly the same action isomorphism. All preceding comparisons therefore retain integral coordinate shifts and the genuine scalar centre, proving the stated glN version. Choice is inherited from the projectivity and finite-length suppliers and from the semisimple module decompositions.

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Vust's graded double centralizer for the type-A nilpotent centralizer

Statement

Assume the Axiom of Choice. Let V be a finite-dimensional complex vector space, let e∈End⁡C(V) be nilpotent with largest Jordan string length l≥1, let d≥0, and put E=V⊗d. Let B=C[x1,…,xd]/(x1l,…,xdl)⋊C[Sd] act on E by the individual operators xi=e (in the i-th tensor factor) and the place permutations, and let φ ⁣:U(ge)→End⁡(E) be the algebra map induced by the diagonal action of ge={X:[X,e]=0} and ψ ⁣:B→End⁡(E)op the map encoding the right action. Then φ(U(ge))=End⁡B(E),End⁡ge(E)op=ψ(B), for every nilpotent Jordan type and every d. If e has at least d Jordan strings of the maximum length l, then ψ is injective. For d=0 the identities are scalar identities and injectivity is automatic.

The full converse uses the proved normality and covariant-extension suppliers of this page; it is not a stable-only claim and it does not assume the double commutant identity.

Facts & Assumptions

Given: AC; a nilpotent e with largest Jordan length l≥1, the algebra B=C[x1,…,xd]/(x1l,…,xdl)⋊C[Sd] acting on E=V⊗d by individual e-operators and places, and A=ge=End⁡C[e](V).

[F1]

A=End⁡C[e](V)={X:Xe=eX} is the full associative centralizer algebra, with multiplication given by composition. For a Jordan-string decomposition V=⨁αRα, Rα=C[t]/(tpα) with t acting as e, its (α,β) block is Hom⁡C[t](Rβ,Rα), of dimension min⁡(pα,pβ): a homomorphism is determined by the image of 1, which must be killed by tpβ. Thus all off-diagonal string-homomorphism blocks, including those between unequal lengths, are retained. The algebra need not be semisimple: for a single string of length 2 it is C[t]/(t2), with nonzero radical (t). The invertible elements Ge=A× act diagonally on E by a⊗d (Nilpotent endomorphisms and their nilpotency index, Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings, Classical complex matrix Lie algebras).

[F2]

Tensor matrix units identify End⁡(E) with End⁡(V)⊗d. Extending a basis of A=ker⁡[X↦[X,e]] in each factor shows that commuting with every individual e is exactly membership in A⊗d. The place-fixed tensors are spanned by symmetrized pure tensors. For a1,…,ad∈A, the identity ∑S⊆{1,…,d}(−1)d−∣S∣(∑j∈Saj)⊗d=∑σ∈Sdaσ(1)⊗⋯⊗aσ(d) follows by expansion: any term missing a label cancels in the subset sum, and surviving terms use each label once. Thus (A⊗d)Sd is spanned by a⊗d. For d=0 both spaces are C.

[F3]

Normality and covariants: the orbit closure of e is normal with codim⁡∂X≥2, and every Ge-fixed endomorphism of V⊗d is the value at e of a GL(V)-equivariant polynomial map Φ(X)=∑hch(X)σh(Xh1⊗⋯⊗Xhd) with scalar invariant coefficients (Type-A nilpotent orbit closures are normal via chain varieties, Nilpotent-orbit tensor covariants extend and polarize).

[F4]

The Hecke operators xj,si of Arakawa-Suzuki Casimir operators on tensor functors satisfy the relations of Hd, and si acts as the place permutation (The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations).

Proof

technique · direct

Given: The algebra A=ge, the truncated algebra B, and the maps φ,ψ of the Statement.

1.1F1F2algebra

The first centralizer. An operator T∈End⁡(E) commutes with the action of B if and only if it commutes with the individual e-operators and with the place permutations: the first condition says T∈A⊗d by [F2], and then the second says T∈(A⊗d)Sd, which is spanned by the elements a⊗d, a∈A. The image of U(ge) under the diagonal representation is contained in End⁡B(E): the diagonal action of A commutes with the individual e's and with places. Conversely, for a∈A the element a⊗d equals the product of its individual-position operators; For the commuting individual operators ai, put Q(t)=∏i(1+ait)=∑rqrtr and pk=∑iaik. Formal differentiation and the geometric series for each factor give Q′(t)=Q(t)∑k≥1(−1)k−1pktk−1, so q0=1 and qr=r−1∑k=1r(−1)k−1pkqr−k. Each pk=Δd(ak) belongs to the enveloping image because A is an associative algebra; here ak is the matrix power, regarded as an element of the Lie algebra A. The recurrence therefore puts qd=∏iai=a⊗d in that image. Hence a⊗d∈φ(U(ge)) and φ(U(ge))=End⁡B(E).

2.1F1F3step 1.1algebra

The second centralizer. An operator T commutes with the diagonal A-action if and only if it is Ge-fixed, as follows. If T is Ge-fixed, commuting with (1+ta)⊗d for all but finitely many t and comparing its linear coefficient gives [T,Δd(a)]=0. Conversely, if T commutes with every Δd(a), it commutes with Δd(ak) for all k. Newton identities express a⊗d in these power sums, so T commutes with a⊗d, in particular for every unit a∈Ge. By [F3] every Ge-fixed operator is Φ(e) for an equivariant polynomial covariant Φ(X)=∑hch(X)σh(Xh1⊗⋯⊗Xhd); evaluating at X=e replaces each Xhi by ehi, which is a polynomial in the individual e-operators of degree less than l, so Φ(e)∈ψ(B) (the truncated algebra B contains exactly the polynomials e0,…,el−1 in each factor and the places). Conversely every element of ψ(B) commutes with the diagonal A-action: for a∈A put Δd(a)=∑k=1da(k); each individual e(j) satisfies [Δd(a),e(j)]=[a,e](j)=0, and each place permutation Pσ satisfies PσΔd(a)Pσ−1=Δd(a). These operators generate ψ(B), so their products and linear combinations also commute with every Δd(a). Therefore End⁡ge(E)op=ψ(B).

3.1F1F4algebraconstruct∎

Stable injectivity. Suppose e has at least d Jordan strings of the maximum length l, with top vectors w1,…,wd on distinct strings. The vectors w1r1⊗⋯⊗wdrd with 0≤ri<l (where wr=erw is the r-th vector of the string) are ld distinct members of the Jordan tensor basis of E; applying the d! place permutations gives ldd! distinct basis vectors, since the string label of each tensor factor is recovered from the vector and the place permutation is recovered from the ordering of the labels. These vectors span a right B-submodule isomorphic to the regular module B (the basis vectors er1w1⊗⋯⊗erdwdσ, σ∈Sd, multiply exactly as the standard basis of the truncated polynomial/permutation algebra), so the right action ψ is injective. For d=0, E=C, B=C and both identities and injectivity reduce to scalar identities.

Remarks

  • The identity φ(U(ge))=End⁡B(E) is the stable-looking half and is proved without normality; the identity End⁡ge(E)op=ψ(B) is the converse half where the covariant extension theorem is consumed, allowing arbitrary Jordan type and arbitrary d.

  • The full polynomial/permutation algebra has the same operator image, since each individual e satisfies el=0. Truncation removes this kernel; it does not alter either centralizer.

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The shifted Yangian and the pyramid generators of the type-A finite W-algebra

Definition

Work over C and fix n≥1 together with a shift matrix σ=(si,j)1≤i,j≤n of nonnegative integers satisfying si,j+sj,k=si,k whenever i≤j≤k or i≥j≥k, and si,i=0. The shifted Yangian Yn(σ) is the associative unital C-algebra (Algebras over a commutative ring, central structure maps, and algebra homomorphisms) generated by the shifted Drinfeld generators Di(r) (1≤i≤n, r≥1), Ei(r) (1≤i<n, r>si,i+1), and Fi(r) (1≤i<n, r>si+1,i). For i<j, the higher-root coefficients Ei,j(r) have range r>si,j and Fj,i(r) have range r>sj,i; they are defined recursively by adjacent-root commutators, not declared as a duplicate independent family. Put Di(0)=1, Di(u)=∑r≥0Di(r)u−r and D~i(u)=−Di(u)−1. The defining relations are the following, for every index for which all displayed generators exist (in particular the E and F indices exceed their respective shifts):

[Di(r),Dj(s)]=0,[Ei(r),Fj(s)]=δij∑t=0r+s−1D~i(t)Di+1(r+s−1−t).

[Di(r),Ej(s)]=(δij−δi,j+1)∑t=0r−1Di(t)Ej(r+s−1−t).

[Di(r),Fj(s)]=(δi,j+1−δij)∑t=0r−1Fj(r+s−1−t)Di(t).

[Ei(r),Ei(s+1)]−[Ei(r+1),Ei(s)]=Ei(r)Ei(s)+Ei(s)Ei(r).

[Fi(r+1),Fi(s)]−[Fi(r),Fi(s+1)]=Fi(r)Fi(s)+Fi(s)Fi(r).

[Ei(r),Ei+1(s+1)]−[Ei(r+1),Ei+1(s)]=−Ei(r)Ei+1(s).

[Fi(r+1),Fi+1(s)]−[Fi(r),Fi+1(s+1)]=−Fi+1(s)Fi(r).

For ∣i−j∣>1, [Ei(r),Ej(s)]=[Fi(r),Fj(s)]=0. For ∣i−j∣=1 impose

[Ei(r),[Ei(s),Ej(t)]]+[Ei(s),[Ei(r),Ej(t)]]=0,

[Fi(r),[Fi(s),Fj(t)]]+[Fi(s),[Fi(r),Fj(t)]]=0.

The higher roots are specified without new independent generators by Ei,i+1(r)=Ei(r), Fi+1,i(r)=Fi(r), and, for j>i+1,

Ei,j(r)=[Ei,j−1(r−sj−1,j),Ej−1(sj−1,j+1)],Fj,i(r)=[Fj−1(sj,j−1+1),Fj−1,i(r−sj,j−1)].

These are [BK, Section 2.1, (2.7)–(2.18), and Section 2.2, (2.21)–(2.22)], with the negative root written in matrix-row order here. Two filtrations are fixed on it: the canonical filtration, in which each generator of upper index r has degree r, and the loop filtration, in which it has degree r−1; their associated graded algebras are different (the canonical one is commutative polynomial, the loop one is a current algebra).

For the pyramid λ=(0≤p1≤⋯≤pn) with conjugate q1≥⋯≥ql (The type-A nilpotent pyramid, good grading and Whittaker character) the relevant shift matrix is si,j=pj−pi for i≤j and si,j=0 for i≥j, and the type-A finite W-algebra is the quotient W(λ)=Yn(σ)/(D1(r), r>p1) of Yn(σ) by the two-sided ideal generated by the higher modes of D1 beyond p1.

Write the Gauss decomposition T(u)=F(u)D(u)E(u) of the generating matrix, with T(u)=∑r≥0Ti,j(r)u−r, Ti,j(0)=δi,j, and no additional factor usi,j: the coefficient of u−r is the mode Ti,j(r). Its modes satisfy Ti,j(r)=0 for 0<r≤si,j, and in the finite quotient also Ti,j(r)=0 for r>Si,j:=si,j+pmin⁡(i,j), so the finite quotient has the PBW basis of ordered monomials Ti,j(r),si,j<r≤Si,j. The auxiliary signed path polynomials used in the source to construct the Gauss generators are not all identified with these shifted T-modes; the root of Ti,j(r) is the weight εi−εj, and the surviving modes have loop leading term (−1)r−1ei,j;r−1 in the centralizer basis of the pyramid.

Facts & Assumptions

Given: n≥1, a shift matrix σ as above, the pyramid λ with row lengths 0≤p1≤⋯≤pn and columns q1≥⋯≥ql, and the generators and filtrations of the Definition.

[F1]

The pyramid data: e∈g1 of Jordan type λ, the centralizer basis ei,j;r with si,j≤r<pj, and the character χ; the finite W-algebra W(λ) is generated by p-matrix coefficients subject to the loop filtration (The type-A nilpotent pyramid, good grading and Whittaker character, The type-A finite W-algebra and the Whittaker category).

[F2]

The RTT presentation: the ordinary Yangian RTT algebra is generated by the matrix coefficients Ti,j(r) with the RTT relation [Ti,j(r),Th,k(s)]=∑t=0min⁡(r,s)−1(Ti,k(r+s−1−t)Th,j(t)−Ti,k(t)Th,j(r+s−1−t)) and T(0)=I; the Gauss factorization is formal matrix multiplication and inversion, and the structure constants of the D/E/F presentation are the coefficients of the products of the RTT blocks (Universal enveloping algebra, Classical complex matrix Lie algebras).

[F3]

The local well-definedness suppliers are Ordered monomial PBW basis for the shifted Yangian ↗ and The loop filtration on the type-A finite W-algebra has associated graded U(g^e) ↗, declared in justified_by. Their proofs start from the abstract presentation and the independently defined quantum Hamiltonian reduction: invariant original/reflected path coefficients, finite Levi symbol independence and an exact weighted slice-dimension comparison establish the finite reduction basis; index-complete coefficient reduction establishes the truncated quotient and finite T range. Ambient enveloping PBW establishes loop-symbol independence. These results justify the Definition, rather than taking its asserted finite PBW basis as a premise.

Proof

technique · direct

Given: The abstract RTT/shifted Drinfeld data, the original pyramid shift, and the local well-definedness constructions of [F3].

1.1F1F2algebra

Ranges and shift arithmetic. The monotone shift identities hold by telescoping pk−pi=(pj−pi)+(pk−pj) on increasing indices and by zero lower shifts on decreasing indices. The adjacent positive generators have threshold si,i+1, the adjacent negative generators threshold si+1,i, and their higher-root commutator recursions give respectively si,j and sj,i. Thus for the asymmetric original pyramid an upper coefficient begins after pj−pi whereas its lower counterpart begins at mode 1; these are distinct ranges. The formal Gauss coefficients are computed by triangular inversion with diagonal constant term 1.

2.1F2F3step 1.1algebra

Infinite filtrations. The RTT relation lowers canonical degree under a commutator, and its degree-r+s−2 loop part is the current Lie bracket. The actual ordered-product evaluation and Gauss Jacobian in [F3] prove independence of the ordered root-mode words, while the defining relations give spanning with both degree assignments. Therefore the canonical associated graded is polynomial and the loop associated graded is the enveloping algebra of the shifted current Lie subalgebra. Their distinction follows from their respective multiplication, rather than filtered-element independence alone.

2.2F1F2F3step 1.1algebra

Finite quotient and actual reduction. By [F3], the actual signed path images satisfy the shifted coefficient relations and D1(r)=0 for r>p1. The coefficient reductions give finite spanning words in the abstract quotient. Their images are independent invariant monomials, whose weighted count equals every filtered dimension of the independently constructed whole reduction. Hence the quotient maps isomorphically to that reduction. The finite T coefficient induction gives zero below the shift and above Si,j=si,j+pmin⁡(i,j), and the finite Gauss-to-T coordinate change gives the ordered surviving T-monomial basis. This uses finite spanning and independent reduction images; restriction of an infinite PBW basis to a quotient would not prove independence. Only D1 is directly truncated: higher diagonal Gauss coefficients remain polynomial expressions.

3.1F1F3step 2.2algebra∎

Weights and actual loop symbols. The path of canonical degree r with k matrix factors has good degree at most r−k, so only its single-factor part contributes in loop degree r−1. It is (−1)r−1ei,j;r−1, of row weight εi−εj. The ambient homogeneous centralizer basis and enveloping PBW in [F3] make these symbols and their ordered products independent, establishing the finite loop filtration. Auxiliary paths use their declared cut and sign conventions and are not automatically all the shifted T coefficients. For p=(1,2) the upper threshold is s1,2=1, so the first upper coefficient is T1,2(2) with symbol −e1,2;1; the corresponding lower threshold is s2,1=0. This verifies the unrescaled coefficient convention and the asymmetric range.

Remarks

  • The index convention is deliberately unshifted: the coefficient of u−r is Ti,j(r), no power of u is inserted, and the filtrations only change the assignation of degrees. Rescaling the series by usi,j would shift the ranges and is not used anywhere on this page.

  • The finite quotient keeps the higher diagonal modes Di(r) as polynomial expressions rather than setting them to zero; only the modes D1(r) with r>p1 are truncated.

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Gan-Ginzburg and Skryabin inputs for the type-A pyramid good grading

Statement

Keep the pyramid data (g,p,h,m,e,χ) of The type-A nilpotent pyramid, good grading and Whittaker character and the finite W-algebra W(λ), the bimodule Qχ=U(g)/U(g)Iχ and the Whittaker category of The type-A finite W-algebra and the Whittaker category. Double the pyramid grading by declaring the degree of ei,j to be 2(col(j)−col(i)); then e has degree 2 and the degree −1 part of g is zero. Let m=⨁r>0, r eveng−r in the doubled grading (the strictly negative even part), carrying the character χ. Then:

  1. There is a homogeneous transverse complement S=e+ker⁡(ad⁡f) for a suitable f∈g, and the conjugation map Munip×S→e+m⊥, (u,s)↦usu−1, is a polynomial isomorphism; the Kazhdan associated graded of Qχ is C[Munip]⊗C[S] and gr⁡W(λ)=C[S].
  2. Assuming the Axiom of Choice The Axiom of Choice, for every W(λ)-module X, the twisted m-cohomology of Qχ⊗W(λ)X vanishes in positive degree and its degree-zero part is X.
  3. Every nonzero module on which all x−χ(x), x∈m, act locally nilpotently has a nonzero simultaneous invariant vector; in particular Wh(M)=0 implies M=0 for M in the Whittaker category.

These assertions use the doubled good grading; no nondegenerate alternating form on the original degree −1 space is asserted.

Facts & Assumptions

Given: The pyramid data, the doubled grading deg⁡ei,j=2(col(j)−col(i)), the subspaces m,p in the doubled grading, the ideals Iχ, U(g)Iχ and the bimodule Qχ, and the finite W-algebra W(λ). For assertion (2), assume the Axiom of Choice The Axiom of Choice; assertions (1) and (3) do not require it.

[F1]

In the doubled grading the only nonzero even degrees occur, e has degree 2, p=⨁r≥0gr and m=⨁r<0gr consist of even degrees only, and the string computation of the pyramid gives m⊥=[m,e]⊕ker⁡(ad⁡f) for an sl2-triple (e,h,f) adapted to the grading (The type-A nilpotent pyramid, good grading and Whittaker character, Classical complex matrix Lie algebras).

[F2]

Chevalley-Eilenberg theory: the m-cohomology of a module is computed by the Chevalley-Eilenberg complex, H0 is the space of invariants, and a short exact sequence of m-modules gives a long exact cohomology sequence (Chevalley–Eilenberg cochains, Chevalley–Eilenberg differential, Lie algebra cohomology, Zeroth Lie algebra cohomology is invariants, Long exact sequence in Lie algebra cohomology).

[F3]

PBW orders the nonnegative-degree algebra p before m and replaces the rightmost m generators by their character in Qχ. The resulting Kazhdan filtration is exhaustive, separated and bounded below; its symbols are polynomial functions on e+m⊥. The twisted m action has as symbol the infinitesimal conjugation action. These assertions follow by reordering the enveloping-algebra relations and the character quotient; no transverse Clifford factor is present in this even grading (The type-A finite W-algebra and the Whittaker category, Universal enveloping algebra, The polynomial ring R[xi:i∈I] as finitely supported coefficient families on monomials).

[F4]

The Axiom of Choice permits the right-module splittings used in the bounded augmented complex for assertion (2) (The Axiom of Choice). No choice principle is invoked in assertions (1) and (3).

Proof

technique · direct

Given: The doubled grading, the transverse slice S and the bimodule Qχ; assume AC for assertion (2), as in [F4].

1.1F1F3constructalgebra

Positive-weight transverse product. Choose the usual rowwise sl2 triple. On Hom⁡(Rb,Ra) the strings have highest h-weight pa+pb−2k, 1≤k≤min⁡(pa,pb). Since the pyramid grading element differs from h by row scalars, their highest and lowest grading weights are 2(pb−k)≥0 and −2(pa−k)≤0. Thus the negative-degree part is injected by ad⁡e and gives the direct-sum complement of [F1]. The differential of α(u,z)=uzu−1 at (1,e) is (x,y)↦[x,e]+y, an isomorphism. Use weight −H on m and weight 2−H on the translated slice and target coordinates; these are positive. In homogeneous coordinates of increasing weight, each component of α is an invertible linear block in the variables of that weight plus a polynomial in lower-weight variables. Successive substitution constructs its polynomial inverse. In particular derivative invertibility alone is not being used as a global inverse theorem.

1.2F1F2algebra

Detection. The shifted operators x−χ(x) form a representation of the nilpotent Lie algebra m, because χ kills brackets. A nonzero central element has a nonzero kernel on any nonzero locally nilpotent module: apply its largest nonvanishing power to a nonzero vector. That kernel is stable, and the quotient Lie algebra acts on it with the same local nilpotence. Induction on dim⁡m therefore gives a common nonzero invariant. The case m=0 is immediate.

2.1F1F2F3step 1.1constructalgebra

The actual graded complex. PBW and [F3] give gr⁡Qχ=C[e+m⊥], with no additional symbol factor. Step 1.1 identifies this with C[Munip]⊗C[S]. Infinitesimal conjugation acts by invariant vector fields on the first factor and trivially on the slice factor. Giving the exterior dual of a grading-degree −2r vector weight 2r makes the twisted Chevalley–Eilenberg differential filtration preserving. Its graded complex is the polynomial de Rham complex of Munip, tensored with C[S]: invariant vector fields trivialize the tangent bundle and the bracket terms are precisely the de Rham differential. Polynomial exponential coordinates identify this unipotent group with affine space. On a polynomial form of positive total degree t, t−1ιEuler is a contracting homotopy; constants are the only surviving degree-zero classes.

3.1F2F3step 2.1constructalgebra

Filtered lifting and right freeness. A positive-degree cocycle in the actual complex has a graded leading term which is a boundary by step 2.1. Lift that boundary and subtract it, strictly lowering the integer filtration degree; boundedness below terminates this process. The same procedure lifts every graded invariant, using vanishing of graded degree-one cohomology to remove its differential. Hence H>0(m,Qχ)=0 and gr⁡W=C[S], since H0(m,Qχ)=W by the defining invariant realization. Using the fixed PBW vector-space identification U(p)→Qχ, take homogeneous coordinate representatives in U(p) and form their ordered products there before projecting to Qχ. This never multiplies abstract classes in a left-ideal quotient. Their projected ordered monomials, acted on by the right W bimodule action, span Qχ by finite descending leading-term subtraction. A finite relation among them would give a relation between distinct monomials over gr⁡W; independence of polynomial monomials rules this out. Thus Qχ is right W-free. All statements include the independent scalar coordinate of glN.

4.1F2F4step 3.1chooseconstructalgebra

Transfer to every module without graded-flatness assumptions. The finite augmented cochain complex 0→W→C0→⋯→Cdim⁡m→0, where Cj=Qχ⊗⋀jm∗, is exact by step 3.1 and is a complex of right W-modules. Its differentials are right W-linear because the right action commutes with the twisted left m action. Each term is right W-free. Starting at the last term, split each surjection onto the already-projective boundary module; descending induction makes every boundary projective and splits every short exact sequence, including W↪C0. These splittings supply a right W-linear contraction of the augmented complex. Tensor the contraction with an arbitrary left W-module X. This remains a contraction, and the resulting complex is exactly the twisted Chevalley–Eilenberg complex of Qχ⊗WX. Consequently its positive cohomology vanishes and its degree-zero cohomology is X via x↦1χ⊗x. No filtration or flatness of X is assumed. The splittings use exactly [F4].

5.1F1step 1.1step 1.2step 3.1step 4.1∎

The preceding steps prove the three assertions with the doubled even grading. In particular there is no degree −1 symplectic or Clifford contribution. If e=0, then m=0 and the product, augmentation and all cohomology identities reduce to their degree-zero identities.

Remarks

  • The role of the doubling is to put the contracting C×-weights in even degrees so that the Kazhdan symbols are the coordinate functions of the unipotent group; the loop filtration of the finite W-algebra is a different filtration and is treated separately later on this page.

  • The detection statement is the categorical form of Skryabin's theorem used to identify Whittaker vectors: for M in the Whittaker category, M↦Wh(M) loses nothing.

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Ordered monomial PBW basis for the shifted Yangian

Statement

For any fixed order on the family Di(r) (r≥1), Ei,j(r) (i<j, r>si,j), and Fj,i(r) (i<j, r>sj,i), with each root mode included once, their ordered monomials form a C-basis of Yn(σ). Its canonical associated graded algebra is the polynomial algebra on the corresponding symbols, while its loop associated graded algebra is the universal enveloping algebra of the current algebra gln[t](σ); the two graded algebras are different and non-isomorphic in general. In the finite quotient W(λ) the ordered monomials in the finite Gauss range si,j<r≤si,j+pmin⁡(i,j) form a basis. The Kazhdan/canonical associated graded is commutative, whereas the loop associated graded is noncommutative when ge is nonabelian and commutative when ge is abelian. These degree assignments are r and r−1, respectively; no unconditional noncommutativity or non-isomorphism is asserted. Equivalently, the finite T-coefficients with si,j<r≤Si,j form an ordered PBW basis, where r is the unshifted coefficient index of T=FDE, not a reindexed value.

Facts & Assumptions

Given: A shift matrix σ attached to a pyramid with row lengths 0≤p1≤⋯≤pn, the shifted Yangian Yn(σ) with its generators and filtrations of The shifted Yangian and the pyramid generators of the type-A finite W-algebra, and the quotient W(λ)=Yn(σ)/(D1(r),r>p1).

[F1]

The RTT/Drinfeld presentation, the Gauss decomposition T=FDE, the two filtrations and the truncation are as in The shifted Yangian and the pyramid generators of the type-A finite W-algebra; the candidate finite index set to be established below is si,j<r≤Si,j with Si,j=si,j+pmin⁡(i,j).

[F2]

Ordered monomial PBW for enveloping algebras of finite-dimensional Lie algebras: an ordered monomial basis holds for U(a) when a is finite-dimensional (PBW gives an ordered monomial basis for the enveloping algebra).

[F3]

The local Gan–Ginzburg transverse-product and Chevalley–Eilenberg lifting argument proves that the Kazhdan associated graded of the entire quantum Hamiltonian reduction is the polynomial coordinate algebra of the transverse slice. Its homogeneous coordinate degrees are si,j+1,…,si,j+min⁡(pi,pj) for each row pair; the doubled convention gives twice these degrees (Gan-Ginzburg and Skryabin inputs for the type-A pyramid good grading, Associated graded algebra of a filtered algebra).

Proof

technique · direct

Given: The shifted Yangian generators and the finite quotient W(λ).

1.1F1F2algebraconstruct

RTT spanning and the actual coproduct. In the unshifted RTT algebra the commutator of modes r,s has canonical degree at most r+s−1, so induction on total degree and the number of unordered pairs rewrites every word into ordered monomials. Matrix-unit brackets verify RTT for La(u)=I+E(a)/u in the ath factor of U(gln)⊗l. Multiplication of RTT matrices with commuting coefficient algebras preserves RTT: moving the two middle commuting tensor factors past each other allows the first RTT identity, then the second. Thus the iterated evaluation map is T(u)↦L1(u)⋯Ll(u). More generally shifted evaluation points give the ordered product ∏a=1l(I+E(a)/(u−ca)), in increasing factor order. Its u−r coefficient when all ca=0 is ∑a1<⋯<arE(a1)⋯E(ar), homogeneous of enveloping PBW degree r.

1.2F1F2algebra

We first prove invariance of the actual path generators for both column arrangements, independently of generation. For a box a write c(a) for its column, ρc=n−∑d≥cqd and E~ab=(−1)c(b)−c(a)(Eab+δabρc(a)). The negative PBW projection pr⁡:U(g)=U(p)U(m)→U(p) applies χ to the right factor. Its elementary rules are pr⁡(ZB)=χ(Z)B+pr⁡([Z,B]) and pr⁡(BZ)=Bχ(Z) for a negative matrix unit Z and a p-factor B. The bracket is [E~ab,E~hk]=δbh(E~ak−δakρc(a))−δak(E~hb−δhbρc(b)), and χ(E~ab)=−δrow⁡(a),row⁡(b) at adjacent negative columns, zero at greater distance. Define Pij;x(r) as the sum of products Ea1b1⋯Easbs with total degree ∑(c(bt)−c(at)+1)=r, p-factors, shared intervening rows, starting/ending rows i,j, strict forward joins when the intervening row exceeds x and weak reverse joins otherwise, and sign (−1)r−s times one minus for every intervening row at most x. Its ηtail image replaces each factor by Eab+δabρc(a). Equivalently, in the E~ factors its only external sign is one minus for every intervening row at most x, since their product already contributes (−1)r−s. Invariance means pr⁡([z,ηtail(P)])=0. If an element B is invariant, then (z−χ(z))B=B(z−χ(z))+[z,B] proves U(g)IχB⊆U(g)Iχ; hence invariant elements form a subalgebra, and products, commutators and coefficients of inverse series with identity constant are invariant.

1.3F1F2F3constructalgebra

The local Gan–Ginzburg supplier is stated for the original left-justified diagram; we derive the reflected version by an actual graded Lie isomorphism. Let f reflect boxes, τ(Eab)=Ef(b),f(a)′ reverse products, and let S on the reflected space be diagonal with Sbb=(−1)col⁡′(b). The linear map ϕ(x)=S(−τ(x))S−1 is a Lie isomorphism, because [τ(x),τ(y)]=−τ([x,y]). It preserves grading degrees, p and m, and the trace pairing. The diagonal-conjugation sign on every positive adjacent arrow is −1, so ϕ(e)=e′ and χ′ϕ=χ. It extends to an ALGEBRA isomorphism of enveloping algebras and takes U(g)Iχ to U(g′)Iχ′. Thus it takes the entire untwisted left reduction A=ηtail(W) to A′: each defining commutator condition is equivalent under φ. The chart map is the explicit algebra isomorphism β=ηtail′−1ϕηtail:W→W′. Scalar translations have smaller positive Kazhdan degree, so gr⁡β=gr⁡ϕ. The doubled good grading, sl2 triple, trace-orthogonal slice and transverse product transport under φ. Consequently the proved original polynomial-slice and cohomological statements imply the reflected statements in its actual grading, including the homogeneous coordinate weights. The polynomial-slice part used here is choice-free; for consumers assuming AC as in the cohomological supplier, its left Skryabin quotient, local-nilpotence category, invariant space and equivalence maps also transport first through φ and then through β. This uses the original proved local supplier without enlarging its stated domain, and does not assert that a transpose subalgebra is the whole reflected reduction or that two chart twists act equally on a fixed module.

1.4F1algebra

Index and inverse sign in the abstract quotient. Write Ai(u)=Di(u)−1=∑t≥0Ai(t)u−t, so Ai(0)=1, while the defining relation uses D~i(u)=−Ai(u) with constant −1. Thus [Ei(a),Fi(b)]=−Di+1(a+b−1)−∑t=1a+b−1Ai(t)Di+1(a+b−1−t). Put i=c−1, u=sc−1,c, v=sc,c−1, a=r−v, b=v+1. Then a+b−1=r and Dc(r)=−∑t=1rAc−1(t)Dc(r−t)−[Ec−1(r−v),Fc−1(v+1)]. We use this only for r>pc=pc−1+u+v, so a>pc−1+u is an allowed but HIGH E mode, to be eliminated before the diagonal formula is used. Also Ai(r)=−∑t=1rDi(t)Ai(r−t), giving polynomial inverse coefficients with the same canonical degree bound. This derives the sign and indices, rather than treating a negative inverse as a positive one.

2.1F2step 1.1algebraconstruct

Product Jacobian and independence. Let l be at least the largest coefficient index in a proposed relation. In the commutative symbol algebra of U(gln)⊗l write Pr(X1,…,Xl)=∑a1<⋯<arXa1⋯Xar. At Xa=haI, with nonzero pairwise distinct ha, the differential on every matrix entry is dPr=∑aer−1(h1,…,ha^,…,hl)dXa. The column coefficient polynomials ∏b≠a(1+hbz) are linearly independent, since evaluating at z=−1/hc leaves only column c, with a nonzero value. Hence the Jacobian is invertible. A polynomial relation of minimal total degree, differentiated and multiplied by the inverse Jacobian over the rational function field, makes each of its partial derivatives a lower-degree relation; minimality and characteristic zero force the relation to be constant and zero. Thus the coordinates Pr,ij, 1≤r≤l, are algebraically independent. A highest weighted-degree part of an enveloping relation among their ordered lifts would contradict this polynomial independence by [F2]. This proves RTT PBW for all modes. The ha are scalar-matrix points in the symbol space, independently of spectral evaluation parameters.

2.2F1step 1.2constructalgebra

Group equal row lengths into the minimal admissible parabolic blocks ν, with final nonempty block m of size t. D/E/F below are its actual Gauss path coefficients. Deleting the last column embeds the smaller shifted matrix units into the current ones; on unshifted diagonal units this compensates the rho difference by a scalar translation, and on negative units it preserves χ. A dot denotes the smaller coefficients. With final column A, preceding column B, Lkj=E~(A,k),(A,j) and Chj=E~(B,h),(A,j), the right end recursions, for any fixed bottom row h, are Da;ij(r)=D˙a;ij(r)+δa,m(∑kD˙a;ik(r−1)Lkj+[D˙a;ih(r−1),Chj]), Ea;ij(r)=E˙a;ij(r)+δa,m−1(∑kE˙a;ik(r−1)Lkj+[E˙a;ih(r−1),Chj]), and Fa;ij(r)=F˙a;ij(r). The E boundary formula is used for r>1. Deleting the FIRST column of the reflected arrangement has the ordinary embedding on the remaining shifted factors. With first column A, next B, Lik=E~(A,i),(A,k) and Cih=E~(A,i),(B,h), its LEFT recursions are Da;ij(r)=D˙a;ij(r)+δa,m(∑kLikD˙a;kj(r−1)+[Cih,D˙a;hj(r−1)]), Ea;ij(r)=E˙a;ij(r), and Fa;ij(r)=F˙a;ij(r)+δa,m−1(∑kLikF˙a;kj(r−1)+[Cih,F˙a;hj(r−1)]), with r>1 in the F boundary formula. To verify these identities, cut each path at its final or initial visit to the added column. Paths missing that column give the dotted coefficient; paths ending or starting in its block give the product sum. For a crossing path the two neighboring cut positions at the common bottom row h have opposite signs and give the two orders in the commutator; further visits pair by moving to the neighboring cut. The identical cut rule in a changed row interval proves the Gauss identities: paths without an intermediate visit occur once; paths with such a visit have the two neighboring cuts with opposite sign. Thus these are identities for the actual Gauss coefficients. In particular LEFT deletion corrects F and leaves E unchanged; it does not use the interchanged E/F display in the source.

2.3F1step 1.4algebra

Finite spanning: earlier blocks and boundary E/F. In the abstract quotient by D1(r), r>p1, let Ωc contain D modes 1≤a≤c, 1≤r≤pa, E roots a<b≤c, sab<r≤sab+pa, and F roots a<b≤c, sba<r≤sba+pa; let Bc be their algebra. Induct on c to show every allowed mode with endpoints at most c belongs to Bc with total canonical degree at most its index. The case c=1 is the imposed truncation, including p1=0. For the inductive step put u=sc−1,c and v=sc,c−1. For r>u+pc−1, the D–E relation gives Ec−1(r)=[Dc−1(r−u),Ec−1(u+1)]−∑t=1r−u−1Dc−1(t)Ec−1(r−t). Replace every earlier D by its block-inductive finite expression and expand its commutator by Leibniz. The bracket of an earlier finite diagonal mode of index a with the lowest boundary E gives terms D(t)Ec−1(a+u−t) with a≤pc−1 in the only nonzero diagonal block, hence new E indices at most u+pc−1. An earlier finite root Eb,c−1(a) gives Eb,c(a+u) and any block-refinement split terms, all with a+u≤sb,c−1+pb+u=sb,c+pb. Earlier negative roots and earlier positive roots without endpoint c−1 commute with the lowest boundary E. Thus the expanded commutator is in Bc. In the sum u+1≤r−t<r, so induction on r reduces those E modes; all products have degree at most r. The reversed D–F relation and reversed product orders give the same argument with boundary bound v+pc−1.

3.1F1F2step 1.1step 2.1algebra

Loop symbols and shifted PBW. Give an RTT mode of index r loop degree r−1. In its commutator relation the term with a zero-index factor is the current matrix-unit bracket; every term with two positive-index factors has smaller loop degree. Thus the straightening in step 1.1 preserves loop degree, and the RTT basis of step 2.1 identifies each loop-filtered space with the span of its ordered monomials of bounded loop degree. Their symbols are therefore a basis, and their brackets are [eijta,ehktb]=δjheikta+b−δkiehjta+b. This identifies the loop graded algebra with U(gln[t]). The required current-algebra PBW uses only [F2]: any finite relation among ordered current monomials maps to a jet quotient gln[t]/tMgln[t] with M larger than every exponent in it, where the relevant modes are distinct basis vectors and their ordered monomials are independent. Coefficientwise Gauss inversion changes an RTT mode of index r only by products of at least two positive-index modes with total index r, whose loop degree is at most r−2. Hence the unshifted Gauss modes have these same current symbols. Sending each simple shifted Drinfeld generator to its unshifted namesake preserves the defining relations and is loop-filtered. For higher roots use their actual shifted commutator recursions: the upper recursion brackets ei,j−1tr−sj−1,j−1 with ej−1,jtsj−1,j, giving eijtr−1; the reversed lower recursion gives ejitr−1 in the same way. Thus the images of all allowed shifted root modes have the distinct current symbols of the unshifted loop algebra just established. Their ordered products are independent there by the jet-PBW argument, so a relation among their lifts, taken in its highest loop degree, is impossible. The shifted coefficient relations, adjacent-root recursions and Serre relations straighten words into these ordered root monomials, with commutator corrections of total canonical index at most r+s−1 for modes of indices r,s; induction on canonical degree and unordered pairs terminates the straightening. It preserves the canonical bound and the loop bound. Independence now proves both the embedding and the filtered ordered basis. Consequently the intrinsic canonical associated graded is the polynomial algebra on the allowed shifted root symbols. This does not identify those canonical symbols with the unshifted Gauss symbols: for s12=0,s23=1, the adjacent relation gives E13(2)(σ)=E13(2)(0)−E12(1)E23(1), whose correction has canonical degree two but loop degree zero. The independence argument uses loop degree one in this example. No independence after truncation is inferred here.

3.2step 1.2step 2.2algebra

Induct on the number of columns, deleting the last column in the original left-justified diagram and the first in the reflected diagram. A one-column diagram has no negative algebra, so every mode is invariant. Empty rows have only formal constants and zero positive coefficients. All earlier D blocks, all nonboundary E/F blocks, and F in right deletion or E in left deletion are unchanged by step 2.2. Their path monomials have no forbidden preceding-bottom target in right deletion, or following-bottom source in left deletion; commuting a new negative into such a monomial produces a negative unit of greater column distance with zero χ, and moving it to the right keeps this absent endpoint. Thus their projected brackets vanish. Induction supplies old-negative invariance of every dotted coefficient. The old negative algebra commutes with L and C in step 2.2, so its character ideal is preserved by those factors, proving old-negative invariance of the changed coefficients. The complete negative Lie algebra is generated by the old one and the new adjacent-column matrices: brackets through a row present in intervening bottom rows produce each longer negative matrix. Jacobi and the normalizer identity in step 1.2 propagate invariance from these generators. Only the new adjacent matrices need be checked below.

3.3F1step 1.4step 2.3algebra

Higher roots and the final diagonal elimination. For b<c−1, the defining root recursions are Eb,c(r)=[Eb,c−1(r−u),Ec−1(u+1)] and Fc,b(r)=[Fc−1(v+1),Fc−1,b(r−v)]. Reduce the earlier endpoint factors by the c−1 hypothesis; the same Leibniz bounds in step 2.3 place every new root in Bc, including high modes, using the finite allowed new roots in Ωc. Now use step 1.4 for Dc(r), r>pc. Every inverse earlier coefficient is in Bc−1 and every Dc(r−t) has smaller index, so induction on r treats its sum. First replace the upper Ec−1(r−v) by the finite expression just constructed, then expand the bracket with the lowest boundary F. Earlier D/F factors give bounded new F roots and earlier factors; earlier E factors commute with that boundary F. A finite new E root starting at c−1 has index a≤u+pc−1, so its E–F convolution has only Dc indices at most a+v≤pc. A new E root starting at b<c−1 gives earlier-endpoint roots and earlier factors, reduced by the block hypothesis, and cannot create a high Dc mode. Thus this commutator uses only Dc indices at most pc, and the induction closes with the asserted degree control. In particular higher diagonal modes are polynomial expressions, not zero modes.

4.1step 1.2step 2.2step 3.2algebra

The changed D^(1) is a sum of the row-pair diagonal-column blocks; its two adjacent-column projected commutators cancel. Let the neighboring column have height u≥t, with b=u−t shorter rows and cutoff x=n−t. In RIGHT deletion put z=E~(A,f),(B,g), f bottom and g arbitrary. In D^(2), and in boundary E^(2) when the shift is1, the single bridge contributes scalar −uδgiδfj. The bottom plus paths ∑kBikAkj contribute +tδgiδfj and matrix terms −δgiAfj+δfjBig for g bottom. The shorter minus paths in B contribute +bδgiδfj and +δfjBig for g shorter. Moving their negative factor through the following block yields one additional χ correction for each shorter row; this is the scalar b term. The single bridge gives the negative of all the matrix terms, and −u+t+b=0. In LEFT deletion put z=E~(B,f),(A,g), f arbitrary and g bottom. The bridge scalar is −tδgiδfj; bottom plus paths ∑kAikBkj give +tδgiδfj and −δgiBfj+δfjAig for f bottom. Shorter minus paths −∑hBihBhj give −δgiBfj for f shorter and NO scalar: the extra negative χ involves a shorter row h and bottom row g. The bridge has the opposite matrix terms. Therefore −t+t=0 and all matrices cancel, for D^(2) and boundary F^(2). Paths outside these adjacent columns have zero projection by the support argument in step 3.2. This proves the exact jump-one base cases in both actual LEFT reductions.

4.2step 1.2step 2.2step 3.2algebra

For a larger boundary shift, or a rectangle, the first two end columns have equal height t. A double dot deletes both and Ks;ij=D¨m;ij(s); replacing K with the corresponding boundary E¨ in RIGHT deletion or F¨ in LEFT deletion gives the same calculation. In RIGHT deletion call the last positions C,B,A, and write Bck=E~(B,c),(B,k), Akj=E~(A,k),(A,j), Chk=E~(C,h),(B,k), Jcj=E~(B,c),(A,j) and Hhj=E~(C,h),(A,j). Twice expanding step 2.2 expresses the changed r-mode as the sum of eight groups A0=Kr;ij, B0=∑cKr−1;icBcj, C0=[Kr−1;ih,Chj], D0=∑kKr−1;ikAkj, E0=∑k,cKr−2;icBckAkj, F0=∑k[Kr−2;ih,Chk]Akj, G0=∑cKr−2;icJcj, H0=[Kr−2;ih,Hhj]. For z=E~(A,f),(B,g) their projected brackets, in that order, are 0,−δfjKr−1;ig,0,+δfjKr−1;ig,R,S,−R,−S, where R=tδfjKr−2;ig−Kr−2;igAfj+δfj∑cKr−2;icBcg and S=δfj[Kr−2;ih,Chg]. The bracket in step 1.2 proves this table by moving each negative factor to the RIGHT. The t summation rows give the scalar in R; the bridge J gives its opposite because ρA−ρB=t. K lies in the twice-deleted p and commutes with z. The eight expressions cancel for EVERY r>1.

5.1step 1.2step 2.2step 3.2step 4.1algebra

At a RIGHT jump-one boundary, for a fixed earlier-block row g and r>1 the coefficient recursions in U(p) are Dm;ij(r+1)=[Fm−1;ig(2),Em−1;gj(r)]+∑s=0rD~m−1;gg(r+1−s)Dm;ij(s) and Em−1;ij(r+1)=[Dm−1;ig(2),Em−1;gj(r)]−∑fDm−1;if(1)Em−1;fj(r). Here D~(u)=−D(u)−1, with order-zero coefficient −I. The corresponding LEFT identities are Dm;ij(r+1)=[Fm−1;ig(r),Em−1;gj(2)]+∑s=0rDm;ij(s)D~m−1;gg(r+1−s) and Fm−1;ij(r+1)=[Fm−1;ig(r),Dm−1;gj(2)]−∑fFm−1;if(r)Dm−1;fj(1). These are algebraic coefficient identities, independent of invariance and generation. Expanding the E identity by the right end recursion gives E˙(r+1)+∑D˙(1)E˙(r), its product with L, and its commutator with C; collecting with step 2.2 gives E(r+1)+∑D(1)E(r). The left F expansion instead gives F˙(r+1)+∑F˙(r)D˙(1), its LEFT product with L and [C, ⋅ ], which collect to F(r+1)+∑F(r)D(1). The unchanged earlier D^(2) has no boundary endpoint and commutes with L,C. Expanding the boundary E–F bracket similarly gives the D identity: the coefficient convolution DD~=−I cancels paired split paths with opposite cut signs, leaving the changed D coefficient. Thus the recursions hold in both product orders. Every earlier D/inverse-D coefficient and the unaffected E or F coefficient is invariant by step 3.2; the changed base coefficients are invariant by step 4.1. Since the sum uses s≤r, induction on r proves invariance of ALL changed jump-one modes.

5.2step 1.2step 2.2step 3.2algebra

The REFLECTED calculation is a direct LEFT-ideal calculation, not an anti-map reversal of step 4.2. Call its first positions A,B,C, and write Lik=E~(A,i),(A,k), Bkc=E~(B,k),(B,c), Ckh=E~(B,k),(C,h), Jic=E~(A,i),(B,c), Hih=E~(A,i),(C,h). The eight groups are A0=Kr;ij, B0=∑kBikKr−1;kj, C0=[Cih,Kr−1;hj], D0=∑kLikKr−1;kj, E0=∑k,cLikBkcKr−2;cj, F0=∑kLik[Ckh,Kr−2;hj], G0=∑cJicKr−2;cj, H0=[Hih,Kr−2;hj]. For z=E~(B,f),(A,g) their projected brackets are 0,+δigKr−1;fj,0,−δigKr−1;fj,R′,S′,−R′,−S′, with R′=tδigKr−2;fj−δig∑cBfcKr−2;cj+LigKr−2;fj and S′=−δig[Cfh,Kr−2;hj]. For example [z,Lik]=δgiE~(B,f),(A,k), and moving this negative through B gives −δfkBkc+δfc; summing k gives the t term. The other part of the product bracket gives the L term. The bridge J has the opposite matrix terms and scalar ρA−ρB=−t; the F/H terms cancel because [z,Hih]=δgiCfh and z commutes with K. Thus every group is accounted for and cancels in the reflected LEFT reduction for EVERY r>1. If there are only two columns, K has only its formal constant coefficients and terms involving the third column vanish, so the same table applies.

6.1step 1.2step 3.2step 4.1step 5.1step 4.2step 5.2algebra

Steps 3.2, 4.1, 5.1, 4.2 and 5.2 cover every allowed parabolic D/E/F mode for the original and reflected arrangements. Refining a minimal block is its formal Gauss decomposition: coefficients of its inverse and resulting factors are polynomials in its previous coefficients, hence invariant by step 1.2. This gives all ordinary simple modes; higher-root commutator definitions give all higher roots. Therefore the actual untwisted-chart images Pii;i−1(r),Pi,i+1;i(r),Pi+1,i;i(r) and all their higher-root polynomials belong to their actual left reductions. This conclusion covers the infinite allowed mode families and does not rely on finite generation, finite truncation or a reflected W identification.

7.1F1F2step 2.1step 6.1algebra

Finite Levi Jacobian. Project U(p) to its column Levi enveloping algebra and take canonical symbols. At its diagonal point Xc=hcI, let Qi(z)=∏c≤pi(1+hcz). The diagonal D first variations are z∏a≤pi,a≠c(1+haz). For i<j, set m=pi, M=pj. A first variation in a common column c≤m has just one off-diagonal factor. Summing the same-column negative-cut repeats and the strictly increasing positive-cut visits in the path formula gives dEij(z)=z∏a=m+1M(1+haz)/(1+hcz) and dFji(z)=z/(1+hcz) on that entry. These are identities for the allowed coefficient derivatives, not an identification of excluded low product coefficients with shifted generators. Their coefficients in modes M−m+k and k, 1≤k≤m, are respectively (−hc)k−1∏a=m+1M(ha−hc) and (−hc)k−1. For higher roots, the canonical symbol of the adjacent root commutator is the Levi Lie–Poisson bracket. At Xc=hcI this Poisson tensor is zero, so the differential of a bracket uses only the two first differentials and the differential of the Poisson tensor. With i<k<j and pk=t, the coefficients from Eik(r−skj) and Ekj(skj+1) multiply to (−hc)a−1∏m<b≤t(hb−hc)∏t<b≤M(hb−hc) when r=M−m+a, since {Xc,ik,Xc,kj}=Xc,ij. For F the reversed recursion uses {Xc,jk,Xc,ki}=Xc,ji, with coefficients one and (−hc)r−1. Thus induction gives the displayed first variations for all higher roots as well. Choose the hc nonzero and pairwise distinct. Each row-pair block is Vandermonde with nonzero column factors; each diagonal block is the elementary-symmetric Jacobian from step 2.1. Different row pairs use disjoint entry variables, so the full Jacobian has rank ∑ijmin⁡(pi,pj). The corresponding finite symbols are algebraically independent by step 2.1's differentiation argument. Reflection reverses column order and interchanges E and F, giving the same invertible blocks with transposed shifts. Empty rows contribute zero-sized blocks.

8.1F2F3step 6.1step 7.1step 1.3algebra

The whole reduction is generated. Write W for the entire quantum Hamiltonian reduction, before any identification with a Yangian quotient. By [F3] its homogeneous Hilbert series is H(t)=∏i,j∏r=sij+1sij+min⁡(pi,pj)(1−tr)−1. Each weight is positive, so every coefficient is finite. Step 6.1 places every ordered finite-generator monomial of total degree at most d inside FdKW. Step 7.1 and enveloping PBW make these monomials independent: a highest-degree relation after Levi projection would give a polynomial relation among the independent symbols. Their number is exactly ∑k≤d[tk]H(t), which is also dim⁡FdKW by [F3] for the original pair and step 1.3 for the reflected pair. Thus their span equals FdKW for every d. Exhaustivity proves generation of the entire reduction and its ordered filtered basis, and also injectivity of the Levi projection on that entire algebra. The same homogeneous dimension equality proves full generation for the reflected reduction using its own allowed modes and transposed shifts. This uses the Gan–Ginzburg slice theorem independently of W-PBW, not just generic independence in a restricted subalgebra.

9.1F1F2step 2.2step 6.1step 8.1step 2.3step 3.3algebra

Relations, finite order and the whole-algebra identification. The end path identities prove the shifted coefficient relations and the D1 cutoff on the invariant representatives. One can check them after Levi projection, now injective on the entire reduction by step 8.1: the right end images are Da(r)↦D˙a(r)+δa,m∑kD˙a;ik(r−1)Lkj, Ea(r)↦E˙a(r)+δa,m−1∑kE˙a;ik(r−1)Lkj, and Fa(r)↦F˙a(r); the left versions place L before the dotted coefficients and correct F instead. Substitute these finite coefficient expressions in each D–D, D–E, D–F, E–F, equal-root and adjacent-root relation. Terms with no L give the smaller relation. Terms with one L give the smaller D-weight relation; terms with two L use [Lij,Lhk]=δjhLik−δkiLhj. The inverse-D convolution cancels paired split coefficients, and the adjacent triple relations group into those same terms and the matrix Jacobi identity. Hence the relations hold by column induction, starting with matrix-unit brackets at one column; injectivity lifts them back to the actual reduction. For D1 the cutoff row interval is empty, so every join is strictly forward; a path beginning and ending in row1 satisfies r=∑(c(bt)−c(at)+1)≤c(bs)−c(a1)+1≤p1. Thus the smallest-row path has no coefficient above p1, giving the actual D1 cutoff in either arrangement. There is therefore a homomorphism from the abstract truncated quotient onto the invariant-generated whole algebra. Steps 2.3 and 3.3 give finite spanning; commutator swapping lowers canonical degree, so induction on that degree and the number of unordered pairs straightens these finite expressions into ordered Ωn monomials. Their images are the independent ordered reduction basis of step 8.1, so the homomorphism is injective as well. This proves the quotient presentation and the finite Gauss PBW basis without restricting an infinite basis through a quotient.

9.2step 6.1step 1.3step 8.1constructalgebra

The full generator theorem just proved for BOTH arrangements now identifies the original head/right model. With the reflected-box anti-map τ from step 1.3, send a path (a1,b1),…,(as,bs) to (f(bs),f(as)),…,(f(b1),f(a1)). Each displacement is unchanged. A reversed join compares l+1−c(ak+1) with l+1−c(bk), so its strict-forward or weak-reverse rule is exactly the original one; its row is row⁡(ak+1)=row⁡(bk), preserving its sign. Total degree, number of factors and total sign are identical; the product order is precisely τ's reversal. This involutive bijection proves τ(Pij;x(r))=Pji;x′(r) for ALL i,j,x and modes r, including the diagonal constants at r=0. In particular τ exchanges simple E/F images and fixes the corresponding D images, transposing the shift matrix and preserving mode number. Since these explicit images generate each WHOLE reduction by step 8.1, both inclusions give τ(W)=W′, rather than only the image of a path subalgebra.

10.1step 1.3step 8.1step 9.1algebra

The preceding construction applies to both directional shift matrices, using the corresponding left or right end formulas in step 9.1. Thus it proves the full finite quotient basis, equality with the whole reduction, and strict canonical/Kazhdan filtration in both arrangements. Its degree-r homogeneous basis is the monomial basis counted by the exact slice Hilbert series, and the projection used for the relation check is injective on the entire reduction. These are the prerequisites for the original right-normalizer identification below.

10.2F1step 2.2step 9.1algebraconstruct

Actual original prefix coefficient identity. Let λm be the first m columns of the decreasing-column pyramid, I=Im−1:U(gm−1)↪U(gm) the ordinary UNSHIFTED box embedding, and ba(j) the box in row j and column a when it exists. Put negative-index coefficients zero and Tij(0)=δij. The original coefficient recursion, for r>0, is Tij(r)(λm)=I(Tij(r))−∑h≤n−qm, shj≤rI(Tih(r−shj))I(Thj(shj))+∑h>n−qmI(Tih(r−1))Ebm(h),bm(j)−[I(Tij(r−1)),Ebm−1(j),bm(j)], where coefficients inside I belong to λm−1 and shifts in the sum belong to λm. The final THREE terms are omitted for j≤n−qm, and a nonexistent box omits its term. To derive the identity before any cutoff is known, apply the right end identities to the last Gauss block in the ordinary chart. D has its smaller D plus its last-column Levi product and minus its previous-to-last bridge commutator; E has the same two corrections and starts with the smaller Eˉ. The precise smaller-block subtraction is Eˉa,b(u)=Ea,b(u)−∑c=ab−1Ea,c(u)Ec,b(s˙cb+1)u−s˙cb−1, all in the smaller diagram. For a shorter block c and last block b, s˙cb+1=scb. Insert these expressions into Tij(u)=∑(Fc,a(u)Dc(u)Ec,b(u))ij. Unchanged terms give the first embedded T; the Eˉ subtractions group by shorter terminal row h into the product with split (r−shj,shj); the L products group into the Levi sum. Leibniz groups the common bridge into the displayed single commutator. Higher-root end identities follow by their adjacent recursion; its earlier-block factor has no terminal bridge endpoint, so its bracket with that bridge is zero. This proves the prefix identity itself and retains its actual coefficient index.

11.1F1F2F3step 3.1step 8.1step 10.1algebra

The two graded algebras. The shifted root relations give the current brackets on the allowed modes eijta, a≥sij; shift additivity makes their span a Lie subalgebra. Step 3.1 identifies its ordered enveloping basis with the intrinsic loop-filtered basis, proving gr⁡LYn(σ)=U(gln[t](σ)). Canonical degree instead gives the commutative polynomial algebra of step 3.1. For the finite reduction the Kazhdan associated graded is the commutative slice algebra from step 8.1, while the leading single-factor terms of the finite generators lie in the actual centralizer ge⊆p; the next theorem identifies the loop graded algebra by ambient enveloping PBW. Noncommutativity distinguishes the two graded algebras whenever the corresponding Lie algebra is nonabelian.

11.2F1step 10.2algebra

Every coefficient above the bound is zero. For the original decreasing-column diagram Sij=sij+min⁡(pi,pj)=pj for EVERY ordered row pair. Induct on the column count m using step 10.2; the one-column T has no coefficient above one directly. An empty row contributes only a diagonal constant. If j≤n−qm, its row length is unchanged on removal, so the only embedded T term vanishes for r>pj by induction. If j is a bottom row, pj=m, and the first embedded T vanishes for r>m because its smaller target-row length is m−1. In each shorter-row product, ph is unchanged and shj=m−ph, so r−shj>ph=Sih(λm−1) for ANY i, killing its first factor. In the Levi sum every h has smaller row length m−1, and r−1>m−1=Sih(λm−1) kills its coefficient. The same inequality kills the T coefficient inside the final commutator. This covers every term, including the boundary r=m+1, and proves Tij(r)=0 for r>Sij. The lower zero range 0<r≤sij follows coefficientwise from FDE and shift additivity. No truncation fact was assumed to prove itself.

12.1F1step 3.3step 9.1step 11.2algebra

Finite T coordinates and loop symbols. Coefficientwise FDE and Gauss inversion are weighted triangular in the original index r: the mode equals its corresponding Gauss coordinate plus products of smaller mode indices of total canonical degree r. The finite Gauss eliminations from steps 2.3 and 3.3 and the actual cutoff in step 11.2 close both inversions on exactly the finite set. Thus these finite canonical symbols are another polynomial coordinate system, and the ordered finite T monomials have the same filtered basis as the Gauss monomials in step 9.1, in any prescribed order. A signed path term with k factors and coefficient index r has ambient good degree at most r−k; scalar replacements lower it further. Only its single-factor part contributes in degree r−1, giving (−1)r−1∑row⁡(a)=i,row⁡(b)=j, c(b)−c(a)=r−1Eab=(−1)r−1eij;r−1. Products introduced by Gauss inversion have at least two factors and smaller good degree. This proves the symbol dictionary with the existing coefficient index and no spectral rescaling.

12.2step 9.2algebra

Put ηhead(Eab)=Eab+δab(n−∑d≤c(a)qd). This and ηtail are algebra automorphisms: a matrix bracket can have diagonal part only from Eab,Eba∈p, which forces equal columns and equal diagonal shifts, so the scalar functional kills the commutator; the negative scalar translation is the inverse. Reflection gives ∑d≥c′(f(a))qd′=∑d≤c(a)qd, hence τηhead=ηtail′τ. Also τ(m)=m′, χ′τ=χ by the trace calculation, and τ(IχU(g))=U(g′)Iχ′, since τ reverses products and sends each shifted negative generator to its reflected one. Therefore τ([ηhead(u),x])=[τ(x),ηtail′(τ(u))]. Bijectivity shows that u satisfies the ORIGINAL head/right condition exactly when τ(u) belongs to the reflected LEFT reduction. Step 9.2 identifies its inverse image with the original W, proving BOTH inclusions in W={u:[ηhead(u),m]⊆IχU(g)}. The induced Gauss transpose also satisfies τ(Tij(r))=Tji′(r): apply the coefficientwise reversed FDE factors and their Gauss cut identities. Thus step 11.2 gives the reflected upper cutoff r>Sji=Sij′, with the same finite triangular T basis. This proves right invariance for every original shifted generator, higher-root mode and product, beyond the numerical identity ηhead−ηtail=−tr⁡mad⁡.

13.1step 1.3step 12.2algebra∎

Write JL=U(g)Iχ and JR=IχU(g). The identities (x−χ(x))ηtail(w)=ηtail(w)(x−χ(x))+[x,ηtail(w)] and ηhead(w)(x−χ(x))=(x−χ(x))ηhead(w)+[ηhead(w),x] prove JLηtail(w)⊆JL and ηhead(w)JR⊆JR for every w∈W. Thus QL=U(g)/JL has its actual right action a‾⋅w=aηtail(w)‾, and QR=U(g)/JR its actual left action w⋅a‾=ηhead(w)a‾, commuting with the respective enveloping actions by associativity. These are module quotients, not quotient rings. Right Whittaker vectors act by v⋅w=vηhead(w) because they annihilate J_R. Turning a right U(g)-module into a left reflected module by a′v=vτ−1(a′) identifies its right Whittaker space and W action with the reflected left ones, using τ−1ηtail′τ=ηhead. For consumers assuming AC, transporting their proved left Skryabin equivalence through the reflected Lie isomorphism in step 1.3 and then this anti-map gives the right equivalence with inverse −⊗WQR; that conditional categorical assertion is separate from the choice-free algebra identity. Every action is the explicit original or reflected chart action; no equality of different twists on an arbitrary fixed representation is assumed.

Remarks

  • The independence argument is a finite-dimensional PBW argument in disguise: any finite relation involves finitely many modes, and mapping the corresponding finitely many generators to a jet Lie algebra makes their PBW images independent. No PBW theorem for the infinite-dimensional current algebra is assumed.

  • The two related graded algebras are a recurring source of errors: the symbolic degrees of the Kazhdan filtration are the coordinates of the Slodowy slice, while the loop degrees are current-algebra degrees; the double centralizer arguments on this page use the loop filtration.

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

Skryabin's equivalence for the type-A Whittaker pair

Statement

Assume the Axiom of Choice The Axiom of Choice, inherited from assertion (2) of the good-grading cohomology supplier.

Let (g,p,h,m,e,χ), W(λ), Qχ and C(λ) be as in The type-A finite W-algebra and the Whittaker category. Then the functor Qχ⊗W(λ)− ⁣:W(λ)-mod→C(λ) is an equivalence of categories, with inverse the Whittaker-vector functor Wh; in particular Wh is exact and Wh(M)=0 implies M=0 for M∈C(λ).

For every finite-dimensional g-module X, the exact functor ?⊗X ⁣:C(λ)→C(λ) transports to the exact functor M⊛X=Wh((Qχ⊗W(λ)M)⊗X) on W(λ)-mod, and whenever M is a p-module viewed as a W(λ)-module by restriction, the natural map μM,X ⁣:M⊛X→M⊗X,(η(u)1χ⊗m)⊗x↦um⊗x, is an isomorphism of W(λ)-modules. The associativity isomorphisms (M⊛X)⊛Y≅M⊛(X⊗Y) are compatible, and for the one-dimensional p-module Cc the resulting isomorphism μd ⁣:Cc⊛V⊛d→Vc⊗d is independent of the order of the composed associativity isomorphisms.

Facts & Assumptions

Given: The pyramid data, the bimodule Qχ and the Whittaker category of The type-A finite W-algebra and the Whittaker category, and a finite-dimensional g-module X. Assume AC The Axiom of Choice for the arbitrary-module equivalence and transported tensor assertions.

[F1]

For every W(λ)-module M, the twisted m-cohomology of Qχ⊗W(λ)M vanishes in positive degrees and its degree-zero part is M; for M∈C(λ) the invariants detect vanishing (Gan-Ginzburg and Skryabin inputs for the type-A pyramid good grading).

[F2]

Qχ=U(g)/U(g)Iχ is a (U(g),W(λ))-bimodule, and tensoring the canonical element 1χ with a W(λ)-module gives a left adjoint to Wh; the unit and counit are the natural maps M→Wh(Qχ⊗W(λ)M), v↦1χ⊗v and Qχ⊗W(λ)Wh(M)→M, u1χ⊗v↦uv (The type-A finite W-algebra and the Whittaker category, Universal enveloping algebra).

[F3]

Chevalley-Eilenberg exactness: tensoring with a finite-dimensional g-module preserves the Whittaker category and is exact, and the long exact cohomology sequence computes the cohomology of extensions (Chevalley–Eilenberg cochains, Long exact sequence in Lie algebra cohomology).

[F4]

Finite-dimensional g-modules have finite m-flags with trivial successive sections. Indeed the column-grading diagonal element H satisfies [H,x]=rx on gr; negative homogeneous generators shift its finitely many generalized eigenvalues by negative integers. Sufficiently long products from m therefore vanish. Induction on the module dimension, choosing a vector in the common kernel and passing to the quotient, gives 0=X0⊂⋯⊂Xt=X with mXj⊆Xj−1 (The type-A nilpotent pyramid, good grading and Whittaker character, Classical complex matrix Lie algebras).

Proof

technique · direct

Given: The bimodule Qχ, a W(λ)-module M, a finite-dimensional g-module X, and the maps μM,X; assume AC as specified above.

1.1F1F2F3algebra

Unit, membership and counit. The shifted m action on Qχ lowers the bounded-below Kazhdan filtration: (x−χ(x))u1χ=[x,u]1χ, and for negative doubled degree −2r the commutator lowers filtration by 2r>0. This proves local nilpotence on Qχ⊗WM too, so the adjunction lands in C(λ). By [F1], its unit M→Wh(Qχ⊗WM) is an isomorphism. For N∈C(λ), the triangle identity makes Wh(cN) an isomorphism. Left exactness gives Wh(ker⁡cN)=0, hence ker⁡cN=0 by detection. Now the short exact sequence with this injective counit has H1 of its domain zero by [F1]; its cohomology sequence gives Wh(coker⁡cN)=0. Detection makes that cokernel zero. Thus the unit and counit are isomorphisms, proving the equivalence without presuming exactness of Wh.

1.2F1F2algebra

Exactness and detection. Exactness of Wh follows because it is inverse to the exact functor Qχ⊗W(λ)− (tensoring with the right-free module Qχ proved in the local cohomology supplier [F1]), and the detection statement is the case H0=0 of [F1].

1.3F1F3algebra

The transported tensor functor. For M∈W(λ)-mod and finite-dimensional X, the functor M↦Wh((Qχ⊗W(λ)M)⊗X) is exact in M because the composed functors are exact; it is the transport of ?⊗X across the equivalence.

2.1F1F3F4step 1.1constructalgebra

Invertibility of the displayed tensor map. Let M be a p-module and put N=Qχ⊗WM. PBW gives representatives η(u)1χ, and ψM(η(u)1χ⊗m)=um is balanced because right multiplication by η(w) changes u to uw. Hence μM,X=(ψM⊗1)∣Wh is a defined linear map. Use [F4]'s finite flag of X. Each quotient of N⊗Xj by N⊗Xj−1 is a finite direct sum of N, with trivial m action on its finite factor. By [F1] it has vanishing positive twisted cohomology and invariants M⊗(Xj/Xj−1). Induction and the long exact sequence give the same vanishing on each N⊗Xj, and give short exact sequences on their invariant spaces. The map μ preserves these filtrations. On each successive quotient, the invariants are represented by 1χ⊗m⊗xˉ and ψM sends them to m⊗xˉ. Thus its quotient maps are identities; induction through the finite short exact sequences makes μ bijective. This argument holds for arbitrary M and needs no cofree realization or completion of M.

2.2F3step 1.1step 1.3algebra

Associativity. The associativity isomorphisms of the transported functor are obtained by inserting the canonical associativity isomorphisms of the tensor product of g-modules into the definition of ⊛ and applying the inverse equivalence; they are compatible by the naturality of the unit and counit of the adjunction and by the coherence of the tensor associativity in C(λ).

3.1F2F4step 2.1algebra

Balancing and W-linearity. PBW gives unique representatives η(u)1χ, u∈U(p), in Qχ. Define ψM(η(u)1χ⊗m)=um. Since the right action of w∈W⊂U(p) sends this representative to η(uw)1χ, the formula is right-W-balanced: (uw)m=u(wm). Moreover ψM(η(v)q⊗m)=vψM(q⊗m) for v∈U(p). The shift η adds a Lie character on p, so on its primitive generators, and hence multiplicatively on U(p), (η⊗id)Δ(v)=Δη(v). The W action on the source Whittaker subspace is therefore Δη(w), while the target restricted p-module M⊗X has action Δ(w). Applying ψM⊗id to the displayed coproduct identity proves μM,X(wz)=wμM,X(z). Together with step 2.1 this proves the actual stated W-module isomorphism. No equality with cofree evaluation or citation-only character-equation argument is used.

4.1step 2.1step 3.1step 2.2algebra∎

Independence of the order. For X=V⊗d the isomorphism μd is the composite of the single-step maps μ∙,V; two different parenthesizations differ by the associativity isomorphisms of step 2.2, and both are restrictions of the balanced evaluation maps of step 3.1, applied with the same iterated coproduct on U(p); coassociativity and the displayed shift identity make these maps equal. Therefore the resulting isomorphism Cc⊛V⊛d→Vc⊗d is independent of the composed associativity isomorphisms.

Remarks

  • The displayed tensor map is the balanced p-module evaluation map. Its invertibility follows from the finite m-flag and cohomology sequence in step 2.1; no identification with constant evaluation in a cofree model is required.

  • The equivalence is exact but its left adjoint in the Schur-functor constructions later on this page is not the naive tensor functor; those constructions use the projective generator T of a single block, treated later.

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The loop filtration on the type-A finite W-algebra has associated graded U(g^e)

Statement

Equip W(λ) with the loop (good) filtration FrW(λ)=W(λ)∩⨁s≤rU(p)s induced by the pyramid grading p=⨁r≥0gr of The type-A nilpotent pyramid, good grading and Whittaker character, and likewise for the shifted Yangian of The shifted Yangian and the pyramid generators of the type-A finite W-algebra. Then the associated graded algebra gr⁡W(λ) is canonically isomorphic to the enveloping algebra U(ge), viewed as a graded algebra via the restriction of the pyramid grading, and the isomorphism sends the leading symbol of the generator Ti,j(r+1) to (−1)rei,j;r, where the ei,j;r are the centralizer basis of the pyramid. In particular W(λ) is a filtered deformation of U(ge), the loop filtration is separated, and the ordered monomials in the generators Ti,j(r+1), (i,j,r)∈K, form a basis of W(λ).

This filtration is not the Kazhdan filtration: the Kazhdan filtration has associated graded the commutative Slodowy-slice algebra C[S], while here gr⁡W(λ)=U(ge) is noncommutative in general.

Facts & Assumptions

Given: The pyramid λ, the finite W-algebra W(λ) with its generators Ti,j(r+1) and loop filtration, and the centralizer basis ei,j;r, (i,j,r)∈K.

[F1]

The ordered monomials in the finite T-modes si,j<r≤Si,j form a PBW basis of W(λ), and the loop degree of Ti,j(r+1) is r (Ordered monomial PBW basis for the shifted Yangian, The shifted Yangian and the pyramid generators of the type-A finite W-algebra).

[F2]

The leading symbol of Ti,j(r+1) in the loop filtration is (−1)rei,j;r; the elements ei,j;r with (i,j,r)∈K form a basis of the centralizer ge and have brackets computed by expanding their sums in the ambient matrix-unit commutator (The shifted Yangian and the pyramid generators of the type-A finite W-algebra, The type-A nilpotent pyramid, good grading and Whittaker character).

[F3]

Ordered monomials in a basis of a finite-dimensional Lie algebra form a PBW basis of its enveloping algebra (PBW gives an ordered monomial basis for the enveloping algebra); the associated graded of a filtered algebra is computed from the leading symbols of a filtered basis (Associated graded algebra of a filtered algebra).

[F4]

The Kazhdan filtration of the Gan-Ginzburg construction has associated graded the commutative coordinate ring of the Slodowy slice, not the enveloping algebra of ge (Ordered monomial PBW basis for the shifted Yangian).

Proof

technique · direct

Given: The PBW basis and leading-symbol data of [F1]-[F2].

1.1F1F2algebra

Actual ambient leading term. Give a matrix unit ea,b∈p its good degree col⁡(b)−col⁡(a). In the explicit signed path formula a term of canonical degree r+1 with k matrix-unit factors has good degree at most r+1−k; a diagonal scalar replacement only lowers that degree. Therefore only single-factor terms contribute in good degree r. Those terms sum to (−1)r∑ea,b over row⁡(a)=i, row⁡(b)=j, col⁡(b)−col⁡(a)=r, namely (−1)rei,j;r. Products introduced by Gauss factorization or its inverse have at least two factors and have smaller good degree. Thus the leading homogeneous component of Ti,j(r+1) in the actual graded algebra U(p) is exactly (−1)rei,j;r. This proves the leading-symbol claim using the path degrees rather than a claim that Gauss inversion alone supplies its sign.

1.2F2F3algebra

Independence in the ambient enveloping algebra. The elements ei,j;r form a homogeneous basis of the actual Lie subalgebra ge⊆p. Extend that finite basis to a homogeneous basis of p, with an order extending the prescribed order of the centralizer basis. Enveloping PBW implies that the ordered monomials in the ei,j;r are linearly independent in U(p), and that the natural homomorphism U(ge)→U(p) is injective. Their products and brackets are the actual ambient products and brackets, including all boundary terms of the centralizer strings. No projection of a current bracket with an arbitrary out-of-range convention is needed.

2.1F1step 1.1step 1.2algebra

Strictness of the loop basis. The finite T monomials form a vector-space basis of W(λ) by [F1]. For a monomial with total loop degree d, step 1.1 says that its degree-d homogeneous component in U(p) is, up to the product of its displayed signs, the corresponding PBW monomial in U(ge). In any nonzero finite linear combination of T monomials, take the largest total loop degree d. The degree-d homogeneous component is nonzero by step 1.2, even when degree-zero generators occur. Thus that combination belongs to ⨁s≤dU(p)s and not to ⨁s<dU(p)s. Consequently the intersection filtration in the Statement is exactly the span of T monomials of total loop degree at most d, and their degree-d symbols form a basis of its associated graded. This verifies symbol independence directly, rather than inferring it from independence of filtered elements.

3.1F3step 1.1step 1.2step 2.1algebraconstruct

The graded algebra isomorphism. For any subalgebra of a nonnegatively graded algebra with its intersection filtration, taking highest homogeneous components embeds its associated graded into that graded algebra: if a representative's component of degree d is zero it already lies in filtration d−1, and multiplication agrees with multiplication of homogeneous components. Apply this to W(λ)⊆U(p). Step 2.1 identifies its image with the span of the ordered monomials in ge, which is precisely the embedded algebra U(ge) from step 1.2. Hence gr⁡loopW(λ)≅U(ge), and the identification sends the symbol of Ti,j(r+1) to (−1)rei,j;r as asserted.

4.1F1F4step 2.1step 3.1algebra∎

Filtration and the second graded algebra. Each generator has finite nonnegative good degree, and each element is a finite sum of T monomials, so the loop filtration is exhaustive and bounded below with F−1=0. The actual homogeneous decomposition in U(p) and step 2.1 give separatedness. The finite basis is already established in [F1], and step 3.1 establishes its filtered deformation property. Independently, the Kazhdan filtration uses positive weights col⁡(b)−col⁡(a)+1 on p and has associated graded C[S] by [F4]; in the doubled convention its weights are twice these. That graded algebra is commutative, whereas U(ge) is noncommutative whenever ge is nonabelian. These are the two claimed filtrations and their respective graded algebras.

Remarks

  • The index shift is part of the statement: the generator with loop degree r is Ti,j(r+1), and its symbol is (−1)rei,j;r. The coefficient index of the source series is r+1, and no additional rescaling is applied.

  • The affine-Yangian proof notes expand the coefficient bookkeeping of steps 1.1-1.2 (Gauss inversion signs and the finite range); the finite-W matrix proof contains the tensor-model check of the same symbol assignment.

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The degenerate cyclotomic Hecke algebra

Definition

Let Hd be the degenerate affine Hecke algebra of The degenerate affine Hecke algebra and let a=(a1,…,al) be a multiset of complex numbers, l≥1. The degenerate cyclotomic Hecke algebra is H0(a)=C for d=0, and for d≥1 is the quotient Hd(a):=Hd/(∏j=1l(x1−aj)), the two-sided ideal being the one generated by the displayed polynomial (Left, right and two-sided ideals, The ideal generated by a subset and principal ideals, For a two-sided ideal I, the additive cosets form a ring R/I with identity 1+I).

Assume the Axiom of Choice The Axiom of Choice for the tensor-realization verification below; the quotient definition itself is choice-free.

The verification below records the structure of Hd(a) used on this page. A C-basis is given by the ordered monomials x1r1⋯xdrdw,0≤r1,…,rd<l, w∈Sd, so that dim⁡Hd(a)=ldd!; the polynomial-degree filtration has associated graded the algebra C[x1,…,xd]/(x1l,…,xdl)⋊C[Sd]. For integral roots aj∈Z this is the cyclotomic quotient Hd(Λ) attached to the dominant weight Λ=∑jmjΛj of the integer type-A root system, with mj=#{i:ai=j}; for general complex roots one uses a separate integer chain in each coset of C/Z, and the symbol Λa denotes a formal fundamental weight on that chain, not an index of the integer-only lattice. The pyramid roots of the finite-W-algebra constructions are aj=cj+qj−n for the origin c=(c1,…,cl) and the pyramid columns q1≥⋯≥ql. If l=1, then xj=a1+∑k<j(k j) in the quotient. The generator-fixing anti-involution of Hd descends to Hd(a). The top coefficient functional of the monomial basis is a nondegenerate symmetric trace on Hd(a), and it restricts to a nondegenerate trace on every central block corner.

Facts & Assumptions

Given: The degenerate affine Hecke algebra Hd, a multiset a=(a1,…,al) of arbitrary complex numbers with l≥1, and its quotient A=Hd/(f(x1)), where f(t)=∏j(t−aj) and the ideal is two-sided. Assume AC The Axiom of Choice for the Skryabin/tensor realization used in PBW independence.

[F1]

The affine ordered monomials form a basis, xi commute, and the cross relations are sixi+1=xisi+1 and sixi=xi+1si−1. Its generator-fixing anti-involution exists (The degenerate affine Hecke algebra).

[F2]

The pyramid construction provides g,p,m,e,χ and the automorphism η(Eab)=Eab+δab(n−∑h≥col(a)qh). The Whittaker bimodule is Qχ=U(g)/U(g)Iχ with right W-action by η. PBW identifies it as a vector space with U(p) (The type-A nilpotent pyramid, good grading and Whittaker character, The type-A finite W-algebra and the Whittaker category, PBW gives an ordered monomial basis for the enveloping algebra).

[F3]

For any p-module M and finite-dimensional g-module X, the tensor-isomorphism of Skryabin's equivalence for the type-A Whittaker pair identifies Wh((Qχ⊗WM)⊗X) with M⊗X by (η(u)1χ⊗m)⊗v↦um⊗v. These identifications are natural and compatible with tensor associativity. No cyclotomic quotient is part of this input.

[F4]

The Casimir operators on M⊗V⊗d satisfy the affine Hecke relations, commute with g, and therefore restrict to Whittaker vectors; their naturality transports them through F3 (The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations).

[F5]

Filtered leading symbols multiply in the associated graded (Associated graded algebra of a filtered algebra).

Proof

technique · direct

Given: A=Hd/(f(x1)), the polynomial-degree filtration, and F1–F5; assume AC for F3 and the transported representation.

1.1F1algebra

Bounded spanning in every variable. For each r, put wr=sr−1⋯s1 (and w1=1). In the affine algebra the cross relations give wrx1wr−1=xr+ terms of polynomial degree zero. Hence wrf(x1)wr−1=xrl+ terms of degree at most l−1. This element is zero in A. Every affine ordered monomial with an exponent at least l can therefore have a factor xrl replaced by terms of strictly smaller total polynomial degree; straightening those terms never increases that degree. Induction on total degree, applied to every such replacement, expresses every monomial as a linear combination of x1r1⋯xdrdw with 0≤ri<l. The same induction proves that FmA is spanned by bounded monomials of degree at most m.

1.2F2F3F4construct

A realization for arbitrary complex roots. For d≥1 choose an integer n≥d and the rectangular partition λ=(l,…,l) with n rows, so every column has height qj=n and e has n strings of length l. On p define the one-dimensional module Ca by Eab↦δabacol(a). This is a Lie character: it vanishes on the strictly positive nilradical and is aj times the trace on the jth Levi block. In particular no integrality or coset condition on aj is needed. Restrict this module to W and use F3 with X=V⊗d. Restrict the affine Hecke operators on (Qχ⊗WCa)⊗V⊗d to Whittaker vectors, then transport through F3. This defines an affine Hecke action on Va⊗d=Ca⊗V⊗d; the si are place permutations. The following step computes x1 before asserting any quotient factorization.

1.3F2F3F4step 1.2algebra

The transported first operator. Write Qc=Qχ⊗WCa and define πc:Qc→C by πc(η(u)1χ⊗1)=u⋅1. It is well defined: the right W-relations become multiplication by the restricted character, and PBW gives representatives η(u)1χ. For a tensor basis vector vj write its unique Whittaker preimage under F3 as z=∑izi⊗vi, with zi∈Qc. Then πc(zi)=δi,j. If col(a)≤col(b), then Eab∈p and πc(Eabzi)=δab(acol(a)+∑h≥col(a)qh−n)δi,j, since η−1(Eab)=Eab−δab(n−∑h≥col(a)qh). If col(a)>col(b), the Whittaker equation for Eab instead gives Eabzi=χ(Eab)zi−∑kzk, where k runs over tensors obtained from i by replacing an occurrence of a by b. Apply πc⊗1 to Ω01z=∑a,b,iEabzi⊗Eba(1)vi. The terms with col(a)≤col(b) give (acol(j1)+∑h≥col(j1)qh−n)vj. The χ term gives vL1(j), because χ(Eab)=1 exactly when b=L(a). In the negative sum, replacing the first occurrence gives −∑h>col(j1)qh vj; replacing an occurrence in position k>1 gives −vj⋅(1 k) exactly when col(jk)<col(j1). Consequently the transported right action is vjx1=vL1(j)+(acol(j1)+qcol(j1)−n)vj−∑k>1: col(jk)<col(j1)vj⋅(1 k). Here a nonexistent left-shift term is zero. In our rectangle qj=n, so the diagonal coefficient is precisely acol(j1).

2.1F1F5step 1.3algebra

The cyclotomic relation and the leading symbols. Let Ck be the span of tensors whose first entry has column at most k, with C0=0. Step 1.3 gives Ck(x1−ak)⊆Ck−1: both the left shift and every exchange strictly lower the first column, while x1 preserves Ck−1. Thus successively applying (x1−al),…,(x1−a1) kills Cl=V⊗d. The factors commute, so f(x1)=0 and the action factors through A. Grade V by deg⁡vb=l−col(b) and give its endomorphism algebra the induced filtration. In step 1.3 the left shift has degree one and every other term has total tensor degree zero. Hence gr⁡1x1=e1. The recursion xj+1=sjxjsj+sj shows by induction that all xj are filtered of degree one with leading symbol ej, and that sj have degree zero with symbols the place permutations.

3.1F1F5step 1.1step 2.1algebra

Independence and the associated graded algebra. The cross relations and the conjugated relations in step 1.1 give a surjection B=C[X1,…,Xd]/(X1l,…,Xdl)⋊C[Sd]↠gr⁡A. Its composite with the associated graded tensor representation is Xj↦ej, w↦ place permutation. Choose the rightmost box in each of d distinct rows and let v be the tensor of those boxes. For bounded r and w, the vectors ve1r1⋯edrdw are distinct tensor basis vectors: their row labels identify the permutation, and their columns identify all ri. Therefore this composite is injective. It follows that B≅gr⁡A. Taking leading symbols of a hypothetical linear relation among bounded monomials, first in its largest total degree and then inductively, proves their independence. Along with step 1.1 this gives the claimed PBW basis, its filtration compatibility, and dim⁡A=ldd!. The longest strings have length l, the number of columns, and there are n=ql≥d of them; no column height is used as their length. For d=0 the algebra, basis and associated graded are all C, so the assertions hold directly.

4.1step 1.3step 3.1algebra

Integral roots and the pyramid dictionary. For integral roots write mi=#{j:aj=i}; then f(x1)=∏i(x1−i)mi, the quotient attached to Λ=∑imiΛi. For arbitrary complex roots the same algebraic definition applies, with integer-chain bookkeeping separately in each coset of C/Z. The rectangle above has cj=aj and qj=n, hence aj=cj+qj−n; the general pyramid dictionary is the displayed diagonal term of step 1.3. No general complex root is identified with an integer-only fundamental-weight index.

4.2F1step 3.1algebra

Level one and the anti-involution. For l=1, x1=a1 and xj+1=sjxjsj+sj give xj=a1+∑k<j(k j) by induction; the basis of step 3.1 identifies the quotient with C[Sd]. The generator-fixing anti-involution fixes f(x1) and preserves its two-sided ideal, so descends to A.

4.3F5step 3.1algebra

The graded top pairing. Put D=d(l−1) and T=x1l−1⋯xdl−1. Let τ0:B→C be the coefficient of X1l−1⋯Xdl−1⋅1. For graded monomials Xrw,Xsv, this coefficient is one exactly when wv=1 and r+w(s)=(l−1,…,l−1), and is zero otherwise. The equivalent reversed condition is vw=1 and s+w−1(r)=(l−1,…,l−1); thus τ0 is symmetric. Each basis element pairs with its unique complementary element, so the pairing is perfect, including between degrees m and D−m. Define τ:A→C as the coefficient of T⋅1 in the PBW basis. By filtration compatibility τ=τ0∘gr⁡D on A=FDA, and it vanishes on FD−1A. Therefore, if a∈FmA and b∈FD−mA, then τ(ab)=τ0(gr⁡m(a)gr⁡D−m(b))=τ(ba). This establishes cyclicity only under the stated degree bound so far.

5.1F1step 4.3algebra

Full generator cyclicity. Since permutations have degree zero, step 4.3 gives τ(aw)=τ(wa) for every a∈A, w∈Sd. To check τ(xib)=τ(bxi) for all bounded basis monomials b, step 4.3 suffices when deg⁡b<D. The remaining ones are exactly b=Tw. The polynomial T is central: it commutes with the xj, and the cross relations directly give sj(xjxj+1)=(xjxj+1)sj, while sj commutes with the other variables. Hence sjT=Tsj. Applying the already proved permutation cyclicity twice gives τ(xiTw)=τ(wxiT)=τ(wTxi)=τ(Twxi). This proves cyclicity with every generator on every element; successively moving generators of a word from the beginning to the end proves τ(ab)=τ(ba) for all a,b∈A. It also covers l=1 (where T=1 and D=0).

6.1F5step 4.3step 5.1algebra∎

Nondegeneracy and block restriction. For 0≠a∈A, take its largest filtration degree m, so gr⁡m(a)≠0. By the perfect graded pairing of step 4.3 choose homogeneous b0∈BD−m with τ0(gr⁡m(a)b0)≠0, and lift it to b∈FD−mA. Then τ(ab)≠0. Thus the pairing has zero left radical, and symmetry gives zero right radical; this proves nondegeneracy without claiming that products of excess total degree have zero trace. If e is a central idempotent and 0≠a∈eA, choose b as above; then τ(aeb)=τ(ab)≠0, so the restriction to eA=eAe is nondegenerate and symmetric as well.

Remarks

  • The integer and nonintegral cases are kept separate on purpose: the integral case is the classical cyclotomic quotient of the type-A root system, while the general complex roots are handled through the pyramid realization whose columns are chosen large enough to make the tensor action faithful.

  • The trace of steps 4.3, 5.1 and 6.1 is the top PBW coefficient functional; it is the tool that rules out nonzero ideals in the radical in the double centralizer arguments on this page.

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The deformed tensor space for the type-A finite W-algebra

Definition

Fix the pyramid λ=(0≤p1≤⋯≤pn) with columns q1≥⋯≥ql, its box-labelled natural module V=CN, an arbitrary origin c=(c1,…,cl)∈Cl, and d≥0. Assume AC The Axiom of Choice for the imported Skryabin and Vust inputs. For X∈p define the column-trace character κc(X)=∑b=1lcbtr⁡(Xbb), where Xbb is its bth column-Levi diagonal block. Write ηc(X)=X+κc(X)1 for the resulting automorphism of U(p), so ηc(ea,b)=ea,b+δa,bccol⁡(a). Let Cc be the corresponding one-dimensional p-module and set ab=cb+qb−n and Λ=∑b=1lΛab, with a separate integer chain for each complex coset as in The degenerate cyclotomic Hecke algebra.

The truncated (deformed) tensor space Ec=Vc⊗d is E=V⊗d with the left U(p)-action obtained by composing the ordinary total tensor representation ρd with ηc. Equivalently it is Cc⊗V⊗d, with one character factor; the origin twist is applied once to the total action. For d≥1 its right Hd(Λ)-action is determined by place permutations si and x1↦(e+∑j=1N(ccol⁡(j)+qcol⁡(j)−n)ej,j)⊗1⊗(d−1)−∑k=2d∑col⁡(i)<col⁡(j)ei,j⊗1⊗(k−2)⊗ej,i⊗1⊗(d−k), with xj+1=sjxjsj+sj. Here the generator-fixing anti-involution of the Hecke algebra converts the displayed operators into a right action. For d=0 there are no xj,si, H0(Λ)=C, and Ec=Cc.

Grade the box basis by deg⁡va=l−col⁡(a), use the total tensor grading and its induced endomorphism filtration, and use the fixed loop chart ζ ⁣:gr⁡W(λ)→U(ge) of The loop filtration on the type-A finite W-algebra has associated graded U(g^e): ζ(gr⁡rTi,j(r+1))=(−1)rei,j;r, (i,j,r)∈K. The coefficient index remains the actual unshifted T=FDE index of The shifted Yangian and the pyramid generators of the type-A finite W-algebra. The restricted character on the fixed centralizer basis is κc(ei,j;r)=δi,jδr,0σi(c),σi(c)=∑b=1picb. Consequently the full graded left representation in this fixed chart is φd,c(X)=∑t=1dX(t)+κc(X)id⁡E(X∈ge), where X(t) acts in tensor position t. In particular its complete mode-symbol dictionary is gr⁡rΦd,c(Ti,j(r+1))=(−1)r(∑t=1dei,j;r(t)+δi,jδr,0σi(c)id⁡E), where Φd,c is the restricted W(λ)-action. On the right, gr⁡1xj=e(j) and gr⁡0si is the place permutation. Thus the graded bimodule is the character-twisted Vust module Cκc∣ge⊗E, with the ordinary truncated polynomial/permutation action. It need not be the untwisted Vust module in the fixed chart. Nevertheless its unital left image algebra and its commutant are exactly the untwisted Vust image algebra and commutant, as proved below.

The displayed right operators commute with W(λ); full p-commutation is not asserted. They make Ec a filtered (W(λ),Hd(Λ))-bimodule. The actual balanced Skryabin map gives a coherent isomorphism μd ⁣:Cc⊛V⊛d→Ec of (W(λ),Hd)-bimodules. For every complex origin, every pyramid and every d, the two filtered image algebras are mutual centralizers, and their associated graded image algebras are the unital Vust image algebras. No admissibility or stable-range restriction enters this centralizer assertion.

If the pyramid is empty, N=l=0, use V=0 and W=U(ge)=C. For d=0 all structures are scalar; for d>0, E=0 and the empty cyclotomic product is 1, giving the zero quotient and zero endomorphism algebra. All formulas and centralizer identities then have these evident empty interpretations.

Facts & Assumptions

Given: The pyramid, its fixed box/row basis and K-index convention, arbitrary c, d≥0, and the left and right operators in the Definition. Assume AC for the imported equivalence and Vust theorem.

[F1]

The pyramid gives deg⁡ea,b=col⁡(b)−col⁡(a), p=⨁r≥0gr, e∈g1, and ei,j;r=∑ea,b over row pair (i,j) and column displacement r; the J↔K bijection retains the physical box labels (The type-A nilpotent pyramid, good grading and Whittaker character).

[F2]

The finite W model uses η(ea,b)=ea,b+δa,bρcol⁡(a) with ρb=n−∑h≥bqh. The canonical loop chart is the inclusion gr⁡W⊆U(p) identified with U(ge), and its mode symbols are (−1)rei,j;r, without a usi,j multiplier (The type-A finite W-algebra and the Whittaker category, The loop filtration on the type-A finite W-algebra has associated graded U(g^e), The shifted Yangian and the pyramid generators of the type-A finite W-algebra).

[F3]

For a p-module M, Skryabin supplies the actual balanced W-linear tensor map (η(u)1χ⊗m)⊗v↦um⊗v, its triangular inverse and coherent associativity. On the ambient genuine g-module the trace-form Casimir and places are natural intertwiners satisfying the affine Hecke relations; restriction to Whittaker vectors therefore transports these operators as W-endomorphisms (Skryabin's equivalence for the type-A Whittaker pair, Arakawa-Suzuki Casimir operators on tensor functors, The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations).

[F4]

The cyclotomic quotient for arbitrary complex roots has its bounded monomial basis and polynomial filtration, with graded algebra B0=C[X1,…,Xd]/(X1l,…,Xdl)⋊C[Sd]; the generator-fixing anti-involution descends (The degenerate cyclotomic Hecke algebra).

[F5]

On the untwisted tensor space E, the unital image A0=φd,0(U(ge)) and the operator image D0 of B0 are mutual centralizers for every nilpotent shape and degree, including scalar degree zero (Vust's graded double centralizer for the type-A nilpotent centralizer).

Proof

technique · direct

Given: The data and actual supplier maps of F1–F5, with AC as stated. Endomorphism algebras below use their induced finite integer filtrations; right image algebras are viewed as algebras of operators when taking commutants.

1.1F1F2constructalgebra

The column-trace function κc kills [p,p]: the diagonal column block of the commutator of two block-upper-triangular matrices is the commutator of their diagonal blocks, and its trace is zero. Therefore X↦X+κc(X)1 respects Lie brackets and extends to the unital automorphism ηc of U(p), with inverse η−c. It preserves the column grading, since only degree-zero generators receive degree-zero scalars. The coproduct gives ρdηc(X)=ρd(X)+κc(X)id⁡, exactly the action on Cc⊗E; no factor d multiplies the character. Its restriction to W is the stated filtered left action.

2.1F2F3step 1.1constructalgebra

Use the actual isomorphism μCc,V⊗d of F3, composed with coherent transported associativity, to identify Cc⊛V⊛d with Cc⊗E. The left action is the one in step 1.1, because the balanced map intertwines Δη(w) on Whittaker vectors with Δ(w) on the target. Indeed (η⊗id)Δ(w)=Δη(w) and the evaluation map obeys ψ(η(u)q)=uψ(q). The ambient universal operators Ω0j+∑k<jPkj and Pj,j+1 preserve the Whittaker subspace and commute with its W-action; transporting them through this actual map gives a right Hecke action commuting with W. Naturality transports the places to ordinary tensor permutations. This argument makes no claim about commutation with the full target p-action.

2.2F1step 1.1algebra

Each ei,j;r has degree r. If r>0 it contains no diagonal matrix units; if r=0 it contains diagonal matrix units only when i=j, and then precisely one in each column 1,…,pi. Consequently κc(ei,j;r)=δijδr0∑b=1picb. Since ge⊂p, the character of step 1.1 restricts to a Lie character on ge. Thus ηc restricts to the graded unital automorphism τc of U(ge), X↦X+κc(X)1, with inverse τ−c. No assertion that ηc preserves W is needed.

3.1F2F3step 2.1constructalgebra

To compute the transported x1, write Qc=Qχ⊗WCc and πc(η(u)1χ⊗1c)=u1c. The evaluation is balanced by F3. For a tensor basis vector vj, write its actual Whittaker preimage as z=∑izi⊗vi; then πc(zi)=δi,j. For Eab∈p, πc(Eabzi)=δab(ccol⁡(a)−ρcol⁡(a))δi,j. For Eab∈m, the actual Whittaker equation instead reads Eabzi=χ(Eab)zi−∑t:it=azi[a↦b at t]. These two identities compute every coefficient of (πc⊗1)Ω01z.

3.2F1F2step 1.1step 2.2algebra

The fixed loop chart F2 identifies the graded inclusion of W in U(p) with the ordinary inclusion of U(ge). The ordinary tensor representation ρd and ηc are graded maps. Therefore taking symbols of their restriction gives gr⁡Φd,c=φd,0τcζ. This is equality of the full graded representation, not merely equality of its image. It proves φd,c(X)=∑tX(t)+κc(X)id⁡ and the complete displayed Ti,j(r+1) symbol dictionary. The term σi(c) survives in degree zero; for positive degree it is absent. The coefficient index, sign (−1)r, finite K-range and physical box labels are unchanged.

4.1F1F2F3step 3.1algebra

In that computation the nonnegative-column terms give (ccol⁡(j1)+∑h≥col⁡(j1)qh−n)vj. The character terms from negative matrices give vL1(j), since χ(Eab)=1 exactly when b=L(a). In the remaining negative sum, replacement in the first tensor position gives −∑h>col⁡(j1)qh vj, and replacement in position k>1 gives −vj⋅(1 k) exactly when col⁡(jk)<col⁡(j1). Adding yields vjx1=vL1(j)+acol⁡(j1)vj−∑k>1:col⁡(jk)<col⁡(j1)vj⋅(1 k), precisely the matrix-unit display in the Definition. A nonexistent left neighbour contributes zero. Recursion with the place permutations gives all higher xj, and their affine relations already hold by transport in step 2.1. Thus the displayed action is the transported action, rather than an unrelated action satisfying a recursion alone.

5.1F1F4step 4.1constructalgebra

For d≥1 and l≥1, let Ck be the span of tensors whose first box has column at most k. The preceding formula preserves every Ck and gives Ck(x1−ak)⊆Ck−1. Successively applying the factors from column l down to column 1 kills Cl=E; they are polynomials in one operator and commute, so ∏b=1l(x1−ab)=0. This proves the quotient factorization directly for arbitrary complex origins, including repeated roots. In the total grading deg⁡va=l−col⁡(a), the left-shift part has degree one; the diagonal part and each two-position exchange have total degree zero. Hence gr⁡1x1=e(1). Since the longest Jordan string has length l, (e(1))k≠0 for 0≤k<l on this nonzero tensor space. A monic annihilating polynomial of degree k<l would have that nonzero degree-k symbol. Therefore the displayed degree-l polynomial is the exact minimal polynomial, consistent with F4.

6.1F4step 5.1step 3.2algebra

The right action is filtered with xj of degree one and places of degree zero: this holds for x1 by step 5.1 and for each xj+1 by xj+1=sjxjsj+sj. Taking degree-one symbols gives e(j+1)=sje(j)sj; the extra sj has degree zero. By F4 the resulting graded right map is the ordinary map Xj↦e(j), w↦Pw on B0. Together with step 3.2 this identifies the entire graded bimodule with the character-twisted Vust module in the Definition.

7.1F5step 2.2step 3.2step 6.1algebra

Since τc is an automorphism, φd,c(U(ge))=φd,0(U(ge))=A0 as unital graded subalgebras of End⁡(E). Equivalently each shifted generator differs from its untwisted operator by the explicitly known scalar multiple of the identity, and either set generates the other together with the common unit. Consequently their commutants are identical as well. By F5, A0 and the unchanged right image D0 are mutual centralizers. This proves the required Vust comparison without identifying the two fixed-chart modules.

8.1F5step 2.1step 7.1algebra

Let C=Φd,c(W) and D be the algebra of right Hecke operators, with filtrations induced from End⁡(E). They commute by step 2.1. The symbol maps in steps 3.2 and 6.1 have images A0,D0, respectively, which are contained in gr⁡C,gr⁡D. For any commuting filtered operator algebras, taking the largest homogeneous terms of a commutator gives the inclusions gr⁡C⊆gr⁡Z(D)⊆Z(gr⁡D), where Z denotes the commutant in the relevant endomorphism algebra. Therefore A0⊆gr⁡C⊆gr⁡Z(D)⊆Z(gr⁡D)⊆Z(D0)=A0. The same argument with C,D interchanged gives D0⊆gr⁡D⊆gr⁡Z(C)⊆Z(gr⁡C)⊆Z(A0)=D0. Every inclusion is equality. This also proves strict equality of the graded image algebras, rather than presuming that an arbitrary filtered representation is strict.

9.1step 8.1constructalgebra

Since C⊆Z(D) and their induced associated graded spaces agree by step 8.1, a member of Z(D) can have its leading homogeneous term matched by a member of C of the same filtration degree. Subtraction lowers the integer degree. The finite grading of E bounds the endomorphism filtration below, so iteration terminates and gives Z(D)=C. Similarly Z(C)=D. Restoring the right-action opposite convention gives Φd,c(W)=End⁡Hd(Λ)(Ec) and End⁡W(Ec)op=Ψd(Hd(Λ)). All arguments hold for arbitrary c and every d; no stable injectivity or admissible-origin Morita assertion was used.

10.1F3F4step 1.1step 9.1algebra

For d=0, Ec=Cc, φ0,c(X)=κc(X) and μ0 is the identity; the right algebra is C. Both unital operator images and commutants are scalar, even when the fixed-chart character is nonzero. For an empty pyramid the positive tensor powers are zero and both operator image algebras and both commutants in End⁡(0) are zero; degree zero is scalar. Thus the exceptional cases stated in the Definition are covered without evaluating a nonexistent x1 or invoking a positive-string Vust hypothesis.

11.1F1F2step 4.1step 3.2step 7.1step 9.1step 10.1algebra∎

In the one-box case p=(1), q1=n=1, c1=1, d=1, the fixed-chart loop generator is T11(1)=E11, and step 3.2 gives its operator 1+1=2; the untwisted Vust operator is 1. Both unital images remain C, exactly as step 7.1 proves. Separately, for gl2, p=(2), c=(0,0) and d=1, the displayed x1 is E12 and H=E11−E22∈p obeys [H,x1]=2E12≠0. This witnesses why the correct commutation claim is the transported W-commutation established in steps 2.1, 3.1 and 4.1. The full filtered bimodule, coherent μd, exact graded character chart and all-origin mutual centralizers have now all been proved.

Remarks

  • The prefix-order cross-column sum has total tensor degree zero; it does not lower the total degree by one. The individual e operator has degree one. This fixes the filtration while retaining all physical indices and the existing unshifted FDE mode convention.

  • Equality of unital image algebras is weaker than equality of fixed-chart representations. The representation here is explicitly φd,0τc; its degree-zero origin character is retained, including on Vc⊗0.

  • The origin shift ηc on U(p) and the head/tail shift η defining the Whittaker model have separate roles. The proof uses the actual balanced μd and ambient trace-form Casimir to establish the raw right operators and their W-linearity.

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

The parabolic highest-weight truncation factors through the cyclotomic quotient

Statement

Assume the Axiom of Choice The Axiom of Choice only for the imported Skryabin equivalence identifying the raw Whittaker bimodule and its affine action. The finite raw-matrix polynomial and minimal-polynomial calculations and the ordinary Pc⊗V column-flag calculation are choice-free.

Let λ=(0≤p1≤⋯≤pn) be a nonempty pyramid with columns q1≥⋯≥ql>0, let c=(c1,…,cl) be arbitrary complex origins, and put aj=cj+qj−n for 1≤j≤l. For d≥1 consider the raw tensor operator x1 on the truncated tensor space Vc⊗d of The deformed tensor space for the type-A finite W-algebra (whose underlying space is V⊗d and whose x1 is the operator displayed there). Then the minimal polynomial of x1 on Vc⊗d is exactly ∏j=1l(x−aj), including repeated roots with their multiplicities. Consequently the action of Hd on Vc⊗d factors through the cyclotomic quotient Hd(a) of The degenerate cyclotomic Hecke algebra. The same polynomial annihilates the action of the ordinary Casimir operator on Pc⊗V⊗d, where Pc is the ground induced module with its genuine column filtration.

The statement does not assert that every unrelated standard object N(A), or every parabolic category-O object, carries that same tensor action. For d=0 there is no operator x1. The integral-root weight Λ and the arbitrary-root coset bookkeeping are the separate conventions of The degenerate cyclotomic Hecke algebra.

Facts & Assumptions

Given: The nonempty pyramid, arbitrary origins c, ab=cb+qb−n, N=∑bqb, and d≥0. The direct polynomial and column-flag arguments are choice-free. Assume AC The Axiom of Choice only for the imported Skryabin equivalence establishing the raw affine action.

[F1]

Define the raw operator locally on E=V⊗d, V=CN, for d≥1 by x1=(e+∑j=1Nacol⁡(j)Ejj)(1)−∑k=2d∑col⁡(i)<col⁡(j)Eij(1)Eji(k). A superscript (k) denotes tensor position k. The box-labelled e sends vj to its left neighbour, with a missing neighbour interpreted as zero, and its longest string has length l=pn (The type-A nilpotent pyramid, good grading and Whittaker character, Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings). This local display supplies every later-position term, without using the downstream Deformed definition as a prerequisite.

[F2]

Put Qb=∑h≤bqh, Q0=0, and μb=cb+Qb−n. The ordinary ground module is Pc=U(g)⊗U(p)Cμ, where Eij1μ=δijμcol⁡(i)1μ. This is a Lie character, being a scalar trace on each column-Levi block and zero on the positive nilradical. PBW gives U(g) free as a right U(p)-module by ordering m before p; the natural module has the p-stable flag V≤b spanned by boxes in columns 1,…,b (The type-A nilpotent pyramid, good grading and Whittaker character, PBW gives an ordered monomial basis for the enveloping algebra, Universal enveloping algebra).

[F3]

Separately, Cc denotes the p-character Eij↦δijccol⁡(i). The actual balanced Skryabin tensor map identifies Wh((Qχ⊗WCc)⊗V⊗d) with Cc⊗V⊗d. Its formula is (η(u)1χ⊗1c)⊗v↦u1c⊗v, with η(Eij)=Eij+δij(n−∑h≥col⁡(i)qh). The ambient trace-form Casimir/place operators preserve Whittaker vectors and satisfy the affine Hecke relations (Skryabin's equivalence for the type-A Whittaker pair, The type-A finite W-algebra and the Whittaker category, Arakawa-Suzuki Casimir operators on tensor functors, The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations). This is a genuine Whittaker model; Pc is treated separately and is not asserted to belong to that category.

[F4]

The trace-form Casimir is Ω=∑i,jEij⊗Eji; its operator on a tensor product of genuine g-modules commutes with diagonal g. The universal first Hecke operator is Ω01, higher operators are Ω0j+∑k<jPkj, and places satisfy xj+1=sjxjsj+sj. The generator-fixing anti-involution converts these endomorphisms into a right action (Arakawa-Suzuki Casimir operators on tensor functors, The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations, The degenerate cyclotomic Hecke algebra).

[F5]

Matrix units act by Eijva=δjavi. For the total grading deg⁡va=l−col⁡(a), an individual e has degree one and a two-position exchange has total degree zero. Leading symbols multiply in the induced endomorphism filtration (Classical complex matrix Lie algebras, Associated graded algebra of a filtered algebra, Nilpotent endomorphisms and their nilpotency index).

Proof

technique · direct

Given: The locally defined raw operator and ordinary induced module of F1–F5. Assume AC only for F3's supplied equivalence and transported action; no integrality or admissibility assumption on c is used.

1.1F1F3F4constructalgebra

Establish the raw affine action without a downstream dependency. Let Qc=Qχ⊗WCc and write πc(η(u)1χ⊗1c)=u1c for the balanced evaluation of F3. For a tensor basis vector vj write its actual Whittaker preimage as z=∑izi⊗vi, so πc(zi)=δi,j. If Eab∈p, then πc(Eabzi)=δab(ccol⁡(a)+∑h≥col⁡(a)qh−n)δi,j. If Eab∈m, the Whittaker equation gives Eabzi=χ(Eab)zi−∑t:it=azi[a↦b at t]. Apply these identities to (πc⊗1)Ω01z. The nonnegative-column terms give the displayed diagonal scalar before subtraction; the negative character terms give the left neighbour of j1; replacement in the first position subtracts ∑h>col⁡(j1)qh, while replacement in any later position k contributes the negative swap precisely when col⁡(jk)<col⁡(j1). Thus the resulting operator is exactly F1. Transported places are ordinary place permutations by naturality. F3–F4 therefore give the affine relations for these raw operators, with xj+1=sjxjsj+sj, independently of the lemma's downstream consumer.

1.2F1F5constructalgebra

On a tensor basis vector the full local formula is vjx1=vL1(j)+acol⁡(j1)vj−∑k>1:col⁡(jk)<col⁡(j1)vj⋅(1 k). Let Cb be the span of tensors whose first box has column at most b, with C0=0. The left shift and every negative swap strictly lower the first column; the diagonal term preserves it. Hence every Cb is stable and Cb(x1−ab)⊆Cb−1. Starting with Cl=E, apply the factors from b=l down to b=1. Their product kills E, and the factors commute since all are polynomials in x1. Thus f(x1)=0 for f(t)=∏b=1l(t−ab), including coincident roots with all their repeated factors.

1.3F2constructalgebra

For the ordinary ground module, PBW gives an exact induction functor U(g)⊗U(p)−, since U(g) is right-free over U(p). The tensor identity is the g-linear map θ:U(g)⊗U(p)(Cμ⊗V)→Pc⊗V, u⊗(1μ⊗v)↦∑u(1)(1⊗1μ)⊗u(2)v, where Δ(Eab)=Eab⊗1+1⊗Eab. The matrix-unit relations show that Δ extends multiplicatively to U(g), and its formula gives the required balancing over U(p). On the PBW basis of U(m), θ has leading term u(1⊗1μ)⊗v; all other terms have smaller PBW degree in the first factor. Finite descending subtraction proves it is bijective. Exact induction and θ carry the flag Cμ⊗V≤b to a genuine g-submodule flag 0=F0⊂F1⊂⋯⊂Fl=Pc⊗V. This is the column flag of the tensor product, not a finite flag of Pc itself.

2.1F1F5step 1.2algebra

Give E the total tensor grading of F5. The left shift raises this degree by one. The diagonal terms have degree zero, and Eij(1)Eji(k) has degree (col⁡(j)−col⁡(i))+(col⁡(i)−col⁡(j))=0, regardless of the column gap. Therefore gr⁡1x1=e(1). For a nonzero polynomial g of degree r<l with leading coefficient γ, the degree-r symbol of g(x1) is γ(e(1))r≠0: a top vector in a longest row has a nonzero rth left shift, and the remaining tensor positions can be any nonzero basis vectors. This includes r=0, whose symbol is a nonzero scalar identity. Consequently no polynomial of degree less than l annihilates E. Together with step 1.2, this proves that f is the exact minimal polynomial, even when roots coincide.

2.2F2F4F5step 1.3algebra

Put m0=1⊗1μ∈Pc and choose a box j in column b. By the matrix-unit action, Ω(m0⊗vj)=∑kEjkm0⊗vk. For col⁡(k)≥b, Ejk∈p, so only k=j survives and contributes μbm0⊗vj. For each earlier-column box k, the primitive coproduct formula in step 1.3 gives Ejkm0⊗vk=θ(Ejk⊗(1μ⊗vk))−m0⊗Ejkvk. The first term belongs to Fb−1 and the second is −m0⊗vj. There are exactly Qb−1 such boxes. Hence Ω(m0⊗vj)≡(μb−Qb−1)m0⊗vj=abm0⊗vj(modFb−1). Since Ω is g-linear and Fb is generated by these ground tensors in columns at most b, this also proves that it preserves the full flag and acts by ab on Fb/Fb−1.

3.1F4step 1.1step 1.2step 2.1algebra

The raw affine action in step 1.1 kills f(x1) by step 1.2, so its right representation kills the two-sided ideal generated by this polynomial and descends to Hd(a). The generator-fixing anti-involution fixes f(x1), so the quotient statement respects the right-action convention. The preceding proof uses only the raw first-column flag and total grading, not a purported Skryabin image of an ordinary category-O object.

3.2F4step 1.3step 2.2algebra

Apply Ω−al,…,Ω−a1 successively to the flag of step 2.2. Each factor moves the relevant flag piece down one column, so their product annihilates Pc⊗V. The factors commute and their order is immaterial. On Pc⊗V⊗d the first ordinary Hecke/Casimir operator is Ω01 tensored with the identity on the remaining d−1 natural factors. Tensoring the annihilating operator identity therefore gives f(Ω01)=0 on this entire module. No irreducibility, integral-origin identification or ordinary-to-Whittaker transfer was used.

4.1F4step 3.1step 3.2algebra∎

The raw minimal-polynomial statement and quotient factorization follow from steps 1.1, 1.2, 2.1 and 3.1, and the ordinary induced-module annihilation follows separately from steps 1.3, 2.2 and 3.2, for arbitrary complex c and every nonempty pyramid. For d=0 there are no xj, so there is no x1 or minimal polynomial to assert; the Hecke algebra is C. The integral-root weight and arbitrary-complex coset conventions remain those of the cyclotomic definition and play no role in either local calculation.

Remarks

  • Repeated roots are retained because the first-column flags use one polynomial factor per column; exact minimal degree uses the largest Jordan string and does not require separability.

  • The raw proof and the ordinary ground-module proof are separate. The raw action comes from the genuine module Qχ⊗WCc via the actual balanced Skryabin map, whereas the ordinary ground module is induced from Cμ with μb=cb+∑h≤bqh−n.

  • The Statement's link to the Deformed definition identifies the actual raw operator context, recorded as a direct dependency. The polynomial and ordinary column-flag arguments remain locally supplied; the Deformed definition independently proves its own raw polynomial and does not depend on this lemma.

LemmaStatement: Literature-sourcedProof: AI-adaptedOpen item page →

Separated integral cosets give typed parabolic category equivalences

Statement

Assume AC. Work in genuine type-A parabolic category O for glN(C) with its fixed Borel. Its column Levi has ordered blocks of heights q1≥⋯≥ql. All entries in column j lie in cj+Z, where the original admissibility condition is cj−ck∈Z⇒cj=ck. Use the source highest-weight convention ηi=ai+i−1 and half-sum ρi=(N+1−2i)/2, with the column reading prescribed by the source Borel. For each occurring entry coset κ retain its columns in their original order. Fix an order on the finite set of cosets; no order on C is used.

Subject to the local HC tensor-projective comparison stated in [F1], stable sorting of the coordinates by κ gives an exact, complex-linear equivalence of the genuine parabolic categories, carrying each ordinary Verma label by the dot permutation and carrying the corresponding generalized standard, simple head and projective cover. On each linkage block, the sorted category is equivalent to the product of the corresponding parabolic blocks for glNκ, where Nκ=∑j∈κqj. Product means the abelian category generated by finite presentations of outer tensor products, equivalently modules over the tensor product of the finite block endomorphism algebras.

For the original pyramid with n rows put nκ=max⁡j∈κqj. The component integral entry dictionary is exactly aiint=ai−cκ+n−nκ,mj=qj−nκ,inf⁡Iκ=1−nκ. Thus mj+1−inf⁡Iκ=qj, with the original nonincreasing retained heights and charges. For the admitted-ground subcategories, where each original entry has a nonnegative integral difference from its own ground entry, this dictionary lands in the bounded-below admitted integral component models of [F4]. For other genuine parabolic blocks it records the integral weight/coset dictionary and the trace shift, without asserting membership in that fixed admitted cut. If the component follows Bκ sorted coordinates, its Levi highest weight and the integral highest weight differ by the scalar trace-character shift δκ=Bκ+cκ−n+nκ. This shift is a Lie algebra character and requires no integrality of cκ. Singular repeated-entry linkage blocks are included. The original complex origins, component entry multisets and their scalar centres remain recorded; different complex cosets are not merged into one integral block.

Sorting commutes coherently with finite tensoring and its invariant Casimir and permutation maps. The separated product decomposition is blockwise and does not assert that unrestricted tensoring is componentwise. The proof gives its actual filtration and block-projection comparison. Choices of sorting word with the same stable permutation yield the natural comparison fixed on the chosen reference highest vector and its tensor-projective presentations.

Facts & Assumptions

Given: The original admissible origins and nonincreasing column heights, the source Borel and highest-weight convention, and AC. No realness, mutual comparability, regularity of the subject block, or integrality across different cosets is assumed.

[F1]

The local tensor-projective comparison The regular coset-dominant Harish–Chandra tensor comparison: for a regular weight λ decreasing within each integral shifted-coordinate coset, finite integral-coordinate tensors E⊗Δλ and their direct summands give projective generators of Oλ+ZN; for finite E,F their Hom spaces are naturally (E∗⊗F⊗Uχλ)g, with evaluation and composition. Its same all-weight Duflo input is required for s⋅λ after a distinct-coset adjacent swap. The all-weight action isomorphism is supplied through that local HC lemma; the present proof uses its Hom comparison at both regular reference weights and does not reprove the Duflo theorem.

[F2]

Finite length, projective covers and PBW: Every object of O has finite length, Category O has enough projectives, PBW gives an ordered monomial basis for the enveloping algebra. The scalar centre of glN splits off from the semisimple theory.

[F3]

Actual linkage, not a central-character identification: Central-character summands refine into linkage blocks, The strong linkage principle for Verma modules, Integral reflection linkage is an equivalence relation. In type A, the integral roots are exactly differences of shifted coordinates in the same C/Z coset; their group permutes those coordinates.

[F4]

Genuine parabolic modules and the admitted integral component convention: Parabolic category O for a standard parabolic, The integral parabolic category-O blocks for higher-level Schur-Weyl duality, Finite-dimensional simple modules are classified by dominant highest weights. Only the Levi-integrable simple criterion, Serre property, largest generalized-Verma quotient and the explicit integral charge/height convention are consumed. The proof below constructs the nonintegral product rather than importing integral highest-weight conclusions for arbitrary complex labels.

[F5]

AC The Axiom of Choice, with the exact inherited/projective use recorded above.

Proof

technique · direct

Given: Use the data of the Statement and [F1]–[F5]. Normalize Chevalley matrices by E=Ei,i+1, F=Ei+1,i and H=[E,F]. Twist by ϕ=exp⁡(ad⁡E)exp⁡(ad⁡(−F))exp⁡(ad⁡E) with twisted action x⋅v=ϕ(x)v.

1.1givenalgebra

Every H-weight in the relevant weight-coset category is nonintegral when the adjacent shifted coordinates belong to different entry cosets: η(H)=(η+ρ)i−(η+ρ)i+1−1, and weight changes are integral. This holds in every subquotient. If Fv=0 for a weight vector of weight h, choose r≥0 maximal with Erv≠0, using positive-root local nilpotence in O. The sl2 relation gives FEr+1v=−(r+1)(h+r)Erv, a contradiction. Thus F is injective on every object and subquotient of that category.

2.1F2step 1.1constructalgebra

Powers of F satisfy both Ore conditions in U(g): iterating Fu=uF+[F,u] gives the finite binomial commutation formula, since ad⁡F is locally nilpotent on each enveloping element. PBW makes U a domain. Its localization UF=⋃k≥0F−kU is a directed union of free right U-modules; consequently localization MF=UF⊗UM is exact. Step 1.1 makes M→MF injective, and the diagram of short exact sequences 0→M→MF→MF/M→0 proves exactness of CF(M)=MF/M. Therefore Ts(M)=ϕCF(M) is exact. The adjoint exponentials defining ϕ are finite on every u∈U; they send E,F,H to −F,−E,−H and act as the adjacent permutation on the Cartan.

3.1F2step 2.1constructalgebra

Let v be the normalized highest vector of Δη. The class F−1v becomes a highest vector of weight s⋅η: its new E is −F, whose value lies in Δη; the other transformed positive roots are positive roots distinct from αi, and commuting them through F−1 leaves positive-root terms killing v. The new F sends F−rv to r(η(H)+r+1)F−r−1v, with every scalar nonzero. PBW, ordered with F first, gives the basis of the localized quotient with F-powers −1,−2,…; reflection permutes the remaining positive roots. Hence the displayed vector generates the quotient. Its character is s(eη∑r≥1erαi∏β>0,β≠αi(1−e−β)−1)=ch⁡Δs⋅η. The highest-vector surjection is an isomorphism by equality of each finite weight dimension. This fixes its scalar by vs⋅η↦[F−1vη].

4.1step 2.1constructalgebrastep 3.1

For finite-dimensional X, localization commutes with tensoring. On MF⊗X the total operator FM+FX has inverse FM−1∑k≥0(−FM−1FX)k; the sum is finite since FX is nilpotent. The localization universal property identifies (M⊗X)F with MF⊗X and identifies the embedded M⊗X. Quotienting and the Weyl matrix WX=exp⁡(EX)exp⁡(−FX)exp⁡(EX) identify Ts(M⊗X) naturally with Ts(M)⊗X. For two finite tensor factors, WX⊗Y=WX⊗WY, so associativity and the tensor-unit diagrams commute. The diagonal Weyl action fixes the invariant Casimir and commutes with flips, proving their compatibility as actual operators.

5.1F1step 3.1step 4.1algebra

Choose regular coset-dominant λ in the weight-coset category. Crossing distinct cosets preserves each coset's internal order, so s⋅λ meets the same regular coset-dominance hypotheses; its central character equals χλ. For a generator map encoded by t∈(E∗⊗F⊗Uχ)g, its action is the finite sum of finite-tensor matrix entries followed by enveloping operators on Δλ. The invariant matrix map commutes with the total F on the tensor modules, so its unique localized extension agrees with the same enveloping-operator formula under the tensor localization of step 4.1. Passing to the quotient, twisting and applying the matrices of step 4.1 transforms t by simultaneous Weyl conjugation in its three factors. Each t lies in a finite adjoint submodule, so that conjugation is exp⁡(Ediag)exp⁡(−Fdiag)exp⁡(Ediag) and fixes t, since its diagonal g-action is zero. Thus Ts induces exactly the common Hom identification of [F1], respecting composition and identity. The scalar from step 3.1 is the same on all generators X⊗Δλ, so it cancels on every generator Hom space; an arbitrary unnormalized scalar is not treated as a literal equality of highest vectors.

6.1F1F2F5step 2.1step 5.1constructalgebra

Every object has a finite presentation by finite direct sums and summands of the generators in [F1]. Exactness and steps 3.1–4.1 show that its Ts image is the cokernel of a map between target generators, hence belongs to the target category O. Step 5.1 identifies all generator maps. Every target presentation therefore lifts, proving essential surjectivity. Applying Hom from a generator to a source presentation and its target presentation gives identical cokernel diagrams, since those generators are projective; applying Hom from a presented object gives identical kernel diagrams. This proves full faithfulness on all objects. Idempotents are preserved and reflected by the generator Hom identification, so summands cause no gap. Consequently Ts is an exact category equivalence, established on actual maps and presentations.

7.1F4step 3.1step 6.1constructalgebra

Compose these swaps in a stable bubble sort by the fixed coset order. Each swap crosses different cosets; none permutes indices inside a coset. The composite sends Δη to Δw⋅η and therefore sends its unique simple head to L(w⋅η). It transports projective covers by exact equivalence and essentiality. Every original column consists entirely of one coset; stable sorting retains its coordinates as a consecutive block and retains their internal order. At the end, the original Levi simple roots are therefore positive simple roots of the sorted column Levi. Their highest-weight integral-dominance pairings are unchanged. By the actual Levi simple criterion and Serre property of [F4], the composite and its inverse restrict to the full parabolic subcategories. Because generalized Vermas are the largest parabolic-finite quotients of ordinary Vermas, their quotient universal property is transported, giving the claimed generalized-standard labels as modules. No intermediate swap is asserted to preserve an intermediate parabolic subcategory.

8.1F1step 4.1step 5.1step 6.1constructalgebrastep 7.1

The coherent comparison of two sorting paths can be made on tensor-projective generators. Each path has the common [F1] Hom matrix identification of step 5.1; their final Weyl representatives differ at most by a diagonal torus matrix when they induce the same coordinate permutation. Diagonal simultaneous action again fixes invariant matrices. Their reference-standard highest lines admit a unique comparison after fixing its nonzero scalar; tensor it with X for every generator and summand. The equality on generator Hom matrices makes these comparisons natural, and taking presentation cokernels extends them uniquely to all objects, independently of a presentation by full faithfulness. Comparisons for three paths compose because they coincide on the normalized reference generator and its tensor presentations. This proves the stated normalization and coherence, without asserting an unnormalized inverse-twist or braid identity.

9.1F2F3constructalgebrastep 8.1

After sorting let q have contiguous coset Levi l=⨁κglNκ and positive outside radical u. In a fixed linkage block C, [F3] says exactly that highest labels are obtained by permutations within the coset blocks, including when entries repeat. Hence all highest labels have the same block-centre values zκ. For each initial union of coset blocks, write Zr for its diagonal trace and br for the common highest-label value. Every module weight satisfies br−μ(Zr)∈Z≥0: this holds on simple highest-weight modules by their negative-root weights and on all finite-length objects by their composition series. An outside negative root strictly lowers at least one prefix; an inside root leaves every prefix fixed. The simultaneous top section S(M)={v:Zrv=brv ∀r} is therefore a Levi module and is annihilated by u. It is exact, since it is a direct sum of Cartan weight spaces and the Cartan acts semisimply. These are integer differences from fixed complex values, not inequalities on complex numbers.

10.1F2F3step 9.1algebra

In fact Mu=S(M). If a nonzero homogeneous radical-invariant vector lies in a lower prefix section, its Levi cyclic module has a highest vector: its positive Levi orbit is finite-dimensional and a maximal weight therein is killed by every positive Levi root. Radical invariants are Levi-stable because [l,u]⊂u. That Levi highest vector is thus a full g highest vector. Its cyclic module has a simple highest-weight quotient of the same weight and the same strictly lower prefix, contradicting the actual label restriction in [F3]. Decomposing a general invariant into centre weights gives the same contradiction componentwise. Moreover S detects nonzero objects: every simple of C has a nonzero highest vector in its top section, and exactness plus a composition series proves the assertion for every nonzero finite-length object.

11.1F2F3step 9.1step 10.1constructalgebra

Let Cl be the product integral-reflection orbit for the Levi highest weights with these fixed scalar centres, and define R(X)=U(g)⊗U(q)X, with u acting by zero. PBW makes R exact and identifies S(R(X))=X naturally: every outside negative PBW monomial lowers some prefix, so only its degree-zero term contributes. For a Levi simple Ll(η), induction is a quotient of the ordinary g Verma of label η, hence lies in C by [F3] and has finite length by [F2]. Every composition factor has nonzero top section by step 10.1; exactness and S(R(Ll(η)))=Ll(η) imply that there is only one factor. Thus R(Ll(η))=Lg(η) is simple. Exactness extends block membership and finite length to R(X) for every finite-length X by a Levi composition series.

12.1F4step 10.1step 11.1constructalgebra

Induction and radical invariants are adjoint, and step 10.1 identifies the latter with S. Their unit is PBW's top-section isomorphism X→S(R(X)). For the counit R(S(M))→M, applying exact S gives this identity, so its kernel and cokernel have zero top section; both are finite-length objects of C and vanish by detection in step 10.1. Hence R and S are inverse exact category equivalences. This argument proves full faithfulness from the actual unit and counit. It does not deduce it from composition matrices. By induction transitivity, ordinary Levi Vermas go to ordinary g Vermas; the corresponding column-generalized Vermas go to their genuine column-parabolic inductions. The Levi integrability criterion restricts the equivalence to the column-parabolic subcategories just as in step 7.1; projective covers again follow by exact equivalence.

13.1F2F4step 12.1constructalgebra

Each finite Levi factor block has a finite projective generator (finite label orbit and [F2], or its parabolic reflector). For two outer tensor projectives, their Hom is the tensor product of their factor Homs, by tensor-Hom and the finite-dimensional factor Hom spaces; applying a factor-projective Hom successively is exact: a fixed weight for the other factors cuts a finite-generated factor-O module, since PBW bounds the negative monomials in those fixed coordinates; factor projectivity therefore applies weight by weight. The resulting multiplicity module is in the remaining factor O, by the same PBW finiteness with the finitely many generator weights of the projective. Their outer tensor sum therefore is projective, and its simple quotients cover all factor tuples. Those tuples exhaust the simple labels of the direct-sum Lie algebra: the outer tensor of the factor simples is cyclic on the tensor of their highest vectors. Any nonzero submodule has a highest vector by positive-root local finiteness and bounded highest-weight support; taking invariants successively in the separate positive root algebras leaves only that tensor highest line, because a simple highest-weight factor has no other highest vector. The submodule thus contains the cyclic generator, proving simplicity and identifying the unique simple quotient of the direct-sum Verma. Thus the outer tensor generator gives finite presentations of every object and has the tensor-product endomorphism algebra. Applying the generator Hom and its presentation inverse proves the product description in the Statement. This also proves standard/simple/projective tensor labels as objects, not just as classes.

14.1F4step 7.1step 13.1constructalgebra

The original tableau convention gives ηi+ρi=ai+(N−1)/2, so dot sorting is literally stable sorting of the ai. In the sorted κ block the Levi coordinate is at+Bκ+t−1. The integral coordinate from the Statement is at−cκ+n−nκ+t−1; their difference is exactly δκ. Tensoring with the one-dimensional Lie algebra representation x↦δκtr⁡(x) is an exact inverse equivalence with inverse shift −δκ, and its tensor associativity is ordinary scalar multiplication. It carries highest vectors, induced standards, simple heads and projective covers. Since a ground entry in global row r is cκ+1−r, its integral image is 1−(r−n+nκ); these are the actual bottom-aligned integral ground rows. The retained heights give mj=qj−nκ nonincreasing and mj+1−(1−nκ)=qj. For an admitted-ground label, subtracting its original ground entry gives a nonnegative integer; the displayed dictionary preserves that difference. Its integral entry is therefore at least the corresponding bottom-aligned integral ground entry and lies in the fixed admitted alphabet of [F4]. For an arbitrary genuine label the scalar shift still gives an integral parabolic highest weight, but no fixed-cut membership follows. Thus the height/charge dictionary holds generally and the fixed admitted component hypotheses of [F4] hold on the stated admitted-ground subcategories, without treating a nonintegral scalar trace character as an algebraic determinant character.

15.1F3step 11.1step 12.1constructalgebrastep 14.1

For clarity about tensor transport, the ordinary induction tensor identity is R(X)⊗V≅U(g)⊗U(q)(X⊗Res⁡qV); it follows from the coproduct and antipode and is natural in X,V. The restricted vector representation has its actual prefix-q filtration whose sections are the coset vector modules Vκ with outside radical zero. Exact induction therefore gives a filtration of R(X)⊗V with sections R(X⊗Vκ). A projected linkage/entry-multiset tensor summand admitting an entry change in coset κ kills the other sections: their highest labels change a different coset multiset, so their central characters or linkage classes differ by [F3]. Only the κ section survives, giving its natural component comparison; the dual vector representation has the reversed filtration and the same argument. Thus the residue-projected operators transport to the appropriate integral factor. Iterated tensor comparisons use the same actual filtrations and the associative tensor identity, so their diagrams commute; no unrestricted tensor-product assertion is inferred.

16.1step 4.1step 7.1step 12.1step 13.1step 14.1step 15.1algebra∎

The trace-character shift changes the relevant vector Casimir eigenvalue by its scalar: for Ω=∑i,jEij⊗Eji, replacing the first-factor action by Eij+δijδ adds δ∑i1⊗Eii=δ on a vector representation; the dual gives the corresponding opposite shift. The offset can be computed explicitly: on a vector-tensor Verma section of highest label η+εi, the quadratic central element has value ∑kηk(ηk+N+1−2k), while its value on the vector is N. Taking half the difference gives the global tensor-Casimir eigenvalue ηi+1−i. For the Levi coordinate t=i−Bκ, the same calculation gives ηi+1−t, greater by Bκ. Hence the trace shift contributes δκ−Bκ=cκ−n+nκ to the original residue: (cκ+qj−n)−(qj−nκ)=cκ−n+nκ. This computes the parameter dictionary and the block projections of step 15.1; no integer residue is silently equated with its complex original. It does not replace a proof of the full affine-Hecke natural-transformation presentation. Together with steps 4.1 and 15.1 this proves the claimed normalized compatibility, and steps 7.1, 12.1–13.1 and 14.1 prove the typed category equivalence with all stated labels and hypotheses.

Adoption boundary

The sixteen-step proof supplies the local category equivalence using the proved local HC comparison in [F1] and the stated category-O suppliers. The fixed bounded-below integral component model is invoked only for the admitted-ground subcategories; the genuine full category equivalence and trace-character dictionary retain their full scope. This draft does not supply the Fock canonical-basis identification, the affine-Hecke presentation, or Whittaker simple-image assertions.

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

The Whittaker functor from the relevant parabolic category-O summand

Definition

Work over C and assume the Axiom of Choice where projective covers, duality and locally unital assemblies enter. Let λ=(0≤p1≤⋯≤pn) be a pyramid with columns q1≥⋯≥ql, let c=(c1,…,cl) be admissible in the sense that ci−cj∈Z implies ci=cj, and let Ocd be the relevant summand of the genuine parabolic category O attached to the labels c and the degree d: its objects are the modules whose column-strict labels have nonnegative integral differences from the ground entries of each column, i.e. the labels with Λ-diagram content cj+qj−n in the sense of The degenerate cyclotomic Hecke algebra (the ambient categories are the ones of The integral parabolic category-O blocks for higher-level Schur-Weyl duality and Parabolic category O for a standard parabolic).

For a U(m)-finitely-generated object N of genuine parabolic O, the Whittaker functor is the covariant finite-dimensional dual V(N):=Hom⁡m(N,Cχ)∗. Its W(λ) action is obtained from the continuous χ-part of the right linear dual, then the reflected head/tail identification proved below. In the notation DrowWhDrow, the middle Whittaker operation is performed on this continuous χ-part, not on the uncompleted ordinary row-restricted dual. Write N(A) for source standard objects, LO(A) for source simples, and LW(A) for the resulting nonzero simple W-modules. These namespaces are distinct.

The verification below records the properties used on this page: V is exact on the U(m)-finitely-generated objects of genuine parabolic O and intertwines tensoring with finite-dimensional Cartan-semisimple g-modules, the Casimir and the flips; V is distinct from the Hecke quotient Hom⁡g(T,−) constructed later; for the ground simple projective-injective Pc and T=Pc⊗V⊗d one has V(Pc)=Cc and V(T)=Vc⊗d; and V(LO(A)) is the simple W-module LW(A) for standard labels A and zero otherwise. Nonintegral origins use the typed equivalence of the all-weight Harish-Chandra comparison of the source; no arbitrary complex c is identified with an integral block. After fixing the ground identification i0 ⁣:V(Pc)→Cc, the compatible functor and the maps jd are unique up to the normalized unique natural isomorphism; without this normalization scalar automorphisms prevent literal uniqueness.

Facts & Assumptions

Given: The pyramid λ, admissible origins c, the categories Ocd and the Whittaker data; assume AC The Axiom of Choice for the stated imported constructions and Baer/vector-space splittings.

[F1]

The parabolic and genuine-category-O interfaces: Pc is the ground simple projective-injective, the standard objects N(A) and simple objects LO(A) are labelled by column-strict tableaux, and the category is a highest-weight category with enough projectives (The integral parabolic category-O blocks for higher-level Schur-Weyl duality, Parabolic category O for a standard parabolic, Parabolic category O is a highest weight category, Category O has enough projectives).

[F2]

The finite W-algebra, its Whittaker category and Skryabin's equivalence, including the filtration Qχ⊗W(λ)− and the tensor identification M⊛X=Wh((Qχ⊗W(λ)M)⊗X) on restricted p-modules (The type-A finite W-algebra and the Whittaker category, Skryabin's equivalence for the type-A Whittaker pair, The deformed tensor space for the type-A finite W-algebra).

[F3]

The truncated tensor space Vc⊗d is a filtered (W(λ),Hd(Λ))-bimodule with the explicit generators, and the tensor compatibility preserves the generators xj,si (The deformed tensor space for the type-A finite W-algebra).

[F5]

Noetherianity, Baer injectivity, complete reducibility and Hilbert basis inputs used to make the functorial constructions finite and exact (Hilbert basis theorem: if R is Noetherian then R[x] is Noetherian, Baer's criterion for injective modules, Weyl's complete reducibility theorem, Standard parabolic and Levi subalgebras from a subset of simple roots).

[F6]

The SAME original finite-W algebra has both its tail/left and head/right normalizer descriptions for every initial-column prefix, with ηhead(Ejj)=Ejj+n−∑k≤col⁡(j)qk; the proved original prefix T recursion retains the actual coefficient index and its last-column Levi sum and positive-matrix commutator (The type-A finite W-algebra and the Whittaker category, The shifted Yangian and the pyramid generators of the type-A finite W-algebra, Ordered monomial PBW basis for the shifted Yangian). Ordinary PBW identifies parabolic induction with U(m)⊗D, and finite-dimensional dominant-weight classification supplies the tensor-summand realization used below (PBW gives an ordered monomial basis for the enveloping algebra, Finite-dimensional simple modules are classified by dominant highest weights). These original-model interfaces hold for every initial-column prefix and retain the original column chart.

[F7]

The normalized highest-component projection is an actual module map with saturated integral kernel spanned exactly by off-standard source dual-canonical LA and independent image basis DA; the original-order source upper ground component is exactly Std (Standard tableau monomials form a basis of the highest weight Fock submodule). The standard/simple matrix is the genuine parabolic composition matrix and gives the simple-class dictionary by inversion (Parabolic Kazhdan-Lusztig polynomials give the dual-canonical transition matrix, The parabolic category-O Grothendieck group is the integral Fock module). Exact biadjoint residue functors have the valid-entry standard flags, the corresponding Chevalley action, and the actual simple-head/socle theorem (The residue translation functors give the integrable Fock-space action, The local affine-Hecke socle argument for residue translations). Highest-weight projective kernels have higher-labelled standard flags and restricted transposition duality fixes simples (Parabolic category O is a highest weight category). Central characters are dot-Weyl orbits, hence are entry multisets in the source shifted-highest-weight convention (Central characters are dot-Weyl orbits). All these inherited AC assumptions and the typed coset dictionary of F4 are retained.

[F8]

In the actual tensor box grading, the original loop/PBW symbols identify gr⁡W with U(ge); the graded left representation is x↦∑tx(t)+κc(x)id⁡, with its actual degree-zero origin character, while the graded right generators are e(j) and the place permutations (The loop filtration on the type-A finite W-algebra has associated graded U(g^e), Ordered monomial PBW basis for the shifted Yangian, The deformed tensor space for the type-A finite W-algebra, The degenerate cyclotomic Hecke algebra). The unital untwisted images of U(ge) and the truncated polynomial/permutation algebra are mutual centralizers in every degree, including scalar and empty cases (Vust's graded double centralizer for the type-A nilpotent centralizer). This raw filtered input does not use the later finite-W/Hecke theorem's Morita clause.

Proof

technique · direct

Given: Assume AC. Use U=U(m) and I=Iχ. The source standards are N(A), source simples LO(A) (abbreviated LO(A) in the computations), and output simples LW(A). The finite tensor/Hopf comparisons use the actual Skryabin displayed map, not cofree constant evaluation.

1.1F1F2F5constructalgebra

Let U=U(m), I=I_chi. Replace x by y=x−chi(x). These shifted generators have the original brackets, because chi vanishes on brackets. Choose a basis adapted to the lower-central filtration, with weight w_i the largest lower-central index containing its basis vector. PBW reordering and the commutator formula show that I^n is spanned by ordered monomials of total lower-central weight≥n: one inclusion follows from reordering n factors, while the reverse follows because each basis vector of weight w lies in I^w, being a linear combination of iterated brackets of length w.

1.2F1F2F5constructalgebra

The Rees algebra R=⊕_(n≥0) I^n t^n is generated by y_i t^r, 0≤r≤w_i. Their span is a finite-dimensional Lie algebra: a nonzero bracket component y_k has w_k≥w_i+w_j, so r+s≤w_k. PBW gives its enveloping algebra a polynomial associated graded. For any left ideal, Hilbert basis gives finitely many generators of its homogeneous leading ideal; lift them and subtract matching highest-degree terms until the nonnegative degree decreases to zero. The lifts generate the original ideal. Thus the enveloping algebra is left noetherian, and its surjection onto R makes R left noetherian. For a left ideal J⊂U, ⊕(J∩I^n)t^n is a graded left ideal of R and has finitely many homogeneous generators. For fixed k, choosing n greater than k plus their largest degrees gives J∩I^n⊂I^k J. This is the precise Artin–Rees consequence needed here.

1.3F1F2F5constructalgebra

Set E_chi=∪_(n≥0)(U/I^n)^*, with left action (x f)(r)=f(r x). To prove injectivity, take a U-linear map phi:J→E_chi. U is noetherian, so choose finitely many generators of J. A common I^k kills their images and hence all images, since I is two-sided. The scalar functional lambda(j)=phi(j)(1) kills I^k J. Choose n with J∩I^n⊂I^k J, extend lambda from J/(J∩I^n) to U/I^n, and call the extension a∈E_chi. The map U→E_chi, u↦u a, extends phi, because at r its value on j is a(rj)=phi(rj)(1)=phi(j)(r). Baer's criterion gives injectivity. This supplies the injective-continuous-dual assertion cited without proof in BK Lemma8.20.

1.4F1F2F5constructalgebra

For a U(m)-finitely generated g-module X, evaluation at1 identifies Hom_m(X,E_chi) with the scalar functionals lambda:X→C that kill I^n X for some n. Indeed, reconstruct the map by F_lambda(v)(r)=lambda(rv); finitely many generators give a common n. The right U(g)-action is (lambda·u)(v)=lambda(uv). On E-valued maps its formula is therefore

1.5F1F2F5constructalgebra

(F·u)(v)(r)=lambda(u r v),

1.6F1F2F5constructalgebra

not the generally non-m-linear expression F(uv)(r)=lambda(r u v). This distinguishes the compressed scalar-functional notation in the source from a literal E-valued composition.

1.7F1F2F5constructalgebra

The right action preserves continuity. For a fixed u∈U(g), the finite PBW subspace generated by all iterated ad m on u is finite-dimensional and its negative-column action is nilpotent; sufficiently long products of ad m vanish. Moving u past a product of sufficiently many shifted m generators therefore leaves at least n of them on the left. Equivalently u I^(n+C)⊂I^n U(g) for some C=C(u). Thus lambda u kills I^(n+C)X. On this continuous-dual module the right shifted m-action is locally nilpotent. Injectivity of E_chi makes Hom_m(−,E_chi) exact, and right Skryabin makes its Whittaker vectors exact. These Whittaker vectors are precisely Hom_m(X,C_chi). Dualizing this finite-dimensional vector space gives an exact covariant functor.

1.8F1F2F5constructalgebra

The restricted dual uses the row-sum torus a=span{Σ_(row(j)=r)E_jj}, not the full Cartan and not the column-origin vector c. Every e-adjacent pair lies in one row, so chi has a-weight0. If X is generated over U(m) by finitely many a-weight spaces, an m-linear functional into C_chi vanishes outside those finitely many weights: lambda(uv)=chi(u)lambda(v), and chi(u)=0 in every nonzero a-weight. Thus the restricted-dual definition agrees with the entire finite-dimensional Hom space. Generalized parabolic Vermas are U(m)-free on a finite-dimensional Levi module by PBW; their finite projective flags/presentations from the repaired parabolic highest-weight supplier make every genuine parabolic O object finitely generated over U(m). This establishes exactness on precisely that category.

1.9F2F3F6constructalgebra

For the natural box module define Xij=(−1)a−bIa−1(Trow⁡(j),row⁡(i)(a−b)) when a=col⁡(i)>b=col⁡(j), and Xij=δij otherwise. These are the actual prefix coefficients, not reindexed series. They give a unitriangular matrix. For x=Ers with col⁡(r)=col⁡(s)+1=A, establish both [x,ηtailXij]+δirηtailXsj∈U(g)I and [x,ηheadXij]+δirηheadXsj∈IU(g). If a<A, disjoint supports give zero. If a>A, the original left/right normalizer theorems for prefix a−1 give both containments; a whole-pyramid shift differs from the corresponding prefix shift only by a uniform trace character, which fixes m, χ and both ideals. For a=A, expand the actual prefix last-column recursion [F6]. Its embedded prefix-a−2 terms and its final commutator with the positive previous-to-last matrix commute with Ers. Only the column-Levi sum ∑hI(Tu,h(d−1))Ebox⁡(h,a−1),box⁡(v,a−1) contributes. Its bracket is δs,box⁡(h,a−1)η(ITu,h(d−1))Er,box⁡(v,a−1). The negative bridge commutes with the prefix-a−2 coefficient, so its left and right reductions both give δirη(ITu,row⁡(s)(d−1)). The two consecutive displacement signs differ by minus one, giving precisely −δirηXsj. Diagonal shifts add commuting scalars, so this boundary calculation works for both head and tail.

1.10F1F2F3F4F5constructalgebra

Finite-Levi Weyl gives, on row variables z_(n−q+1),…,z_n,

1.11F1F2F3F4F5constructalgebra

ch L(nu)=det(z_r^(nu_s+q−s))/det(z_r^(q−s)) =(Π_(r=n−q+1)^n z_r^(n−1)) det(z_r^(a_s))/det(z_r^(q−s)).

1.12F1F2F3F4F5constructalgebra

The numerator exponent is exactly a_s+n−1; the column height and reading offset cancel. The prefactor and denominator are independent of the entries. Products over columns therefore identify the row-torus character of V(N(A)) with a fixed factor times products of nested bottom-row flag minors, evaluated at y_(r,a)=z_r^a. For the ground column a_s=c+1−(n−q+s), the determinant cancels the Vandermonde and gives precisely Π z_r^c, verifying the origin normalization.

1.13F1F2F3F4F5constructalgebra

All exponential expressions lie in the group algebra of the finitely generated additive subgroup generated by their occurring complex weights and the integral row weights. That subgroup is finitely generated and torsion free, hence free abelian; its group algebra is a Laurent polynomial domain. The nonzero Vandermonde may therefore be cancelled. A zero character of an actual nonzero finite-dimensional module is impossible: its coefficients are nonnegative weight dimensions, and evaluation of the group algebra at1 is its positive dimension.

1.14F1F2F3F4F5constructalgebra

Fix a finite entry alphabet U, and introduce independent variables y_(r,a), with row space C^n and entry space U. Antisymmetrizing each column of a tensor gives its bottom-row minor, and multiplying gives a GL(U)-linear map from the column-wedge tensor F to Sym(C^n⊗U). Each minor is killed by the lower-row raising operators: replacing a present row by a later row duplicates a row inside its bottom-row set. The product has row weight (p_1,…,p_n).

1.15F1F2F3F4F5constructalgebra

Classical Cauchy decomposition follows from the actual published Schur–Weyl decomposition: identify the degree-N symmetric power with diagonal S_N invariants of (C^n)^tensor N⊗U^tensor N, then use the two Specht decompositions. The needed self-duality is complex linear: polytabloids have real coefficients, so their span is conjugation-stable; the bilinear tabloid form B(v,w)=sum v_T w_T is invariant and B(v,conjugate(v)) is the positive Hermitian norm. It is therefore nondegenerate on the Specht span. Schur's lemma with this explicit bilinear duality leaves one multiplicity space for each matching partition. The lower-row highest-weight line at (p_1,…,p_n) selects the partition (p_n,…,p_1), so the entire flag-minor image lies in the irreducible entry module of highest weight Lambda=Σ_j omega_(q_j). The ground product of minors is a nonzero polynomial. Hence the image is exactly this irreducible module. Actual16 proves that this constituent occurs once in F; therefore this nonzero normalized map has exactly the kernel of actual16's highest-component projection pi. No quantum flag algebra or quantum Peter–Weyl theorem is imported.

1.16F1F2F3F4F5constructalgebra

For different complex cosets, first apply the companion typed category equivalence and use one independent set of variables for each coset. The same Cauchy proof applies to each coset's columns, with their retained sorted heights. Multiplication across the disjoint variable sets is injective on the tensor product. Thus the kernel is the sum of the component projection kernels, exactly the off-standard lower-basis kernel of the product of actual16 models. The shift a↦a−c_kappa+n−n_kappa and inf I_kappa=1−n_kappa is explicit in that companion proof.

1.17F1F2F3F4F5constructalgebra

V is exact on the genuine parabolic category and sends N(A) to its finite-Levi standard V(A). Actual16 identifies [L_O(A)] with its source positive-parameter dual-canonical vector L_A at parameter1. Its projection pi L_A is zero exactly off Std. The preceding flag-minor factorization consequently gives zero row-torus character of V(L_O(A)) for every off-standard A. Positivity of actual module characters makes V(L_O(A))=0.

1.18F1F2F3F4F5constructalgebra

The kernel of the Grothendieck map of V is stable under every residue e/f operator, because the actual tensor identity and Casimir/flip compatibility give V e=e V and V f=f Wh. Thus after quotienting by the already-known off-standard kernel, any additional kernel would be a submodule of actual16's irreducible highest component (or the irreducible tensor product for the direct sum of coset root algebras). The ground class survives: its V image is the one-dimensional C_c by the induced-module computation. Hence no additional kernel exists. Every Std simple therefore has a nonzero V image. This argument does not presume that image simple, does not rely on injectivity of the exponential evaluation on the entire abstract polynomial module, and does not require a classification of all finite-dimensional W simples.

1.19F1F2F3F4F5constructalgebra

Take finite alphabets containing the relevant finite labels and tensor words, with the proved boundary block projections; actual16 gives compatibility under enlarging the cuts. The argument applies on each cut and hence to every object in the selected finite degree/category. All comparisons use integer order within a coset, not an order on C.

1.20F1F4F7constructalgebra

The actual highest-component projection π is module-linear and, in its integral L/D bases, is the coordinate projection with πLA=0 off Std and πLA=DA on Std. Its kernel is therefore a direct summand, and specialization at parameter one gives exactly K=⨁A∉StdZLA(1), with no extra specialization kernel. For a nonstandard simple, exact residue translation and the source K0 dictionary give [fiLO(A)]∈K and [eiLO(A)]∈K. Expanding these actual modules in their simple classes and projecting gives a sum of independent DB(1) with nonnegative composition multiplicities; each standard-label coefficient must vanish. Exactness then proves that the Serre subcategory of objects with only off-standard composition factors is stable under both residue functors. In several complex cosets apply the product of component coordinate projections and the typed residue shift iint=i−cκ+n−nκ. To treat finitely many objects or elementary moves outside an initial admitted cut, shift every origin down by a sufficiently large common integer; the category, cosets and standard predicate are unchanged and all those labels lie above the new ground. No order on different complex cosets is used.

1.21F1F4F7constructalgebra

Every standard N(C) embeds in an iterated lowering translate of a standard simple. To construct the monomorphism, shift the entries of column j upwards by an integer kj≥0, choosing these successively so that every shifted entry in that column is greater than every earlier-column entry in the same coset. The resulting B is standard and minimal in its fixed-multiset Bruhat orbit; the triangular standard/simple multiplicity matrix gives N(B)=LO(B). For each column j=2,…,l, list its original entries increasingly and lower its smallest entry from a+kj to a, then its next entry, and so on, using ea+kj−1,…,ea in that chronological order. At each step the distinguished change in column j is valid: its smaller entries already have their original values, while its larger entries and the later columns remain above the required range. Every other valid change occurs in an earlier column and gives a strictly smaller label in the prefix Bruhat order. The distinguished standard is therefore the largest section of the multiplicity-free residue standard flag. Move it to the bottom by splitting adjacent extensions. Indeed the projective-cover kernel of N(D) is filtered by standards N(E) with E>D, while Hom⁡(N(E),N(C))=0 unless E≤C, since a nonzero image has its LO(E) head as a composition factor of N(C). Thus for largest D and smaller C, every map from that projective kernel to N(C) vanishes; the projective-cover exact sequence gives Ext⁡1(N(D),N(C))=0. This proves the precise splitting orientation locally from the highest-weight suppliers. This produces an actual monomorphism at each elementary step. Exactness preserves these monomorphisms under the remaining lowering functors, giving N(C)↪ei1⋯eirLO(B). For mixed cosets the same construction is performed only among comparable entries; the typed standard and tensor equivalence transports the inclusion.

1.22F3F8constructalgebra

Prove the raw centralizers here before using any Morita conclusion. Give M its finite box grading, let C be the image of W and D the right Hecke image regarded as operator algebras, and give them the induced integer filtrations in End⁡(M). They commute by the actual tensor model. The loop/PBW symbol dictionary [F8] gives A0⊆gr⁡C for the unital image of the character-twisted U(ge) representation, and the Hecke symbol dictionary gives D0⊆gr⁡D for the truncated polynomial/permutation image. The character κc defines the automorphism u↦u+κc(u)1 on primitive centralizer generators, with inverse given by −κc, so A0 is EXACTLY the untwisted unital Vust image; the degree-zero scalar origin terms remain present in the full representation. Vust gives Z(D0)=A0 and Z(A0)=D0. Taking leading terms of commuting operators yields A0⊆gr⁡C⊆gr⁡Z(D)⊆Z(gr⁡D)⊆Z(D0)=A0, and interchanging C,D gives D0⊆gr⁡D⊆gr⁡Z(C)⊆Z(gr⁡C)⊆Z(A0)=D0. All inclusions are equality. This uses the declared raw loop/PBW/Vust suppliers and has no dependency on the later double-centralizer theorem's Morita clause.

2.1F2F6step 1.7step 1.8constructalgebra

Put DχN=⋃r≥1(N/IrN)∗ with the RIGHT U(g) action proved above, and HN=Wh⁡right(DχN)=Hom⁡m(N,Cχ). The original-head right-normalizer theorem [F6] gives [ηhead(w),x]∈IU(g) for the SAME original W⊂U(p), not an unidentified reflected algebra. Thus (fw)(v)=f(ηhead(w)v) preserves HN, since its commutator error starts with a shifted m generator killed by f. Finite duality now defines the genuine covariant left W action on V(N)=HN∗. Precomposition with a source morphism intertwines this action, proving functoriality. The numerical identity ηhead−ηtail=−tr⁡mad⁡ is consistent with the two column counts, but the actual original-head normalizer theorem supplies the algebra identification.

2.2F6step 1.9constructalgebra

The inverse Y=X−1 is the finite sum of descending-column paths, with a length-t path product multiplied by (−1)t. Prove [ηheadYij,Ers]+ηheadYirδsj∈IU(g) directly from this path sum. Before the unique possible column-A vertex, every factor belongs to a larger prefix W and therefore normalizes the right ideal; after it, the factors have disjoint support from Ers. Reduction of the product commutator is consequently legitimate. The surviving bracket replaces a factor starting at r by its factor starting at s. Pair the path which next visits s with the path omitting that visit; the products coincide because Xss=1 and their signs are opposite. Only the terminating visit s=j remains, with sum −ηheadYirδsj. This proves the right inverse equation without multiplying arbitrary right-ideal congruences on their left. Adjacent negative matrices generate m, so the commutator rule propagates both matrix equations to every negative generator.

2.3F2F5step 1.4step 1.7constructalgebra

The ordinary finite tensor pairing restricts to Dχ(N⊗Z)≅DχN⊗Z∨ as right U(g) modules. Continuity is checked on both sides: take an Engel flag with b successive factors on which m acts trivially. If Ir kills each coefficient functional on N, expanding the diagonal shifted action shows that Ir+b kills the tensor functional. Conversely use the flag successively: on a successive quotient the diagonal shifted action is its first-factor shifted action; subtracting the already-controlled lower-flag coefficients gives a fixed larger first-factor exponent for each coefficient. Induction through the finite flag proves that all coefficient functionals lie in DχN. This establishes equality of the continuous subspaces as well as the uncompleted tensor-dual equality.

2.4F1F7step 1.20step 1.21constructalgebra

If a simple LO(A) embeds in N(C), compose with the monomorphism of step 1.21 and use repeated biadjunction to obtain a nonzero, hence surjective, map fir⋯fi1LO(A)→LO(B) with B standard. Step 1.20 excludes this when A is nonstandard. Thus the socle of every standard has only standard labels. For a simple submodule of a standard-filtered module, choose the first filtration term it intersects nontrivially: it lies in that term, has zero intersection with the preceding term and embeds in the corresponding standard section. Consequently EVERY standard-filtered module has standard-label socle, including all projectives and the tensor object T. This is a statement about actual submodules, not about its entire list of composition factors.

2.5F8step 1.22constructalgebra

An operator in Z(D) has, by step 1.22, the same largest homogeneous symbol as a member of C. Subtract that member to lower its integer degree. The finite grading of M bounds the endomorphism filtration below, so this procedure terminates and gives Z(D)=C. Interchanging the two images gives Z(C)=D. Restoring the right-action opposite convention proves Wd=End⁡B(M) and B=End⁡W(M)op, where B is the cyclotomic IMAGE algebra. For tensor degree d=0 both images are scalar; for an empty pyramid and positive degree both images and both commutants in End⁡(0) are zero. No admissibility, stable injectivity, projectivity or Morita assertion entered this raw filtered argument.

3.1F1F2F6step 2.1constructalgebra

For N=Ind⁡pgD with finite-dimensional D, PBW gives N=U(m)⊗D. Restriction r(f)(d)=f(1⊗d) identifies HN with D∗; its inverse is f^(u⊗d)=χ(u)f(d). Moreover r(fw)(d)=r(f)(ηhead(w)d). Hence r∗:D→V(N) is W-linear for the head-twisted action w∘d=ηhead(w)d. For every p-map b:D→D′, (Ind⁡b)(1⊗d)=1⊗b(d) makes the restriction square commute, so V(Ind⁡b) is the ACTUAL map b under these identifications. This proves induced quotient and antisymmetrizer naturality without using equality of characters or presuming right-Hecke linearity. In particular V(N(A)) is the finite-Levi standard V(A); a source standard is not asserted simple.

3.2F5F6step 1.9step 2.2constructalgebra

The two matrix equations persist under direct sums and summands by an adapted basis and uniqueness of the triangular left lift. For tensor factors Z,Z′ put δZ=(id⊗ρZ)Δ, XZ⊗Z′=δZ(XZ′)(XZ⊗1) and YZ⊗Z′=(YZ⊗1)δZ(YZ′). Inserting the two successive left/right Whittaker lifts proves their equations, and these displayed products are inverse. Modules with trivial derived slN action use identity matrices, including central Jordan multiplicity spaces. Complete reducibility of slN writes each finite-dimensional module as a sum of a derived irreducible tensored with such a multiplicity space; finite-dimensional dominant-weight classification and exterior antisymmetrizers realize the derived irreducible as a summand of natural tensor powers after a scalar-character correction. Thus every finite-dimensional g-module Z has these double-admissible matrices. This algebraic construction also allows central Jordan multiplicities; the category-O tensor compatibility below requires a Cartan-semisimple tensor factor. The usual left contragredient Z∗ and the right vector-space dual Z∨, defined by (ϕa)(z)=ϕ(az), keep their separate action conventions; no Z∗=Z identification is used.

3.3F1F4F7step 1.18step 2.4constructalgebra

The ground central-character multiset determines a unique column-strict label. Within each charge coset its smallest entry cκ+1−n occurs once per column; strictness permits that entry at most once in each column and only at its bottom, so its multiplicity forces every such bottom entry. Remove these entries and repeat with the next minimum in every remaining column. Induction fixes all ground entries. Different charge cosets are distinct and are never compared. In the source convention λi=ai+i−1, the coordinates λi+ρi=ai+(N−1)/2 show that the central character is precisely this entry multiset. Hence the ground block has the sole column-strict label Ac. The generalized standard has diagonal simple multiplicity one and no other simple label in this block, so N(Ac)=LO(Ac). Actual BGG reciprocity and the projective standard flag give (P(Ac):N(Ac))=1 and no other section, so Pc=P(Ac)=N(Ac)=LO(Ac). Simple-preserving restricted duality makes this simple projective injective. The typed coset equivalence transports the same proof to every admissible complex origin. Tensoring has the exact ordinary-contragredient tensor adjoint on both sides, so T=Pc⊗V⊗d is projective-injective. Simple-preserving restricted transposition duality fixes Pc and the natural module and commutes with this tensor product; hence T is self-dual. Its standard flag follows from the actual parabolic tensor identity, so step 2.4 gives a standard-label socle and duality gives a standard-label head. Conversely every degree-d standard label A is an incoming crystal move f~iB from a degree-d−1 standard label, except ground in degree zero. Inducting from the ground quotient, exact fi gives fiTd−1↠fiLO(B)↠LO(A) using the ACTUAL simple-head theorem; fiTd−1 is a summand of Td, so LO(A) is a quotient of Td. Lift any such quotient through its projective cover. Essentiality of the cover makes the lift Td→P(A) surjective, and projectivity of P(A) splits it. Therefore the projective summands of Td are exactly the covers of the standard-label simples, with positive multiplicities; they are injective as summands of Td. It follows that every nonzero submodule X⊆Td has a nonzero standard-label simple socle. Exact V and the nonvanishing already proved in step 1.18 then give V(X)≠0. This proves the required detector; it does not assert that every composition factor of Td is standard or that Td generates the whole parabolic category.

4.1F2F6step 3.2constructalgebra

For a finite-dimensional left W module M, the left Whittaker lift of m⊗zj is ∑i(Xij⋅1χ⊗m)⊗zi; the right lift of f⊗zi is ∑j(f⊗1χ⋅Yij)⊗zj. The matrix equations put these vectors in the appropriate Whittaker spaces. For the natural module each lift respects the finite column flag and has diagonal 1χ⊗m⊗zj; the tensor, direct-sum and summand constructions of step 3.2 retain a finite flag with trivial m sections. The local cohomology supplier gives vanishing positive twisted cohomology on Qχ⊗WM. On its tensor product with this flag, the long exact sequence therefore makes invariants exact on successive sections, identifying each section with M tensored with the corresponding trivial section. The lift induces the identity there. Finite filtration induction proves it is an isomorphism. The same argument for the reflected right pair proves invertibility of the right lift. This is exactly the cohomology/flag argument of the repaired Skryabin tensor proof, applied to the two displayed lifts. Set AZ(w)=YZδZ(w)XZ. Left Whittaker invariance makes its entries elements of the ORIGINAL W. The identity δZ(w)XZ=XZAZ(w) gives w(m⊗zj)=∑iAZ(w)ijm⊗zi; YZδZ(w)=AZ(w)YZ gives (f⊗zi)w=∑jfAZ(w)ij⊗zj. The head/tail shifts add Lie characters, so their coproduct identities reduce both computations to the same unshifted δZ. Therefore the perfect finite pairing ⟨f⊗ϕ,m⊗z⟩=f(m)ϕ(z) is a MODULE pairing: (M⊛Z)∗≅M∗⊛rightZ∨. This is the necessary algebra-action argument, rather than a vector-space duality substituted for it.

4.2F1F2F3F4F5constructalgebra

Fix an admissible origin: c_j−c_k integral implies c_j=c_k. The original arbitrary-origin deformed tensor algebra remains separate and unrestricted. In a column of height q whose global row numbers are n−q+1,…,n, write its strict entries a_1,…,a_q. The genuine head-model action proved in step 3.1 makes its finite-Levi highest weight nu_s=a_s+n−q+s−1. This follows directly from the global highest weight lambda_i=a_i+i−1 and eta_head diagonal shift n−q_1−…−q_col: the column-reading position i=q_before+(global_row−n+q) gives lambda_i+eta_head=a_i+global_row−1.

5.1F2F6step 2.3step 4.1constructalgebra

Let Z be a finite-dimensional Cartan-semisimple g-module. Then N⊗Z is again a genuine parabolic object: its weights are sums of weights of N and Z, and local finiteness for p follows from U(p)n⊗Z being finite-dimensional for each n. It is finitely generated over U(m) by tensors of generators of N with a basis of Z: induction on word length uses xn⊗z=x(n⊗z)−n⊗xz. Thus its V image is defined on the stated domain. Apply the original-head right Skryabin counit HN⊗WQχ,right→DχN, f⊗a‾↦fa. Tensor it with Z∨, apply right Wh and use step 2.3 to obtain HN⊛rightZ∨≅HN⊗Z. Combine this actual counit with the module pairing of step 4.1 and take finite duals. This gives the natural W isomorphism νN,Z:V(N⊗Z)→V(N)⊛Z for EVERY genuine parabolic object N, including objects without an induced-module realization. Coassociativity, counit associativity and the inverse product formulas of step 3.2 make its two iterated tensor constructions agree under transported associativity. Naturality in a map of finite tensor factors follows from its ordinary dual map and the basis-independent evaluation pairing; hence adjacent flips are intertwined.

6.1F2F3F6step 1.9step 2.2step 4.1step 5.1constructalgebra

Compute the actual Casimir coefficients in ordinary box matrix units. On the LEFT lift, the coefficient at vk after Ω=∑Eab⊗Eba is ∑hEh,kηtailXhj. Positive matrices give (Eh,k−δhkρktail)Xhj after undoing the shift. Negative matrices give χ(Eh,k)Xhj−Xkj by step 1.9. Their total scalar is −ρktail−∑b>col⁡(k)qb=qcol⁡(k)−n. On the RIGHT lift the coefficient at vh is ∑kηheadYikEh,k; step 2.2 moves negative matrices left, giving χ(Eh,k)Yik−Yih, and the total scalar is −ρhhead−∑b<col⁡(h)qb=qcol⁡(h)−n. Multiplying by Y on the left or X on the right therefore gives the SAME entries Cj,i=∑col⁡(h)≤col⁡(k)Yi,kEh,kXh,j+∑k(qcol⁡(k)−n)Yi,kXk,j+∑row⁡(h)=row⁡(k), col⁡(h)=col⁡(k)−1Yi,hXk,j. There is no extra displacement sign on the ordinary Eh,k; signs are already in X,Y. The entries lie in W because the Casimir preserves the actual Whittaker subspace. The module pairing now intertwines the two transported Casimirs, while the continuous tensor pairing transposes the source Casimir term by term. Hence ν intertwines the source and target Casimir maps. With flip compatibility this also intertwines their polynomial and generalized-eigenspace residue projections, with the usual contragredient retained for reverse translation.

7.1F1F2F3F4step 3.1step 5.1step 6.1constructalgebra

Fix the head-normalized ground map i0:V(Pc)→Cc obtained from step 3.1 and the finite-Levi character calculation below. Iterate ν on Pc⊗V⊗(d−1) to obtain id:V(Pc⊗V⊗d)→Cc⊛V⊛d, and compose with the proved ACTUAL balanced tensor map μd to get jd. Casimir and flip compatibility prove (W,Hd)-bimodule linearity. Any source endomorphism b is transported as jdV(b)jd−1; in particular a native Casimir/place word representing right multiplication by h becomes the actual map m↦mh. This identifies maps in the cyclotomic IMAGE algebra, without asserting a faithful abstract Hecke action outside its allowed range. The construction uses no origin integrality. Typed category-O/coset transport is used only for the selected admissible-origin source labels and their character dictionaries, whereas the unrestricted deformed tensor model retains its arbitrary origins.

8.1F1F2F3F4step 6.1step 7.1constructalgebra

Hd acts on T by the universal tensor Casimir and places. At the first tensor step the actual finite p flag of the natural module has one standard section per column. On the jth section, the ordinary quadratic-Casimir identity Ω=(Ctotal−Csource−CV)/2 gives eigenvalue cj+qj−n. Successively applying the factors in the column-order flag makes ∏j(x1−(cj+qj−n)) annihilate T; subsequent tensor factors leave this first-step relation intact. Hence the source action factors through the genuine cyclotomic algebra, not only its V image. Step 7.1 transports it to M=Vc⊗d as the actual (W,Hd) bimodule action.

8.2F1F2F3F7step 7.1step 3.3step 2.5constructalgebra

V maps End⁡g(T)op into End⁡W(M)op=B by step 2.5, and its image contains B because every target Hecke operator is the transport of its actual source Casimir/place operator. A nonzero source endomorphism has a nonzero image X⊆T. Step 3.3 proves V(X)≠0, and exactness identifies V(X) with the image of its transported endomorphism. Hence the endomorphism map is injective as well as surjective, giving End⁡g(T)op=B. Detection uses the standard-label SOCLE criterion, never a claim that all composition factors of T are standard.

9.1F1F2F3F4F5F7step 1.18step 3.3step 8.2constructalgebra

Choose a full finite projective generator Q of the genuine O summand containing T as an explicit summand and write its algebra as A; the projector onto T is e and B=eAe. The exact Schur functor is e(−). It kills precisely the offStd simples. Its left adjoint Ae⊗_B− is right exact and satisfies e(Ae⊗X)=X. The counit Ae⊗eN→N has kernel and cokernel killed by e. Applying V sends it to an isomorphism. Therefore V factors through e(−), and its factor F on B-mod is naturally M⊗_B− by finite free presentations. This factor is exact: the only failure of exactness after the left adjoint is killed by e and hence by Wh. It is faithful, since every B-simple is eL_O(A) for a Std label and its V image is nonzero; exactness then detects every nonzero image of a morphism.

10.1F1F2F3F4F5F8step 2.5step 9.1constructalgebra

A finite-dimensional right B-module whose tensor functor is exact is projective. Explicitly, take its finite projective cover P→M with kernel K⊂P rad B. Tensor the inclusion K→P with B/rad B; flatness makes K/K rad B inject into P/P rad B, but this map is zero, so Nakayama gives K=0. Faithfulness forces every right indecomposable projective to occur in M: otherwise tensor with the corresponding left simple would vanish. Thus M_B is a progenerator. The first independently proved raw centralizer identity in step 2.5 gives Wd=End_B(M). The usual generator presentation/evaluation argument now gives the genuine Morita equivalence Wd-mod≃B-mod. In particular F sends B-simples to Wd-simples, proving the full relevant V simple-image claim without assuming it earlier.

11.1F1F2F3F4chooseconstructalgebra∎

Tensor compatibility and the actual Casimir/flip intertwiners are proved in steps 1.9–1.18, using the original head/right normalizer and the actual balanced Skryabin map. Thus V(Pc)=Cc and V(Pc⊗V⊗d)=Vc⊗d. The preceding kernel/Morita construction proves V(LO(A))=LW(A) for standard labels and zero otherwise; it never asserts that the image of a source standard N(A) is simple. The normalized comparison is determined on the ground and its tensor words, hence on the detecting tensor bimodule and on finite free quotient presentations through the established exact Morita factorization. Its ground normalization removes scalar ambiguity. This proves the stated properties of the genuine Whittaker functor, while keeping it distinct from the Hecke Hom quotient.

Remarks

  • The proof uses the continuous χ-dual and its right action; plain row-restricted duality does not make an ordinary category-O object Whittaker. Source simples and standard objects have separate names throughout.

  • The definition deliberately separates three functors that are often conflated: the genuine Whittaker functor V on category O, the Hecke Hom quotient Hom⁡g(T,−), and the Morita equivalence on the finite-W side. Only the first is defined here; the quotient is defined two items later.

  • The nonintegral-origin construction uses the typed Harish-Chandra comparison of the source (all-weight Verma comparison, Ore twists, coset sorting), which is the content of the declared local supplier interfaces [F4]; those interfaces are recorded as dependencies and their proofs are supplied by their own items.

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

The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer

Statement

Assume the Axiom of Choice. Fix the pyramid λ with columns q1≥⋯≥ql, an origin c∈Cl, and d≥0, and let Vc⊗d be the truncated tensor space of The deformed tensor space for the type-A finite W-algebra. Let Wd=φd(W(λ))⊆End⁡(Vc⊗d) be the image of the finite W-algebra and let Bd=ψd(Hd(Λ)) be the image of the cyclotomic Hecke algebra of The degenerate cyclotomic Hecke algebra under the right action. Then:

  1. Wd and Bd are mutual centralizers on Vc⊗d, for every complex origin c and every d, and their associated graded image algebras are the corresponding images of U(ge) and of the truncated polynomial/permutation algebra.
  2. For a nonempty pyramid, if ql≥d, then the action of the full cyclotomic algebra Hd(a) is faithful.
  3. If c is admissible (that is, ci−cj∈Z implies ci=cj), then the tensor module is a progenerator and Hom⁡Wd(Vc⊗d,−) is a Morita equivalence between Wd-mod and Bd-mod.

Mutual centralizers alone do not imply Morita for arbitrary c: the explicit example with c=(0,1), q=(1,1), d=2 in step 7.1 below has a nonprojective left Wd-module.

Facts & Assumptions

Given: The pyramid λ, an origin c, the truncated tensor space Vc⊗d, and the image algebras Wd, Bd.

[F1]

In the fixed loop chart, the associated graded left representation is the character-twisted Vust representation X↦∑tX(t)+κc(X)id⁡. Its unital image is exactly the untwisted Vust image, because it is obtained by the automorphism X↦X+κc(X)1 of U(ge). The right graded image is the ordinary truncated polynomial/permutation image. These image algebras are mutual centralizers for every Jordan type and every degree, including scalar degree zero and the empty-pyramid zero tensor case (The deformed tensor space for the type-A finite W-algebra, Vust's graded double centralizer for the type-A nilpotent centralizer).

[F2]

W(λ) has a separated loop filtration with associated graded U(ge), and the cyclotomic quotient has the bounded monomial basis x1r1⋯xdrdw with 0≤ri<l; both filtrations are compatible with the bimodule structure (The loop filtration on the type-A finite W-algebra has associated graded U(g^e), The degenerate cyclotomic Hecke algebra).

[F3]

The genuine original-head Whittaker comparison is exact, identifies induced standards with their head-normalized finite Levi modules and scalar content central characters, sends standard-labelled simples to the distinct exhaustive finite-image simples and other simples to zero, and intertwines both ordinary tensor functors with V and V* and the actual right Casimir/flip operators; the standard-label crystal supplies predecessor head quotients, and the category-O detector contains every standard projective cover and has only standard labels in its head and socle (Skryabin's equivalence for the type-A Whittaker pair, The Whittaker functor from the relevant parabolic category-O summand).

[F5]

The genuine standard/Casimir interfaces proved in The Whittaker functor from the relevant parabolic category-O summand supply the admissible character/quotient computations.

Proof

technique · direct

Given: The filtered bimodule Vc⊗d, its actual character-twisted graded representation and its unchanged unital Vust image algebras.

1.1F1F2constructalgebra

The graded unital images. Write E=V⊗d, C=Wd, and D for the right Hecke image viewed as an algebra of operators on E. The supplied actual tensor model in F1 gives commuting filtered operator algebras, with the graded symbols containing the unital images A0 of U(ge) and D0 of the truncated polynomial/permutation algebra. The character automorphism in F1 gives exactly the same A0 as the untwisted representation; no equality of the fixed-chart twisted and untwisted modules is inferred. Since A0,D0 are mutual centralizers, taking leading homogeneous terms of commuting operators gives A0⊆gr⁡C⊆gr⁡Z(D)⊆Z(gr⁡D)⊆Z(D0)=A0, where Z is the commutant in End⁡(E). Interchanging C,D gives D0⊆gr⁡D⊆gr⁡Z(C)⊆Z(gr⁡C)⊆Z(A0)=D0. Thus every inclusion is equality, establishing strict equality of both graded images as well as their commutants.

1.2F3constructalgebra

The exact ordinary-dual adjoint. For a finite rational g-module E, Skryabin transports ordinary evaluation E∗⊗E→C and coevaluation C→E⊗E∗ to the tensor functors FE(M)=M⊛E. The ordinary zigzag identities give both adjunctions between FE and FE∗. These functors are exact: tensoring is exact, it preserves generalized Whittaker modules by a finite Engel-flag nilpotence bound, and Skryabin is an exact equivalence. They preserve Rc: a faithful finite image module embeds the regular algebra into a finite direct sum of copies of itself by evaluation on a basis, so every finite-image module is a subquotient of a finite sum of tensor modules; exact tensor transport sends degree d to degree d+1. For N>0, also V∗=⋀N−1V⊗det⁡−1, and the exterior power is a summand of a tensor power by the antisymmetrizer. Determinant shifts therefore give closure under V∗ too. Consequently FV preserves projectives in the entire rational category through its exact right adjoint FV∗. Here V∗ is the ordinary contragredient natural module, distinct from V; the transpose contravariant duality of category O is not this adjoint.

2.1F1F2step 1.1constructalgebra

The filtered centralizers. For an operator in Z(D), equality of the induced graded spaces in step 1.1 supplies a member of C with the same leading symbol. Subtracting lowers its integer filtration degree. The finite grading of E bounds the induced endomorphism filtration below, so this terminates, proving Z(D)=C. The same procedure proves Z(C)=D. Returning to the right-action opposite convention gives both mutual-centralizer identities and the stated associated graded image algebras. At degree zero both images are scalar, while for an empty pyramid and positive degree E=0 and both are zero; these are already covered by the actual tensor model of F1. This proves clause (1) for every origin, without a Morita assumption.

3.1F1F2step 2.1constructalgebra

Stable injectivity. For a nonempty pyramid with ql≥d, choose d distinct terminal boxes on length-l Jordan strings. In the associated graded tensor action each bounded PBW word x1a1⋯xdadw, 0≤ai<l, sends their ordered terminal tensor to the tensor with those distinct strings permuted by w and each box moved ai places left. These ldd! outputs are distinct basis tensors, so the graded PBW word images are independent. A nonzero filtered Hecke element has a nonzero leading PBW symbol, hence a nonzero leading operator and a nonzero actual operator. Thus the raw action is faithful. For the empty pyramid, degree zero is the scalar identity and positive-degree tensor space and cyclotomic algebra are zero, so the action is faithful there too without using an undefined ql.

3.2F1F2step 1.1step 2.1constructalgebra

The finite-image row projectives. Assume c admissible. A row occupancy ν=(ν1,…,νn) determines a tuple jν of terminal row boxes and the diagonal row-multiset projection eν. Since the right tensor matrices preserve row multisets, eν∈Wd by step 2.1; these orthogonal idempotents sum to one. Here is the actual basis of their projective left ideals. For a commuting matrix ∑bi,jEi,j, place permutations identify diagonal Sd-orbits, and the U(p) image forces bi,j=0 when some source column is smaller than its output column. Comparing its coefficients with xk and replacing j by Rk(j) expresses each nonterminal coefficient in coefficients with larger total source column sum: the first term is bRk(i),Rk(j), the diagonal term is (ccol⁡(ik)+qcol⁡(ik)−ccol⁡(jk)+1−qcol⁡(jk)+1)bi,Rk(j), and the two remaining sums run over swaps (h k) with respectively both columns at most, or both columns greater than, the kth columns. Their signs are respectively plus and minus. This is terminating elimination from terminal source tuples. The graded string-orbit matrices are independent and indexed by the same terminal orbits, so step 1.1 makes the terminal-coordinate map an isomorphism. Let Ξi,jν be the normalized preimages. Evaluation on vjν gives exactly the orbit sums under ∏rSνr, which form the monomial basis of Zν=⨂rSym⁡νr(V≤pr) with its actual c-twist. Thus Wdeν≅Zν as actual modules, and the regular module is their sum. This proves these projectivities in the finite image, without invoking Morita.

4.1F5F3step 3.2constructalgebra

Projectivity of the ground object. For r≥0, take degree Nr and the one-dimensional determinant-shifted ground object Dr=Cc⊛det⁡r, with tableau Ac+r1. Its content reconstructs it uniquely among column-strict tableaux: in each charge coset the minimum appears in every column and hence in its bottom box; removing these boxes and repeating reconstructs all columns. Therefore its scalar central-character summand has exactly this one simple, by F3. The regular-module multiplicity of Dr is one. Indeed, the Levi decomposition of Zν uses semistandard tableaux of shapes given by the column partitions of ground differences, with the alphabet in column j consisting of the terminal row boxes whose rows reach that column. This follows by expanding the complete symmetric characters of its symmetric factors and using the Schur semistandard formula, or successive horizontal-strip multiplication; its finite radical filtration makes it an actual p-filtration by these Levi sections. For Dr the shapes are rectangles (rqj) and the allowed alphabet has exactly qj letters. Each length-qj strictly increasing tableau column must contain every letter in order. There is exactly one tuple, and its row-i multiplicity is rpi. Thus the coefficient is one for νi=rpi and zero for every other occupancy. Other standards cannot contain Dr because their scalar central characters differ. The supported regular summand has length one and is Dr itself, so Dr is projective over WNr. For a surjection in the rational finite-W category Rc, a common determinant twist puts its terms into finite sums of polynomial-image categories. The scalar degree operator splits these by degree. A map from Cc becomes a map from Dr into the degree-Nr summand, where it lifts by the projectivity just proved. The inverse determinant twist gives the original lift. Hence Cc is projective in Rc, without claiming projectivity in arbitrary W(λ)-mod.

5.1F3step 4.1step 1.2constructalgebra

The finite-W projective covers. Write VWh for the genuine continuous-dual functor V of The Whittaker functor from the relevant parabolic category-O summand, and put Q(A)=VWh(P(A)) for standard labels. At degree zero this is the ground object, projective by step 4.1. For a positive-degree standard A, the actual standard-label crystal supplies A=f~iB and a quotient LO(B)⊗V→LO(A). Lifting along the projective cover and splitting proves P(A) is a summand of P(B)⊗V. The genuine tensor comparison sends this to a summand of Q(B)⊛V, projective by step 1.2. To identify its head, write P(B)⊗V=⨁CP(C)mC with standard C, using the independently proved detector head/socle property in F3. Exact VWh gives dim⁡Hom⁡W(Q(C),LW(D))≥δCD. On the other hand ordinary-dual adjunction, the induction hypothesis and the genuine simple/tensor comparison give dim⁡Hom⁡W(Q(B)⊛V,LW(D))=[LW(D)⊛V∗:LW(B)]=[LO(D)⊗V∗:LO(B)]=mD. Comparing this equality with the sum over C forces dim⁡Hom⁡W(Q(C),LW(D))=δCD for every summand with mC>0. Thus each Q(A) is the genuine projective cover of LW(A). Exhaustion of finite-image simples and occurrence of every standard cover in the detecting tensor object now show that Ud=VWh(Pc⊗V⊗d) is a projective generator of Wd-mod. This uses the actual simple-image and tensor maps of F3, rather than inferring covers from characters or mutual centralizers.

6.1step 2.1step 5.1constructalgebra

Morita for the finite images. Since Ud is a finite projective generator of Wd-mod, every module admits a presentation by finite sums of Ud. The evaluation maps from the tensor-Hom adjunction are isomorphisms on Ud and its direct sums and summands, hence on every module by passing to the cokernels of such presentations. Conversely the same argument for presentations of modules over End⁡Wd(Ud)op gives the inverse evaluation. Thus Hom⁡Wd(Ud,−) is an equivalence with inverse Ud⊗Bd−, and step 2.1 identifies its target algebra with the genuine Hecke image Bd. This proves clause (3) under admissibility independently of any supporting-block Morita assumption. In the empty-pyramid case the positive-degree tensor and both image algebras are zero, so their module categories are zero and the equivalence is immediate; degree zero is the scalar equivalence.

7.1F1step 2.1constructalgebra∎

The nonadmissible boundary. For c=(0,1), q=(1,1), d=2, use the basis b=(v1⊗v1,v1⊗v2,v2⊗v1,v2⊗v2). The raw formula gives x1b1=x1b2=0, x1b3=b1−b2+b3, x1b4=b2+b4, and s1 swaps b2,b3 and fixes b1,b4. Put w=b1+b2+b3+2b4, let f(b4)=w/2 and f(b1)=f(b2)=f(b3)=0, and let N(b2)=N(b3)=b1, N(b4)=−b1, N(b1)=0. Solving the two linear commutation equations with x1,s1 gives Z(x1,s1)=span⁡{f,1−f,N}. Indeed f2=f, fN=Nf=N2=0, and direct coefficient comparison gives precisely these three free parameters. By step 2.1 this is Wd≅C×R, R=C[ϵ]/ϵ2. Its module decomposes as Cw⊕U, U=span⁡{b1,b2,b3}, where ϵ acts by N. The basis b2,b1,b2−b3 identifies U≅R⊕R/(ϵ). The last summand is not projective: a section of R↠R/(ϵ) would send 1 to an element killed by ϵ, hence to (ϵ), whose quotient is zero. Thus the tensor module is nonprojective over the left finite-W image, and the Morita conclusion fails, although the mutual centralizers still hold.

Remarks

Context only: The stable injectivity criterion: if e has at least d strings of maximum length l, the longest-string vector realizes the regular right module, so the right action is injective (Vust's graded double centralizer for the type-A nilpotent centralizer).

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

The Whittaker functor is exact and fully faithful on the required projectives

Statement

Assume the Axiom of Choice. For admissible origins c the genuine Whittaker functor V of The Whittaker functor from the relevant parabolic category-O summand is exact on Ocd, and γ ⁣:Hom⁡g(T,−)→Hom⁡W(Vc⊗d,V(−)) is a natural isomorphism, where T=Pc⊗V⊗d. Both V and the Hecke quotient Hom⁡g(T,−) are fully faithful on all projective objects of the relevant summand, and the quotient is also fully faithful on tiltings. T is a self-dual prinjective detecting object containing all standard-labelled projective-injective covers, each individually self-dual, but it need not be a generator of the entire category-O summand. V(T)=Vc⊗d is a projective generator of Wd-mod, and V preserves projectivity on add⁡(T); it need not send every projective of O to a projective W-module. The composite of V with the Morita equivalence is the Serre quotient killing exactly the off-standard simples.

Facts & Assumptions

Given: Assume AC. Fix admissible c, the finite whole-block summand Ocd, its standards N(A)=M(A), simples L(A), restricted duality D, ground Pc, detector T=Pc⊗V⊗d, genuine Whittaker functor V ⁣Wh, tensor image U=Vc⊗d, and right Hecke image B.

[F1]

The genuine continuous-dual Whittaker construction is exact, sends N(A) to its finite-Levi W-standard, kills precisely off-Std simples, and has a coherent bimodule isomorphism j:V ⁣Wh(T)→U. Its independent filtered loop/Vust construction proves the raw mutual centralizers before this factorization; stable faithfulness is established directly in step 11.1 below. Its actual tensor maps intertwine Casimir operators and crossings, including tensoring by the distinct contragredient V∗; its exact faithful factor through the corner has the form U⊗B− and is Morita. These are the local original-head/right-normalizer, continuous-dual, tensor and Nakayama constructions of The Whittaker functor from the relevant parabolic category-O summand. No simple-image classification is assumed before the factor/progenerator calculation there.

[F2]

Finite parabolic whole-block summands have projective covers, injective hulls, BGG reciprocity, standard/costandard Hom and Ext vanishing, and simple-preserving restricted duality (Parabolic category O is a highest weight category, The integral parabolic category-O blocks for higher-level Schur-Weyl duality, Standard- and costandard-filtered objects and tilting objects). In source Bruhat order, [N(C):L(A)] vanishes unless A≤C, and Ext⁡1(N(C),N(A))=0 unless C<A. PBW and ordinary polynomial Schur modules are PBW gives an ordered monomial basis for the enveloping algebra and Schur-Weyl decomposition and highest weights.

[F3]

The actual integral normalized Fock projection is module-linear, with coordinate kernel spanned by the dual-canonical LA for off-Std labels and independent images DA for Std; the simple-class dictionary at parameter 1 and exact biadjoint residue functors are Standard tableau monomials form a basis of the highest weight Fock submodule, The parabolic category-O Grothendieck group is the integral Fock module, Parabolic Kazhdan-Lusztig polynomials give the dual-canonical transition matrix and The residue translation functors give the integrable Fock-space action. The last supplier includes the actual simple crystal-head theorem. For admissible complex origins the same interfaces use the exact component shifts of Separated integral cosets give typed parabolic category equivalences.

[F4]

The cyclotomic algebra has its bounded PBW basis and symmetric top-coefficient trace, nondegenerate on every central block corner (The degenerate cyclotomic Hecke algebra). The actual row-weight operators on tensor space and the Casimir formula are those of The deformed tensor space for the type-A finite W-algebra; original path and Gauss coefficient expansions are The shifted Yangian and the pyramid generators of the type-A finite W-algebra. The finite-Levi standard has its entry-multiset scalar central character. Restricted transpose duality has a nondegenerate form on Pc and on V, so their tensor product supplies T≅DT, with the Casimir and crossings self-adjoint. This is transposition duality, not an assertion V∗=V.

Proof

technique · direct

Given: The objects, finite summands and local supplier contracts above. For the empty pyramid the degree-zero category and its Whittaker/Schur functors are finite-dimensional vector spaces with the identity functor and T0=U0=C; all positive-degree categories and tensor objects are zero. Every asserted comparison and copresentation is then immediate. The construction below treats the nonempty pyramid.

1.1F3algebra

The categorical nonstandard kernel. In the Fock L/D bases the normalized projection is a coordinate projection with coefficients 0,1, so specialization at 1 has precisely the off-standard span as kernel. Module-linearity makes this kernel stable under every Ei,Fi. Under [F3], expand [fiL(A)] for off-standard A as ∑CnCLC(1), where nC≥0 are actual composition multiplicities. Projecting gives ∑C∈StdnCDC(1)=0, and independence forces every such nC=0; the same holds for ei. Exactness extends this to the entire off-standard Serre subcategory. For complex c, apply the product of the component projections with entry and residue shift a↦a−cκ+n−nκ, nκ=max⁡j∈κqj; its coordinate kernel consists of labels nonstandard in at least one component. A common downward origin shift includes any finitely many labels and residue moves in an admitted cut and does not change Oc or the standard predicate.

1.2F2constructalgebra

Maximal ground-column induction. Split off the last column, with two-block Levi g′⊕g′′ and upper radical r, and define R(X)=U(g)⊗U(q)(Cβ⊗X), β=(0N′,(N′)ql), and right adjoint H(Y)=C−β⊗Yr. PBW gives exact R and R(N(C′)⊠N(C′′))=N(C). The top Levi slice of a simple is its Levi simple: a proper submodule of that slice would generate a proper global submodule by PBW. There are no additional lower r-invariants, since moving opposite-radical PBW monomials across the nondegenerate contravariant form pairs a lower invariant to zero against every vector. Hence H(L(C))=L(C′)⊠L(C′′). For a costandard, invariant functionals vanish on all positive-degree opposite-radical monomials, giving H(∇(C))=∇(C′)⊠∇(C′′). Taking the exact top eigenvalue slice of the first-block trace, when B,C have the same degree split, now gives [N(C):L(B)]=[N(C′):L(B′)][N(C′′):L(B′′)]: smaller top eigenvalues contribute nothing and the top Levi simple determines its concatenated label uniquely.

2.1F2F3step 1.1constructalgebra

Actual standard embeddings. Given C, shift columns j≥2 upward by integers kj≥0, chosen successively so each shifted entry in column j exceeds every earlier-column entry in its coset. The resulting B is standard and Bruhat-minimal, hence N(B)=L(B) by [F2]. Write column j of C as aj,1<⋯<aj,qj and set Ej=(eaj,qj⋯eaj,qj+kj−1)⋯(eaj,1⋯eaj,1+kj−1), composing rightmost first. Apply E2, then E3, through El: the smallest entry is lowered first. In each elementary standard flag, alternative valid lowers occur in earlier columns, hence have strictly smaller prefix Bruhat label. Our desired section is largest and can be moved to the bottom: each adjacent swap splits by the Ext ordering in [F2]. Thus each move gives an actual monomorphism of standards, and exact subsequent residue functors preserve it. Composition gives N(C)↪El⋯E2L(B). If L(A)↪N(C), biadjunction gives a surjection from an iterated fi image of L(A) onto the standard simple L(B); step 1.1 forbids this for off-standard A. Every standard therefore has standard-labelled socle.

2.2F2step 1.2constructalgebra

An actual cover isomorphism. Append the ground last column to B′. Every C≥B retains that ground column: a same-coset Bruhat move toward a larger label increases earlier-column sums, so the last-column sum cannot exceed its ground sum, whereas polynomiality makes each last-column entry at least its ground value. Equality forces all of them to be ground; admissibility excludes cross-coset swaps. Thus all C≥B have degree split (d′,0). Adjointness and step 1.2 show that X=R(P(B′)⊠Ccl+ql−n) has simple head L(B). Lift the cover map to obtain P(B)↠X, whose image is all of X because it surjects onto its head. By BGG and step 1.2 their standard-flag multiplicities agree in the fixed split and vanish elsewhere. The kernel of this existing epimorphism therefore has every composition multiplicity zero and is zero. Consequently X≅P(B); an equality of characters has only been used to kill the kernel of an already constructed map.

3.1F2F3F4step 2.1constructalgebra

The detector and the injective hulls it contains. The ground simple is projective-injective. Tensoring by V preserves both projectives and injectives because the distinct tensor functor −⊗V∗ is exact and adjoint on both sides. The tensor product contravariant form gives T≅DT. Every simple submodule of a standard-filtered object embeds in one of its successive standard sections, by taking the first section meeting it; hence step 2.1 proves standard socle for every projective and for T. Duality gives standard head for T. Every standard label of positive degree is f~iB for a lower-degree standard label by [F3]; induction using the actual crystal head of fiL(B) gives T↠L(A). Lift this epimorphism through P(A)↠L(A); essentiality makes the lift surjective and projectivity splits it. Thus the indecomposable summands of T are exactly the standard-labelled covers, all with positive multiplicity and all injective. Moreover I(A)=DP(A)∈add⁡(DT)=add⁡(T) for every standard A. This hull membership does not presume individual summand self-duality.

3.2F2step 2.2constructalgebra

Cumulative-column projectives. Put V≤j=E1⊕⋯⊕Ej and ZA=⨂iSym⁡ai(V≤col⁡(i)), with degree d=∑iai, and Z(A,c)=Ind⁡pg(C−ρ⊗ZA,c). Induct on the number of columns. One column is completely reducible. Removing the last column and using tensor identity gives Z(A,c)=R(Z(A′,c′)⊠Ccl+ql−n)⊗⨂i=N−ql+1NSym⁡ai(V). By induction and step 2.2 the first factor is a sum of actual projective covers. The remaining finite tensor product preserves projectives by its exact distinct-dual adjoint. Polynomial labels form whole blocks: their shared entry multiset cannot admit a below-ground entry, since column strictness would put an entry below the common coset minimum in the bottom row. Thus these ambient projectives lie in the required finite polynomial summand. Every Z(A,c) is genuinely projective.

4.1F2step 3.2constructalgebra

Every cover occurs and the quotient has a standard flag. For a label B, take A=B−Ac. Project each prefix onto its last-column Levi quotient. The tensor product of the resulting row symmetric powers surjects onto V(B): row symmetrization followed by column antisymmetrization of the row-filled tensor produces a nonzero polynomial highest vector, and Levi complete reducibility gives the simple Schur quotient. Exact induction gives Z(A,c)↠N(B)↠L(B), and projectivity plus essentiality of the cover makes P(B) a split summand of Z(A,c). Averaging symmetrizers embed ZA as a p-submodule of V⊗d; PBW preserves this injection and identifies the ambient induction with T. Its finite p-quotient has polynomial Levi simple sections: the radical acts nilpotently by the column filtration, and its invariant subspace in each simple section is Levi-stable and therefore the whole section. Inducing its composition filtration exactly gives a standard flag of T/Z(A,c).

5.1F2step 2.1step 3.1step 4.1constructalgebra

All-projective copresentations. For an indecomposable projective P, choose a splitting Z(A,c)=P⊕Q from step 4.1 and view P as its actual submodule of T. The sequence 0→Q→T/P→T/Z(A,c)→0 gives a standard flag of T/P, since Q is projective and has its BGG flag. Its socle is standard by step 2.1, so its finite injective hull I(T/P) belongs to add⁡(T) by step 3.1. Compose T↠T/P↪I(T/P) to obtain 0→P→T→I(T/P), exact at P,T. Finite sums give every projective a two-step copresentation 0→P→T0→T1 with both Ti∈add⁡(T). The last arrow need not be surjective.

6.1F2step 3.1step 5.1constructalgebra

The right-adjoint unit. Choose a full finite projective generator of the entire category-O summand containing T as an explicit summand, with algebra A, and let e be the projector onto this actual T. Thus eAe=End⁡g(T)op=B, retaining all its multiplicities. For F(X)=eX, B=eAe, the right adjoint is Ge(M)=Hom⁡B(eA,M) with unit ηX(x)(ea)=eax. The restriction eηX is an isomorphism, so its kernel and cokernel are annihilated by e. If X has standard socle then ηX is monic. In particular ηT is monic and splits since its source T is injective. A complementary summand C has eC=0, but adjunction gives Hom⁡A(C,GeFT)=Hom⁡B(eC,FT)=0, forcing its inclusion to vanish and C=0. Thus η is an isomorphism on add⁡(T). Apply exact F and left-exact Ge to step 5.1; the comparison of kernels gives ηP an isomorphism for every projective. Adjunction therefore proves F fully faithful on all projectives, while left-adjoint recovery has only been asserted on add⁡(T).

7.1F2step 2.1step 6.1algebra

Tilting full faithfulness. If X has standard head and Y standard socle, then ηY is monic and its cokernel is annihilated by e. Every map from X to that cokernel vanishes: a nonzero image would have a standard simple head because it is a quotient of X, while all its factors would be off-standard. By adjunction each B-map FX→FY gives X→GeFY, which therefore factors uniquely through Y. This proves the Hom isomorphism. A tilting's standard flag gives standard socle by step 2.1, and its costandard flag gives standard head by duality. Thus the quotient is fully faithful on all tiltings.

8.1F1step 3.1step 6.1step 7.1constructalgebra

The actual Whittaker comparison and quotient. By [F1] the exact Whittaker functor factors through F as the actual equivalence U⊗B−, with U a right B-progenerator and Wd=End⁡B(U). Its inverse is Hom⁡Wd(U,−), and its unit on FX is m↦(u↦u⊗m). Under the source action this is precisely γX(f)=V ⁣Wh(f)j−1, since the counit on T⊗BFX is evaluation; thus the comparison is a natural isomorphism of actual maps and Hecke modules. In particular U is a left Wd-progenerator, and V ⁣Wh is fully faithful on projectives by step 6.1. The corner functor F is the Serre quotient with kernel consisting of objects with only off-standard factors; applying the genuine equivalence identifies the same quotient for V ⁣Wh. Projectivity is preserved on add⁡(T), whose image consists of the corresponding projective covers. This does not assert preservation for other ambient projectives.

9.1F1F2step 3.1step 8.1algebra

Simple images and standard heads. The exact corner functor kills precisely off-standard simples and identifies its other simple images with the distinct exhaustive B-simples; the genuine equivalence of step 8.1 transports these to the corresponding finite-W simples LW(A). For standard A, P(A)∈add⁡(T), so πP(A) is an indecomposable B-projective with head πL(A): its Hom to each simple is the corresponding Hom from P(A) by the elementary add(T) equivalence. Lift P(A)→L(A) through N(A)→L(A); the image surjects onto the standard's head and is therefore the whole standard. Applying exact π makes πN(A) a nonzero quotient of this indecomposable projective, so it has the same unique simple head. Through Morita, the actual finite-Levi standard V(A)=V ⁣WhN(A) likewise has unique simple head LW(A). This does not assert that a specified finite-Levi highest vector generates it.

9.2F1F2F4step 8.1constructalgebra

Independent row compression. Add t full ground rows until the enlarged smallest column has height at least d; all roots aj=cj+qj−n remain fixed. For each row r, the normalized coefficient Dr(1) is its row-Cartan operator, with ground scalar κr=∑j: r lies in column jcj. On the actual tensor space and every finite-Levi standard of degree d its eigenvalues are κr+h, 0≤h≤d, since the remaining weight is polynomial row occupancy. Thus the SAME finite-image element e=∏r deleted∏h=1d(1−(Dr(1)−κr)/h) is the zero-deleted-occupancy projector on both tensor space and all these standards. In U+ it selects tensors using only retained rows. The actual dot formula preserves row multisets, so e commutes with dots and crossings and belongs to the left image by the independent raw first centralizer of [F1]. Each right matrix restricts identically under the retained-box embedding: left neighbours and row/column indices agree and its scalar aj is unchanged. Therefore eU+=U as right Hecke modules. Extending a commuting endomorphism of eU+ by zero shows eA+e=A, where A+,A are the large and small left image algebras. For the finite-Levi standard, the zero-deleted-occupancy part of Ccj⊗Sμ(j)(Cqj+t) is Ccj⊗Sμ(j)(Cqj) by its tensor Young-symmetrizer realization, and vanishes exactly when a deleted-row partition entry is nonzero. In the original path expansion, Levi projection kills off-column factors and each surviving strictly-forward path has at most one factor in each column. A deleted intermediate row changes removed-coordinate occupancy in a column with no later factor there to undo it; compression therefore kills that monomial. Remaining paths are exactly the small paths. The head shift in column j changes by −(j−1)t, cancelling the retained source-reading shift +(j−1)t; its normalized highest weight remains the entry plus row index minus one. The corner action and its Gauss coefficients consequently give eV(A+)=V(A) for contractible labels and zero for noncontractible labels, as actual module identifications.

10.1F1step 9.1step 9.2constructalgebra

Simple contraction without highest-vector assumptions. Every noncontractible standard simple is killed by e, because it is a quotient of the standard annihilated in step 9.2. For a finite algebra and an idempotent e, restriction gives a bijection between its simple modules surviving e and the simples of eAe: any nonzero vector in eL generates eL=eAev, and for a small simple M the module Ae⊗eAeM has a unique simple quotient surviving e. Indeed its e-part is M; every proper submodule has zero e-part, since a submodule containing that part generates the whole induced module. The sum of all such proper submodules is still annihilated by e and is the unique maximal submodule. Apply this to the independent corner in step 9.2. By step 9.1 both simple lists are complete, and small standard labels are in bijection with contractible large standard labels by adjoining full ground rows. Thus the survivors form a subset of the contractible list with exactly the same finite cardinality, so every contractible simple survives. Its restriction is a simple quotient of eV(A+)=V(A), which has the unique head from step 9.1, hence eLW(A+)=LW(A).

11.1F1F2F4step 9.2step 10.1constructalgebra

Fullness and the central Hecke corner. If a contractible A+ and another label have the same entry-multiset central character, admissibility separates charge cosets and identifies all charges within each coset. Its minimal bottom entry cj+1−(n+t) appears in each column of that coset; strictness and nonnegative ground differences force the same entries into the bottom row of the other label. Remove that row and repeat for every deleted row. Thus the contractible labels form a union of whole central-character blocks. Let f be their central support in A+; then e=ef=fe, since e kills all complementary simples. Every simple of Af=fA+f survives e by step 10.1. If AfeAf were proper, its nonzero quotient would have a simple killed by e, a contradiction. Hence f=∑kakebk. Multiplication Afe⊗eAfeeM→M has inverse m↦∑kake⊗ebkm; balancing and this identity verify both composites. This gives a faithful Morita equivalence on all supported-block modules. The operator f belongs to the right centralizer and is central there, so restriction identifies fB+f=End⁡Af(fU+)op with B=End⁡eAfe(eU+)op. To verify enlarged stable faithfulness directly, choose d distinct terminal boxes on length-l Jordan strings. In the associated graded tensor action each bounded PBW word x1a1⋯xdadw, 0≤ai<l, sends their ordered terminal tensor to the tensor in which those distinct strings have been permuted by w and the box on string i moved ai places left. These ldd! outputs are distinct basis tensors, so the graded PBW word images are linearly independent. A nonzero filtered Hecke element has a nonzero leading PBW symbol; graded injectivity makes its leading operator nonzero, hence its actual operator is nonzero. The enlarged stable action is therefore faithful, giving B=fHd(a)f. Its trace is therefore symmetric and nondegenerate by [F4]. This local proof precedes, and does not depend on, a later stable-range definition.

12.1F2F4step 5.1step 11.1constructalgebra

The actual duality comparison. Let β:T→DT be the tensor contravariant form. Put δM=Hom⁡g(M,T) with (bf)(m)=f(m)b∗, and X#=Hom⁡B(X,B) with the same twist. Transposition gives the natural isomorphism δM→πDM, f↦Df∘β, whose inverse is g↦β−1∘Dg∘bidual⁡M. This uses only T≅DT, not individual projective self-duality. Tensor-Hom gives δπ∗≅#, and the symmetric trace of step 11.1 gives #≅DB by h↦tr⁡∘h. Define θM:M→Dπ∗δM by θM(m)(t⊗f)=(t,f(m)). The form identity (xtb,t′)=(t,xtrt′b∗) makes this balanced and g-linear. Applying π gives a natural map π→πDπ∗δ≅#πD between exact functors; exactness of # follows from the symmetric algebra's injective regular module. On T it is the regular trace-duality isomorphism, and hence is invertible on add(T). Use the copresentations of step 5.1 and kernels to prove it invertible on every projective; use finite projective presentations and cokernels to prove it invertible on every object. Dualizing gives the genuine module isomorphism πD≅DBπ.

13.1F2step 3.1step 6.1step 12.1algebra∎

Individual standard prinjectives are self-dual. For standard A, I(A)=DP(A)∈add⁡(T) by step 3.1. Step 12.1 gives πI(A)=DBπP(A) and fixes its simple label because DL(A)=L(A). In a symmetric algebra the primitive projective BeA is also the injective hull of its corresponding simple: the perfect trace identifies its linear dual with the corresponding right ideal, and the ∗ twist sends the primitive to the primitive carrying the dual simple. Since that simple is fixed here, DBπP(A)≅πP(A). Both I(A) and P(A) are projectives, so full faithfulness of step 6.1 lifts this isomorphism and its inverse; their composites are identities by faithfulness. Hence I(A)≅P(A), so each standard projective-injective is individually self-dual. This last conclusion has been derived after the copresentation, central-corner and duality constructions, and was not used to prove them.

Remarks

The proof uses the full Col-labelled polynomial summand to construct the projectives Z(A,c) and their copresentations. The object T is a generator of its prinjective additive subcategory and a detector for submodules, and need not generate the entire category-O summand. Its composition factors include off-standard labels; only its head and socle are confined to standard labels. The right-adjoint recovery of all projectives is distinct from the left-adjoint recovery on add⁡(T).

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The higher-level Schur-Weyl projective generator and Schur functor

Definition

Keep the pyramid and admissible origins c of The Whittaker functor from the relevant parabolic category-O summand, the ground object Pc, the tensor object T=Pc⊗V⊗d and its central decomposition. For a charge α∈Q+ with ht(α)=d let Iα be the finite set of residue sequences of content α, and let Tα be the corresponding central component of T; in the integral model Tα=∑i∈Iαfid⋯fi1Pc, the sum of the residue-induction images of the ground object. Put Bα:=End⁡g(Tα)op, the corresponding central component of the Hecke image algebra (the opposite convention is fixed here), and define the Schur functor of the block by πα:=Hom⁡g(Tα,−) ⁣:Oαd→Bα-mod. Its left adjoint is πα∗:=Tα⊗Bα−.

For the whole polynomial Colcd summand, use the distinct finite projective generator Gd=⨁A∈TabdZ(A,c), with actual prefix symmetric modules Z(A,c) as constructed independently from the raw inducing modules in steps 1.2, 2.2, 3.2 and 4.1 of The Whittaker functor is exact and fully faithful on the required projectives. Every category-O projective cover is a summand of Gd; every Z(A,c) embeds in Td with a standard-filtered quotient. Exact projection gives Gα on the entire central block. The tensor detector Tα remains the object defining πα; Gα generates all Col labels, while Tα contains the standard-labelled projective-injective covers. These roles are distinct.

The verification below records the properties used on this page and marks the boundaries explicitly: πα is exact, being Hom from a projective object; its left adjoint is right exact but not exact in general; it sends Bα-projectives to projective objects and πα∗πα recovers add⁡(Tα), including every standard-labelled prinjective; neither exactness of πα∗ nor recovery of every category-O projective is asserted, both failing in the two-equal-charge rank-one computation in step 3.1 below. The components assemble as a locally unital sum over the charges, and all ambient labels, including those killed by π, remain in the category O.

Facts & Assumptions

Given: The ground object Pc, the tensor object T with its central decomposition, a charge α, and the objects Tα, Bα, πα.

[F1]

T is a self-dual prinjective detector: it contains all standard-labelled projective-injective covers, need not be a full generator, and the Whittaker functor is exact and fully faithful on the required projectives (The Whittaker functor is exact and fully faithful on the required projectives, The Whittaker functor from the relevant parabolic category-O summand).

[F2]

The residue-induction construction produces the central components Tα as images of the ground object, and the Hecke action endomorphisms give Bα=End⁡g(Tα)op on the admissible block (The integral parabolic category-O blocks for higher-level Schur-Weyl duality, Skryabin's equivalence for the type-A Whittaker pair, The deformed tensor space for the type-A finite W-algebra).

[F3]

Projective covers, tiltings and the standard/costandard filtrations exist and are classified; Grothendieck-group adjunction is available for the rigid-block arguments (Indecomposable tilting objects exist and are classified in parabolic category O, Standard- and costandard-filtered objects and tilting objects, The Grothendieck group and character of O).

[F4]

The actual prefix modules are projective in the whole finite Col summand, contain each projective cover as a direct summand, and embed in Td with standard-filtered quotients (The Whittaker functor is exact and fully faithful on the required projectives). The local construction in its steps 1.2, 2.2, 3.2 and 4.1 uses top-to-bottom ordinary readings and arbitrary admissible origins; its mixed-coset category-O basics transport through the proved separated-coset exact equivalence.

Proof

technique · direct

Given: The component Tα and the functor πα.

1.1F1algebra

Exactness of πα. Tα is a direct summand of the projective object T=Pc⊗V⊗d by [F1]; Hom⁡g(P,−) is exact for projective P, and passing to a direct summand preserves exactness, so πα is exact.

1.2F2F3algebra

The left adjoint. The tensor-Hom adjunction gives πα∗=Tα⊗Bα− as left adjoint of πα; tensoring with a right module is right exact but not left exact in general, and the rank-one witness exhibits the failure of exactness. Free Bα-modules map to direct sums of copies of Tα, which are projective, and direct summands of projective objects are projective, so πα∗ sends Bα-projectives to projectives.

1.3F4algebra

The whole-summand generator. By [F4], the finite sum Gd is projective and contains every Col-labelled cover; exact central projection gives the projective generator Gα of the whole block. The same supplier gives actual inclusions of each prefix summand in Td with standard-filtered quotients, providing the projective-copresentation prerequisite without identifying Gα with the detector Tα.

2.1F2step 1.2algebra

Recovery on add⁡(Tα). The evaluation πα∗πα(Tα)=Tα⊗BαEnd⁡g(Tα)→Tα is an isomorphism by the endomorphism-algebra description [F2] (the standard evaluation of a free rank-one module), and for direct summands it follows by restriction of idempotents; hence πα∗πα recovers every object of add⁡(Tα), in particular every standard-labelled prinjective contained in Tα.

3.1F1F2F3step 1.2step 2.1constructalgebra

The rank-one boundary. Take q=(1,1), c=(0,0) and d=1. The ground sl2 highest weight is −1, and its natural tensor gives the regular-block detector T=P(−2). The rank-one Verma formula efkv=k(λ−k+1)fk−1v gives the nonsplit sequence 0→L(−2)→Δ(0)→L(0)→0 and Δ(−2)=L(−2). BGG reciprocity in [F1] gives P(0)=Δ(0) and the nonsplit flag 0→Δ(0)→T→L(−2)→0; the flag cannot have Δ(0) on top because the cover has head L(−2). Thus T has head and socle L(−2) and middle factor L(0). Let x be its head-to-socle endomorphism. Then x2=0, and the level-two d=1 endomorphism algebra is R=C[x]/x2 by the supplied Hecke identification. Any map T→P(0) has image in soc⁡P(0)=L(−2): its composite to L(0) is zero. Hence πP(0)=R/(x), and π∗πP(0)=T/xT has head L(−2), whereas P(0) has head L(0), so recovery fails. Moreover tensoring the injection (x)↪R with T gives T/xT→xT, with nonzero kernel ker⁡x/xT≅L(0). Thus π∗ is not exact. All modules lie in this fixed regular block and retain its scalar gl2 centre.

4.1F2step 1.1algebra∎

Assembly. Since the charges decompose T into finitely many central components in each degree and the categories are locally unital in the infinite case, the functors πα assemble to the locally unital sum; the ambient category retains all labels, including those killed by the functors.

Remarks

  • The opposite convention in Bα=End⁡(Tα)op is fixed so that the Schur functor lands in left modules and the composition of endomorphisms is read left-to-right; this convention is used by every later item of the pair.

  • The two-term copresentations of the exactness theorem show that every projective has a copresentation by objects of add⁡(T), but a copresentation does not imply recovery by the left adjoint: the left adjoint is only right exact.

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Stable range and block idempotent corner for higher-level Schur-Weyl duality

Definition

Assume the Axiom of Choice. Keep a nonempty pyramid λ=(0≤p1≤⋯≤pn) with l=pn>0 columns of heights q1≥⋯≥ql, the origin c, and Ud=Vc⊗d of The deformed tensor space for the type-A finite W-algebra. The stable range is ql≥d: there are at least d rows of maximum length l. Put aj=cj+qj−n, Ad=im⁡(W(λ)→End⁡Ud) and Bd=im⁡(Hd(a)→End⁡Udop).

For every complex origin the finite image algebras are mutual centralizers, and the raw Hecke action is faithful in the stable range. For an admissible origin, meaning cj−ck∈Z implies cj=ck, the following construction defines the central support outside that range. Append t full ground rows of length l until ql+t≥d, keeping l and c fixed. Then n and every qj increase by t, so every aj stays fixed. In the enlarged tensor space Udbig, let e be the projection onto tensors using only retained rows, equivalently having zero occupancy in every deleted row. A large tableau is contractible if every deleted-row entry is the ground entry cj+1−r in row r and column j. The supporting central idempotent f acts as one on precisely the contractible standard-labelled simples and as zero on the others. Through the faithful enlarged Hecke action it is a central idempotent of Hd(a), and Bd≅fHd(a)f,ker⁡ψd=(1−f)Hd(a).

This f is a sum of entire supporting central blocks. Individual residue idempotents e(i) need not be central; they do not individually define this two-sided corner. The unrestricted tensor model does not by itself supply the admissible central-support conclusion.

For the empty pyramid l=N=0, the convention is separate: in degree zero the tensor and image algebras are C with the identity corner f=1; in positive degree the tensor, image algebras and their module categories are zero and f=0. No ql or nonempty stable-range condition is used in that case.

Facts & Assumptions

Given: The actual tensor actions, the small and enlarged pyramids, and their finite image algebras.

[F1]

The actual right tensor matrices, independent filtered double centralizer, stable injectivity and admissible finite-image projectivity are supplied by The deformed tensor space for the type-A finite W-algebra, The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer and Vust's graded double centralizer for the type-A nilpotent centralizer.

[F2]

The genuine original-head standard/simple comparison identifies V(A) as the head-normalized inducing Levi module, with scalar central character given by the content θ(A); a standard-labelled V(A) has unique simple quotient LW(A) by the essential-projective-head and genuine finite-W Morita argument in step 9.1 of The Whittaker functor is exact and fully faithful on the required projectives, and these are the distinct exhaustive finite-image simples. Its original path and Gauss generators are those of The Whittaker functor from the relevant parabolic category-O summand and The shifted Yangian and the pyramid generators of the type-A finite W-algebra.

Proof

technique · direct

Given: Ubig, U, the retained-box embedding i↦i^, and admissible c for the central-support claims.

1.1F1constructalgebra

The retained projection is an actual left-image idempotent. The matrix e=∑i∈IdEi^,i^ commutes with the right xk and sk: left-neighbour moves, place swaps and scalar terms preserve the row multiset, so none changes zero deleted-row occupancy. Thus e∈Adbig by the independent first centralizer. Every term of the right tensor formula restricts identically under vi↦vi^, because row and column positions and left neighbours agree and cj+(qj+t)−(n+t)=aj. This proves the actual right-bimodule identification eUbig=U and a surjective restriction map ρ:Bdbig→Bd. Extending a commuting operator on eUbig by zero on (1−e)Ubig shows Ad=eAdbige. No Morita conclusion is used.

2.1F1F2step 1.1constructalgebra

The standard contraction has the same corner action. In column j the finite Levi module is Ccj⊗Sμ(j)(Cqj+t), with μ(j) the partition of the ground differences. The zero-occupancy part is Ccj⊗Sμ(j)(Cqj), by the tensor Young-symmetrizer realization; it is zero precisely when a removed-row partition entry is nonzero. For the original Tij;0(r) path sum, every summand is a product of matrix units with strictly increasing join columns. Levi projection kills strict off-column matrix factors, leaving at most one factor in each column. A deleted intermediate row causes an off-diagonal crossing in a column whose removed-coordinate occupancy then cannot be restored by another factor, so zero-occupancy compression kills it. Every surviving path has only retained rows and is exactly a small path. The head shift changes by −(j−1)t in column j, while a retained box's ordinary source reading position changes by +(j−1)t. Its source highest weight Abox+k−1 therefore cancels that shift: the normalized weight is Abox+row⁡(box)−1 in both diagrams. Hence the complete retained matrix action, and then formal Gauss elimination, gives eV(A)=V(Aˉ) for contractible A, and zero otherwise, with the corner identification of step 1.1.

3.1F2F3step 2.1constructalgebra

The simple contraction and central saturation. The same projector acts on all standards: let Hr=Trr;0(1) be the row Cartan and κr=∑j:row r reaches column jcj. Its head-normalized action on a degree-d Levi standard has Hr−κr equal to polynomial row occupancy with eigenvalues 0,…,d. Hence e=∏r deleted∏h=1d(1−(Hr−κr)/h) is exactly zero removed-row occupancy on every standard and equals step 1.1's image idempotent; for d=0 the inner product is one. Exactness of e(−) and step 2.1 therefore kill every noncontractible simple. For a surviving big simple L, each nonzero v∈eL generates eL=eAdbigev, so eL is simple. Conversely for a corner simple S, every proper submodule of Adbige⊗eAdbigeS is killed by e: one with image S generates that whole induced module. The sum of proper submodules is thus proper and is its unique maximal submodule. Its simple quotient has e-image S. This proves a bijection between corner simples and surviving big simples without a Morita assumption. Every small standard tableau extends uniquely by full ground rows to a contractible large standard tableau. The complete Std simple lists in F2 and the corner of step 1.1 show that the survivor subset has the same finite cardinality as all contractible Std labels, so every contractible simple survives. Its simple image is a quotient of eV(A)=V(Aˉ), whose already proved unique head gives eLW(A)=LW(Aˉ). If θ(B)=θ(A) and A is contractible, separate the charge cosets. Admissibility makes all charges in one coset equal. The minimal bottom entry cj+1−(n+t) occurs once in every column of that coset; strictness and nonnegative ground differences force these occurrences into the same bottom row of B. Remove that row and repeat for all deleted rows. Then B is contractible. Scalar central characters therefore separate contractible from noncontractible simples, so generalized central-character decomposition gives a central idempotent f∈Adbig with exactly that support. Since e kills all complementary simples, e(1−f)=0: a nonzero idempotent acts nontrivially on some simple of a finite algebra. Hence e=ef=fe.

4.1F3step 3.1constructalgebra

Fullness and the supported module equivalence. Set Af=fAdbigf. Every simple Af-module survives e. If AfeAf were proper, the nonzero finite quotient Af/AfeAf would have a simple killed by e, a contradiction. Thus write f=∑kakebk. Multiplication Afe⊗eAfeeM→M has inverse m↦∑kake⊗ebkm; the fullness identity and tensor balancing verify both composites. Also e(Afe⊗N)→N is the canonical isomorphism. These actual maps give inverse equivalences on all supported-block modules. In particular the functor e(−) is faithful on that summand, and its kernel on all large finite-image modules is exactly the complementary summand.

5.1F1step 1.1step 4.1constructalgebra

The simultaneous central corner and both kernels. The operator f commutes with Adbig, hence belongs to Bdbig by the second centralizer. It is central there because every right operator commutes with every left operator. The equivalence of step 4.1 identifies End⁡Af(fUbig)op with End⁡eAfe(eUbig)op, so the restriction of ρ is an isomorphism fBdbigf→Bd. Its kernel on Bdbig is (1−f)Bdbig. The enlarged stable action is faithful by F1, giving Bd=fHd(a)f and ker⁡ψd=(1−f)Hd(a). On the left, fUbig has annihilator (1−f)Adbig, and eUbig is faithful for its corner eAdbige; the latter need not be a module for all of Adbig. Infinite-W kernels are the inverse images of these finite-image kernels.

6.1F1step 3.1step 5.1algebra∎

The parameter boundary. Stable faithfulness and the matrix restriction of step 1.1 hold for every complex origin. Central saturation in step 3.1 used admissibility, so the supporting-block and faithful-equivalence assertions are made only there. The supporting idempotent is a sum of whole central blocks; individual residue idempotents are not thereby made central. All row additions keep l fixed and add full rows, preserving cj+qj−n exactly.

Remarks

The equivalence above is between the supported finite-image summand and the retained finite-image corner. If the enlarged tensor module is a progenerator, this explicit equivalence transports its supported part to the small tensor progenerator. Ground and ordinary-dual adjunction proofs establish that hypothesis in the admissible double-centralizer supplier; the corner proof does not assume its own Morita conclusion.

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Hecke induction and restriction functors on degenerate cyclotomic blocks

Definition

Assume inherited AC The Axiom of Choice for the invoked cyclotomic PBW supplier. Fix a multiset of complex roots a=(a1,…,al) with l≥1, allowing repeated roots. Write B=Hd(a) and A=Hd+1(a) for The degenerate cyclotomic Hecke algebra. The generator-preserving tower map embeds B in A.

For every generalized eigenvalue i of xd+1 in the regular representation of A, let ui∈C[xd+1] be its polynomial generalized-eigenspace projector. All such eigenvalues lie in ⋃j(aj+Z). These are additive residue chains, separately indexed in each coset of C/Z; coincident roots do not give extra projectors. The ui are mutually orthogonal, sum to one, commute with B and satisfy ui∗=ui. They need not be central in A.

For finite-dimensional left modules define the residue functors ei(M)=uiM,fi(N)=Aui⊗BN. Here the first functor takes its B-action from the tower inclusion and the second takes its A-action from the first factor. They are exact and biadjoint and commute naturally with the generator-fixing ∗-duality. Consequently they preserve projectives and induce adjoint operators for the projective/module Hom pairing. Projecting further by source and target content idempotents gives the supported-block functors. Neither primitivity of a central content projector nor equality B=uiAui is needed or asserted here. Actual image towers in admissible stable realizations use the compatible projected tensor actions of Stable range and block idempotent corner for higher-level Schur-Weyl duality.

For level zero use H0(∅)=C and Hd(∅)=0 for d>0. The map H0→H1 is the zero homomorphism C→0, so it is not an embedding. Every positive-degree residue induction and restriction functor is zero; all biadjunction and exactness assertions then hold for zero functors.

Facts & Assumptions

Given: The roots a with l≥1, the algebras B=Hd(a) and A=Hd+1(a), finite-dimensional left modules, and inherited AC for the PBW supplier. We prove the nonzero-level assertions and then the level-zero convention.

[F1]

The bounded PBW basis, polynomial-degree filtration and associated graded algebra are gr⁡Hn=C[X1,…,Xn]/(X1l,…,Xnl)⋊C[Sn]. The generator-fixing anti-involution ∗ and the nondegenerate symmetric trace τn given by the coefficient of x1l−1⋯xnl−1⋅1 are supplied by The degenerate cyclotomic Hecke algebra. These hold for every complex root multiset, including repeated roots.

[F2]

Finite Chinese remainder interpolation gives the generalized-eigenspace polynomial projectors for a finite-dimensional operator (Chinese remainder theorem for pairwise comaximal ideals).

Proof

technique · direct
1.1F1givenconstructalgebra

The tower map and both finite free structures. The first d dot and crossing generators in A satisfy the relations of B, including the same cyclotomic polynomial in x1. Their bounded PBW words are a subset of the bounded basis of A, so the generator-preserving homomorphism is injective. Let wt=st⋯sd for 1≤t≤d and wd+1=1; these are the minimal right Sd coset representatives in Sd+1, with wt(d+1)=t. The elements wtxd+1r, 0≤r<l, form a right B-basis of A. Indeed multiply them by the bounded PBW basis of B. In the associated graded algebra their symbols are the distinct bounded words obtained by permuting the first d dot exponents by wt and placing exponent r in the omitted position t, with permutation wtv, v∈Sd. These run over exactly all bounded words of gr⁡A, so filtered leading-degree induction proves that the products form a basis of A. Applying ∗ gives the left B-basis ηt,r=xd+1rwt−1. Thus both ranks are l(d+1), and this is valid without any separation of roots.

2.1F1step 1.1constructalgebra

An actual relative Frobenius trace. Use the two symmetric traces to define t:A→B uniquely by τd(bt(a))=τd+1(ba) for every b∈B. Nondegeneracy of τd proves existence and uniqueness. Cyclicity of both traces gives t(b1ab2)=b1t(a)b2, so t is a B-bimodule map. The map Φ:A→Hom⁡B(BA,BB), Φ(a)(c)=t(ca), is an (A,B)-bimodule isomorphism, where the left action on Hom is (a⋅h)(c)=h(ca) and its right action is multiplication on the output. To see invertibility directly, h↦τd∘h identifies this Hom space with DCA: given λ∈DCA, define h(c) by τd(bh(c))=λ(bc), which is uniquely determined and B-linear. The symmetric A-trace identifies A with DCA by a↦[c↦τd+1(ca)]. Their composite is precisely Φ, including both bimodule actions. This proves the Frobenius extension identity using the two traces and the actual finite extension, rather than assuming tensor products commute with linear duality.

2.2F1F2step 1.1constructalgebra

The projectors and residue chains. For each regular-spectrum eigenvalue i of xd+1, apply [F2] to its annihilating polynomial to obtain ui∈C[xd+1]. Since the regular representation is faithful and every finite module is a quotient of a finite free module, these projectors act as the generalized-eigenspace projectors on every module. Cross relations show xd+1 commutes with B, so ui centralizes B and is fixed by ∗. Their products and sum give the stated orthogonality and identity. For the root-coset claim use joint dot projectors and ϕr=sr(xr−xr+1)+1, which satisfies ϕr2=1−(xr−xr+1)2 and swaps the adjacent dot operators. On a weight with adjacent entries differing by neither 1 nor −1, this square is invertible by a finite nilpotent geometric series. A leftmost eigenvalue outside ⋃j(aj+Z) can therefore be moved past all preceding entries in that union, since its differences from them are not integers; this produces a nonzero first-position eigenvalue contradicting the cyclotomic relation. Thus every eigenvalue lies on one of the specified coset chains. No orbit-sum primitivity is used.

3.1step 1.1step 2.1constructalgebra

Induction equals coinduction, with explicit inverse. Index the left basis ηs from step 1.1 by s=(t,r) and let ps:A→B be its left-coordinate maps, so c=∑sps(c)ηs. Put as=Φ−1ps. Then t(ηsas′)=δss′ and c=∑st(cas)ηs. Finite freeness makes the natural map Hom⁡B(A,B)⊗BN→Hom⁡B(A,N) an isomorphism: it sends h⊗n to [c↦h(c)n] and its inverse sends g to ∑sps⊗g(ηs). Composing with Φ gives the natural A-module isomorphism A⊗BN≅Hom⁡B(BA,N), a⊗n↦[c↦t(ca)n], with inverse g↦∑sas⊗g(ηs). Consequently induction is both left and right adjoint to ordinary restriction. It is exact by the right freeness in step 1.1, independently of any duality argument.

4.1step 1.1step 2.1step 3.1step 2.2constructalgebra

The residue Frobenius isomorphism and two adjunctions. Write u=ui. For every c∈A, one has t(uc)=t(cu): pairing either side with b∈B under τd gives τd+1(buc)=τd+1(bcu) by bu=ub and trace cyclicity. Hence right multiplication by u on A corresponds under Φ to precomposition by left multiplication by u. Restricting the isomorphism of step 3.1 therefore gives Au⊗BN≅Hom⁡B(BuA,N) as left A-modules, with the same explicit relative-trace formula on uA. The usual tensor-Hom adjunction gives Hom⁡A(Au⊗BN,M)≅Hom⁡B(N,uM), and the usual restriction-coinduction adjunction gives Hom⁡B(uM,N)≅Hom⁡A(M,Hom⁡B(uA,N)). Together these prove fi⊣ei⊣fi. The functor ei is exact as an idempotent summand of restriction; Au is a right-B direct summand of the free module A, so fi is exact. The units and counits are the tensor-Hom evaluation maps and the relative-trace/dual-basis coinduction maps just constructed, not maps inferred from an abstract symmetry of two algebras.

5.1step 3.1step 2.2step 4.1constructalgebra

The correct dual tensor comparison. For a left A-module X write DAX=Hom⁡C(X,C) with action twisted by ∗, and write DBN for the same construction on the left B-module N. The actual natural isomorphism is DA(A⊗BN)≅Hom⁡B(BA,DBN). It sends a linear functional λ to [c↦(n↦λ(c∗⊗n))], with inverse h↦[a⊗n↦h(a∗)(n)]. The balancing relation and ∗ show B-linearity and A-linearity directly. Composing its inverse with the genuine induction/coinduction isomorphism of step 3.1 gives A⊗BDBN≅DA(A⊗BN). The same formulas for the summands give DA(Au⊗BN)≅Hom⁡B(uA,DBN)≅Au⊗BDBN, since u∗=u and step 4.1 applies. Restriction similarly gives uDAM≅DB(uM) by restricting functionals, with inverse extending by zero on (1−u)M. Thus each residue functor commutes with ordinary ∗-duality. This proof does not identify Au with its linear dual as an unqualified bimodule.

6.1step 4.1step 5.1constructalgebra

Projectives and Grothendieck operators. Exact biadjunction proves projective preservation: for projective P, Hom⁡A(fiP,−)≅Hom⁡B(P,ei−) is exact, and Hom⁡B(eiQ,−)≅Hom⁡A(Q,fi−) is exact for projective Q. The Hom pairing descends to split K0 of projectives and G0 of finite-dimensional modules, because Hom is additive on projective direct sums and exact in its second variable. The two adjunctions compute ⟨[fiP],[M]⟩=⟨[P],[eiM]⟩ and ⟨[eiQ],[N]⟩=⟨[Q],[fiN]⟩. Exactness makes all operators well defined on these groups. Central source/target projections restrict the bimodules, adjunctions and duality comparisons to supported content summands; no primitivity premise is required for those restrictions.

7.1F1step 1.1step 2.2step 4.1step 5.1step 6.1given∎

Boundaries and level zero. The entire proof used only the actual bounded PBW extension and its two symmetric traces, so it applies to all complex roots and their repetitions. The realization assertion invokes only the actual admissible projected tensor actions of the named stable-range supplier, not a block-primitivity assertion. For l=0 the empty cyclotomic polynomial is 1, so every positive-degree algebra is zero; the map C→0 is explicitly noninjective, all positive-degree functors are zero, and their exactness and adjunctions are the unique zero-functor ones. Together with steps 1.1–5.1 this proves every asserted boundary and functor property.

Remarks

The Frobenius extension is a relative statement: it uses finite left/right freeness and the two nondegenerate symmetric traces to construct Hom⁡B(A,B)≅A. Symmetry of A alone neither gives the residue bimodule Au an unqualified self-duality nor turns linear duals of tensor products into tensor products. Repeated roots use the same generalized-eigenvalue projectors and require no change to the proof.

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The higher-level Schur-Weyl endomorphism isomorphism

Statement

Assume the Axiom of Choice. Let λ be a pyramid with columns q1≥⋯≥ql, let c be an admissible origin, let Pc be the ground simple projective-injective of the relevant summand of the parabolic category O of The integral parabolic category-O blocks for higher-level Schur-Weyl duality, and let T=Pc⊗V⊗d with V=CN. Write Bd=ψd(Hd(Λ)) for the image of the right cyclotomic Hecke action of The degenerate cyclotomic Hecke algebra and Bα for its central components. Then the right Hecke action gives an algebra isomorphism End⁡g(T)op=Bd, and on each central component, cut by the central idempotents fα of Bd acting on T=⨁αTα, End⁡g(Tα)op=Bα=fαHα(a)fα, where Hα(a) is the corresponding block of the cyclotomic Hecke algebra. For a nonempty pyramid, in the stable range ql≥d the image is the full cyclotomic algebra, Bd=Hd(a) and Bα=Hα(a); a single component is not identified with the entire degree-d algebra. Outside the stable range the central-corner identification uses the admissible-origin corner of Stable range and block idempotent corner for higher-level Schur-Weyl duality. The maps Hd(a)↠Bd are surjective in all cases, and the full action Hd(a)→End⁡(Vc⊗d) is injective precisely when ql≥d for a nonempty pyramid. For the empty pyramid l=N=0, the degree-zero objects and algebras are T0=U0=H0=C, and for d>0 they are Td=Ud=Hd=0. All endomorphism identities hold there, and the raw action is faithful in every degree, including the zero-algebra action; ql is not defined in this branch.

Facts & Assumptions

Given: The pyramid λ, an admissible origin c, the ground object Pc, the tensor object T=Pc⊗V⊗d with its central decomposition, and the Hecke image Bd.

[F1]

The right Hecke action on T exists and its generators xj,si are natural endomorphisms of the tensor functor, commuting with g; the image is Bd=ψd(Hd(Λ)), and the Whittaker functor sends T to Vc⊗d (Arakawa-Suzuki Casimir operators on tensor functors, The degenerate cyclotomic Hecke algebra, The higher-level Schur-Weyl projective generator and Schur functor).

[F2]

The Whittaker functor is exact on Ocd, its kernel is the Serre subcategory generated by the off-standard simples, T is a self-dual prinjective detector whose simple socle constituents are standard-labelled and whose indecomposable summands are precisely the standard-labelled projective-injective covers, each occurring with positive multiplicity, and V(T)=Vc⊗d (The Whittaker functor is exact and fully faithful on the required projectives, The higher-level Schur-Weyl projective generator and Schur functor).

[F3]

The filtered double centralizer identifies the two image algebras on Vc⊗d for every complex origin: Wd and Bd are mutual centralizers, and in particular End⁡Wd(Vc⊗d)op=Bd; for a nonempty pyramid, if ql≥d the full action of Hd(a) is faithful (The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer).

[F4]

Outside the stable range the image of the Hecke action is a central block corner fHd(a)f for admissible origins, and in the stable range Bd=Hd(a) (Stable range and block idempotent corner for higher-level Schur-Weyl duality).

Proof

technique · direct

Given: The objects Pc, T, the Hecke image Bd⊆End⁡C(T)op, and the admissible-origin hypotheses.

1.1F1algebra

The Hecke action lies in the g-endomorphisms. For the empty pyramid, the empty tensor in degree zero and its ground object give T0=U0=H0=C. In positive degree V=0 gives Td=Ud=0, and the level-zero cyclotomic relation is the empty product 1, so Hd=0. The stated endomorphism identities and faithfulness follow directly, with the unique zero-algebra map injective; the remaining argument assumes a nonempty pyramid. Each generator xj of the truncated tensor action is built from the trace Casimir and place permutations and commutes with the diagonal g-action; the place permutations are natural in the module variable, so the resulting right Hd(a)-action on T consists of g-endomorphisms, and its image is Bd by definition. Hence there is a surjection Hd(a)↠Bd and an inclusion Bd⊆End⁡g(T)op, with the opposite convention fixed by the right action.

1.2F2algebra

The Whittaker comparison is injective. Let φ:T→T be nonzero and put X=im⁡φ, a nonzero submodule of the finite-length object T. Choose a simple submodule L(A)⊆X; because soc⁡X⊆soc⁡T, [F2] gives A∈Std. Exactness gives an injection V(L(A))↪V(X), and the first module is nonzero, so V(X)≠0. Exactness also identifies V(X) with the image of V(φ), hence V(φ)≠0. This proves injectivity of End⁡g(T)op→End⁡Wd(Vc⊗d)op. No restriction on all composition factors of T is used.

2.1F1F3step 1.2algebra

The image of the comparison. On V(T)=Vc⊗d the induced map lands in the centralizer of the finite-W action, End⁡Wd(Vc⊗d)op; by the filtered double centralizer [F3] this centralizer equals Bd; and the induced map contains Bd because every Hecke generator on Vc⊗d arises from the corresponding endomorphism of T by [F1]. Since Bd is the whole target, the injective map of step 1.2 is also surjective, so End⁡g(T)op=Bd.

2.2F3F4step 1.1algebra

Stable range. For a nonempty pyramid, if ql≥d then the action of Hd(a) is faithful by [F3] and the image is the full algebra Bd=Hd(a); a single central component is correspondingly a block Hα(a), not the whole algebra. Outside the stable range the corner identification of [F4] applies for admissible origins, while the map Hd(a)↠Bd remains surjective by step 1.1.

3.1F4step 2.1algebra

Central components. The central idempotents fα of the finite-dimensional algebra Bd decompose T=⨁αTα and Bd=⨁αBα; applying the isomorphism of step 2.1 componentwise gives End⁡g(Tα)op=fαBdfα=Bα. The component Bα sits inside the cyclotomic block as the corner fαHα(a)fα by [F4]; it is not the entire degree-d algebra.

4.1F2F4step 2.2constructalgebra∎

Failure of raw faithfulness below the stable range. For a nonempty pyramid, suppose d>ql and use an enlargement by full ground rows with smallest height at least d. In its last column, raise the first ql+1 entries above their ground values by 1; raise its top entry further by d−ql−1, and leave every other entry ground. This is column strict, has total degree d, and is standard: for columns with the same charge, the changed rightmost entry is at least every unchanged entry to its left in that row; different charge cosets are incomparable. The first ql rows of this column are retained, but its next row is deleted, so this standard label is noncontractible. Its nonzero large finite-W simple belongs to a complementary central block. Hence the supporting idempotent f of [F4] is proper; the faithful large tensor progenerator makes 1−f nonzero also in the large Hecke algebra. The small raw action has the nonzero kernel (1−f)Hd(a) and is not faithful. Together with step 2.2 this proves the asserted precise stable-range criterion.

Remarks

  • The key point is that the Whittaker functor is faithful on endomorphisms of T although it is not faithful on the whole category: every nonzero image has a standard composition factor, and the kernel consists precisely of the off-standard simples.

  • The opposite algebra convention in End⁡g(T)op is the one fixed in The higher-level Schur-Weyl projective generator and Schur functor: the right Hecke action composed left-to-right matches the left action of Bα on the modules of the Schur functor.

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The higher-level Schur-Weyl double centralizer and Schur quotient

Statement

Assume the Axiom of Choice. Fix the pyramid λ with columns q1≥⋯≥ql, an origin c, a degree d≥0, and let Vc⊗d be the truncated tensor space with its finite W-algebra image Wd and cyclotomic Hecke image Bd. Then:

  1. Wd and Bd are mutual centralizers on Vc⊗d, for every complex origin c; this is the raw double centralizer.
  2. For admissible origins, Vc⊗d is a progenerator and Hom⁡Wd(Vc⊗d,−) is a Morita equivalence between Wd-mod and Bd-mod.
  3. The genuine Whittaker functor followed by this equivalence is the exact Schur Serre quotient killing exactly the off-standard simples; it is fully faithful on all projectives of the relevant parabolic summand and on all tiltings, and its left adjoint is right exact and recovers add⁡(T) but need not recover every projective.
  4. For a nonempty pyramid, in the stable range ql≥d the algebra Bd is the full cyclotomic algebra Hd(a); outside the stable range and for admissible origins the central-corner identification Bd=fHd(a)f is used.

Mutual centralizers alone do not give the Morita statement: the nonadmissible origin example with c=(0,1), q=(1,1) and d=2 has a nonprojective tensor module while the mutual centralizer identities still hold.

Facts & Assumptions

Given: The pyramid, the origin c, the tensor space Vc⊗d, the image algebras Wd, Bd, and the tensor object T=Pc⊗V⊗d of the relevant parabolic summand.

[F1]

The raw filtered double centralizer holds for every complex origin; for admissible origins the tensor space is a progenerator and Hom⁡Wd(Vc⊗d,−) is a Morita equivalence Wd-mod→Bd-mod; the nonadmissible counterexample with c=(0,1), q=(1,1), d=2 separates the two assertions (The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer).

[F2]

End⁡g(T)op=Bd and, componentwise, End⁡g(Tα)op=Bα for admissible origins; the map Hd(a)↠Bd is surjective with injectivity exactly in the nonempty stable range and also in the trivial empty branch (The higher-level Schur-Weyl endomorphism isomorphism).

[F3]

The Whittaker quotient π=Hom⁡g(T,−) is exact, its kernel is the Serre subcategory of off-standard simples, it is fully faithful on all projectives and on tiltings, its left adjoint π∗=T⊗Bd− is right exact, and π∗π recovers add⁡(T) but need not recover every projective of the ambient category (The higher-level Schur-Weyl projective generator and Schur functor, The Whittaker functor is exact and fully faithful on the required projectives).

[F4]

The stable range is ql≥d; in it Bd=Hd(a), and outside it the admissible-origin image is the central block corner fHd(a)f (Stable range and block idempotent corner for higher-level Schur-Weyl duality, The degenerate cyclotomic Hecke algebra).

Proof

technique · direct

Given: The mutual centralizer and Morita inputs of [F1], the endomorphism isomorphism of [F2], the Schur quotient properties of [F3], and the stable-range/corner dictionary of [F4].

1.1F1algebra

The raw double centralizer. For arbitrary complex origin the filtered leading-symbol lifting argument of [F1] gives Wd=Bd′ and Bd=Wd′ on Vc⊗d, with associated graded images the Vust centralizers; this is the all-origin clause and does not use admissibility.

1.2F1F2algebra

Admissible Morita equivalence. Assume c admissible. By the progenerator clause of [F1], Vc⊗d is a progenerator for Wd and Hom⁡Wd(Vc⊗d,−) is a Morita equivalence; by the component clause of [F2] its endomorphism algebra is Bd=End⁡Wd(Vc⊗d)op, so the equivalence is the standard one attached to the (Wd,Bd)-bimodule Vc⊗d, identifying Wd-mod with Bd-mod.

2.1F2F3step 1.2algebra

The Schur Serre quotient. The composite of the genuine Whittaker functor with the equivalence of step 1.2 is π=Hom⁡g(T,−) by [F2] and [F3]; it is exact and its kernel is the Serre subcategory generated by the off-standard simples, so it is the exact Schur Serre quotient killing exactly those simples.

3.1F3step 2.1given

Full faithfulness and the left adjoint. By [F3] the quotient is fully faithful on all projectives of the relevant parabolic summand and on all tiltings, while its left adjoint T⊗Bd− is only right exact and π∗π recovers add⁡(T) but need not recover every projective; these boundaries are part of the statement and are not repaired by changing conventions.

4.1F2F4step 1.1algebra∎

Stable range and central corner. For the empty pyramid degree zero is the scalar identity and positive degree is the zero-algebra identity, so all comparisons hold directly with f=1 in degree zero and f=0 in positive degree. For a nonempty pyramid, if ql≥d then Bd=Hd(a) by [F4] and the component form of step 2.1 uses the full cyclotomic algebra; outside the stable range, and for admissible origins, the image is the central block corner Bd=fHd(a)f of [F4], with the component corners Bα=fαHα(a)fα of [F2]. For nonadmissible origins only the raw mutual centralizer statement of step 1.1 remains.

Remarks

  • The statement separates three levels of structure that are often conflated: the all-origin mutual centralizer (step 1.1), the admissible-origin Morita equivalence (step 1.2), and the stable-range simplification Bd=Hd(a) (step 4.1). Each consumes a different supplier.
  • The left adjoint π∗ is used only where it is exact enough: recovering add⁡(T) on standard-labelled prinjectives, never for arbitrary projectives.
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Schur functor images of standard, simple, projective and tilting objects

Statement

Assume the Axiom of Choice and fix an admissible origin c. Let π=Hom⁡g(T,−) be the Schur functor of The higher-level Schur-Weyl projective generator and Schur functor, T=Pc⊗V⊗d. Use the current category-O namespace: N(A):=M(A) is the generalized standard, K(A):=∇(A) the costandard, L(A) the category-O simple and P(A) its projective cover, as in The integral parabolic category-O blocks for higher-level Schur-Weyl duality. The source17 symbol K(A) denotes our L(A), not our costandard K(A). Let V ⁣Wh denote the genuine continuous-dual functor of The Whittaker functor from the relevant parabolic category-O summand, and write L(A):=V ⁣Wh(L(A)) for the finite-W image of the category-O simple; for A∈Std this is the source finite-W simple appearing in the Whittaker/Morita contract of The Whittaker functor is exact and fully faithful on the required projectives. In particular the Wd-Hom below takes a finite-W module as its second argument. Let Std be the standard labels. Then:

  1. For every label A, the Schur image of the standard object N(A) is the intrinsic affine-induced Specht module S(A)=Hd⊗Hd1,…,dl(⨂jevaj∗Sμ(j)),aj=cj+qj−n, where μ(j) is the partition of dj read from the nonnegative ground differences in the j-th column of A and the factors are induced along the affine Young subalgebra Hd1,…,dl=Hd1⊗⋯⊗Hdl. Its affine action factors through the cyclotomic image Bd, so the same module is obtained by replacing Hd in this tensor product by Hd(a).
  2. For A∈Std the module D(A)=π(L(A))≅Hom⁡Wd(Vc⊗d,L(A)) is simple, the modules D(A), A∈Std, form a complete set of pairwise non-isomorphic simples of the Hecke image Bd, and π(L(A))=0 for A∉Std.
  3. For A∈Std, π(P(A)) is the projective cover Y(A) of D(A), and π∗π(P(A))≅P(A); ambient off-standard projectives still have their genuine images, and no projective-preservation assertion is made for them.
  4. Images of tiltings carry the opposite-parabolic standard/Specht flag coefficients, and π is fully faithful on tiltings.
  5. For A∈Col and B∈Std, [S(A):D(B)]=[N(A):L(B)]=dB,A(1), where dB,A is the typed canonical-basis coefficient of the Fock-space dictionary; for B∉Std the symbol D(B) is not a Hecke simple. All interfaces are ungraded at parameter 1.

Facts & Assumptions

Given: The admissible origin c, the tensor object T=Pc⊗V⊗d, the Schur functor π, the standard and costandard objects N(A),K(A), the simples L(A), the projectives P(A), and the Hecke image Bd.

[F1]

In the actual category-O namespace the generalized standards are M(A)=N(A), the simples are L(A), projective covers are P(A) and costandards are ∇(A)=K(A). These have the BGG reciprocity and standard/costandard/tilting flags of The integral parabolic category-O blocks for higher-level Schur-Weyl duality, Standard- and costandard-filtered objects and tilting objects and Indecomposable tilting objects exist and are classified in parabolic category O. Composition multiplicities below are always taken against the simple L(B); they are not standard-flag multiplicities against a costandard.

[F2]

The Schur functor π is exact, kills exactly the off-standard simples, recovers add⁡(T) under π∗π, and is fully faithful on all projectives and on all tiltings; T contains every standard-labelled projective-injective cover (The higher-level Schur-Weyl projective generator and Schur functor, The Whittaker functor is exact and fully faithful on the required projectives).

[F3]

The filtered double centralizer identifies Bd=End⁡Wd(Vc⊗d)op, and the Schur quotient is the composite of the genuine Whittaker functor with the Morita equivalence; the stable range gives Bd=Hd(a) (The higher-level Schur-Weyl double centralizer and Schur quotient, The higher-level Schur-Weyl endomorphism isomorphism, The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer, Stable range and block idempotent corner for higher-level Schur-Weyl duality).

[F4]

The Fock-space dictionary: the canonical, dual-canonical and quasi-canonical bases of the higher-level Fock module carry the typed labels of simples, projectives and tiltings of the summand, and the coefficient dB,A(1) computes the corresponding multiplicity at parameter 1 (The dual-canonical, canonical and quasi-canonical Fock bases, Simples, projectives and tiltings map to the three distinguished Fock bases).

[F5]

The cyclotomic Hecke algebra has the bounded monomial basis and the affine evaluation homomorphisms eva ⁣:Hdj→C[Sdj], xk↦a+∑h<k(h,k) (The degenerate cyclotomic Hecke algebra).

[F6]

For each finite-dimensional complex column space Ej, classical Schur–Weyl duality identifies its polynomial highest-weight multiplicity spaces with the ordinary Specht modules, with the length cutoff ℓ(μ)≤dim⁡Ej (The Schur-Weyl mutual centralizer theorem on tensor powers, Schur-Weyl decomposition and highest weights). Cancelling the common origin character leaves the same intertwiners. The row symmetrizer in Ej⊗dj realizes the corresponding product of symmetric powers; its Young-symmetrizer quotient has the Specht fibre.

Proof

technique · direct

Given: The standard N(A), the costandard K(A), the labels of Std, and the corner data of the stable realization. For the empty pyramid, degree zero has the sole empty label and all its modules and functors are C and the identity; positive degree has no labels and only zero modules. The assertions follow directly there, and the following construction treats a nonempty pyramid.

1.1F3F5constructalgebra

A regular corner in the stable realization. Add full ground rows until there are d distinct rows of length l, and choose one rightmost box in each such row; let vS be their ordered tensor and eS the row-weight projection onto tensors using these rows once each. The actual tensor matrices in [F3] preserve row multisets, so this projection commutes with the right Hecke action and belongs to the left image by the first centralizer. The vectors vSx1r1⋯xdrdw, 0≤ri<l, w∈Sd, have distinct leading tensors: the leading dot moves its box one column left, while a permutation changes the ordered distinct rows. They therefore form a basis of eSU by triangularity, and its cardinality is ldd!. Thus b↦vSb identifies eSU with the right regular Hd(a)-module. Put A=End⁡Hd(a)U. Since eSU is regular, AeS=Hom⁡Hd(eSU,U)≅U by evaluation at vS. Consequently h:Hd(a)→eSAeS, characterized by h(b)vS=vSb, is an algebra isomorphism, and θ↦θ(vS) identifies Hom⁡A(U,M) with eSM for every finite-image module M. The left Hecke action on this corner is h, not the naive right action on M.

2.1F1F3F5step 1.1constructalgebra

The cyclic symmetric generator and its bottom quotient. Write A−Ac=(m1,…,mN), retaining aj=cj+qj−n exclusively for the cyclotomic roots, and form the actual cumulative-column p-module Z=⨂iSym⁡mi(V≤col⁡(i)). Its bottom column degree is b=∑imi(l−col⁡(i)); the higher-degree part is a p-submodule, and Z/Z>b is the inflated Levi module Zb=⨂j⨂rSym⁡μr(j)(Ej). Put wA=∑w∈∏iSmiw and xA=∏i∏k=1mi∏j>col⁡(i)(xm1+⋯+mi−1+k−aj). Apply these commuting factors one tensor place at a time, starting with the first place, and within each place in descending column order j=l,l−1,…,col⁡(i)+1. The actual dot formula gives vSxA=vj, where j has the ordered rows of vS and column sequence prescribed by A−Ac; subtracting aj cancels the scalar at column j and moves that box one column left. Hence vSxAwA=vjwA∈eSZ. More generally the vectors vSwx1r1⋯xdrdxAwA, with 0≤rk<col⁡(jk) and w ranging over cosets of ∏iSmi, have distinct leading symmetrized tensors and span eSZ by the ordinary symmetric-tensor basis. Thus this vector generates eSZ as a corner module, and its image generates eS(Z/Z>b). These are actual vector identities and triangular basis statements, rather than a character identification.

3.1F3F5F6step 1.1step 2.1constructalgebra

The affine colour fibre. Ordinary Levi Schur-Weyl gives Hom⁡h(U,Zb)≅⨂jMμ(j) on the canonical colour fibre, where Mμ is the symmetric-group permutation module. Its vectors in the corner are vjwwA+eSZ>b with w∈Sd1×⋯×Sdl. For k=d1+⋯+dj−1+1, the identity vj=vSxA and commutativity of dots give h(xk)vjwwA=vSxAxkwwA=vjxkwwA. In the bottom quotient the dot formula has scalar aj=cj+qj−n: its left-neighbour term has higher degree, all preceding places have strictly smaller column and all later places have greater or equal column, so both signed transposition sums are empty. Thus xk acts as aj on that canonical fibre. The affine cross relations then determine the remaining dots as aj plus their within-block Jucys-Murphy sums. This proves that the fibre inclusion is a homomorphism for the affine Young subalgebra Hd1⊗⋯⊗Hdl, with module ⨂jevaj∗Mμ(j), and its image generates the entire corner by step 2.1.

4.1F1F2F3F5F6step 1.1step 3.1constructalgebra

The genuine Specht isomorphism. The Levi Young-symmetrizer map gives an actual quotient Zb↠V(A) and hence a p-quotient Z/Z>b↠V(A). The canonical colour fibre quotient is ⨂jSμ(j), by ordinary Levi Schur-Weyl. The affine fibre map in step 3.1 descends through this actual quotient and still generates: eS is exact and the generating vector of its source maps onto a generator of its quotient. Affine induction therefore gives a surjection S(A)↠eSV(A). The multilinear row-weight part of ⨂jSμ(j)(Ej) has one summand for each allocation of the d distinct rows into ordered colour subsets of sizes dj, and on each subset its weight space is the polytabloid Specht space. Its dimension is d!/(d1!⋯dl!)∏jdim⁡Sμ(j). This is also the induced module's dimension, since the affine algebra is free over its affine Young subalgebra with the finite shuffle basis. The existing surjection is therefore an isomorphism. Steps 1.1 and [F2] identify its target with Hom⁡Wd(U,V(A))=π(N(A)), preserving the actual Hecke maps.

5.1F3step 4.1constructalgebra

Descent to the original pyramid. Extend the original label A by the added ground rows, producing a contractible large label A+. Its column partitions μ(j) and roots aj are unchanged. The actual original-path/zero-occupancy compression in [F3] gives eV(A+)=V(A) and eU+=U, with the faithful supporting-block Morita equivalence and natural Hom comparison. Every simple constituent of V(A+) has the same entry-multiset central character as A+; the bottom-row minimum argument forces every such label to be contractible. Hence the supporting central idempotent satisfies fV(A+)=V(A+), and the Hom comparison identifies the original Hom⁡Wd(U,V(A)) with the entire large Hom module, rather than an arbitrary quotient of it. Step 4.1 therefore descends the same intrinsic Specht isomorphism to the original pyramid.

6.1F1F2F4step 5.1algebra

Tilting images and full faithfulness. The opposite-parabolic flag coefficients are the actual tilting-character coefficients of [F1] and [F4]; exact π carries each successive standard section to its Specht module by steps 4.1–5.1, so it preserves these flag multiplicities. For fullness, the local corner proof of [F2] applies: in the finite summand algebra A, π is equivalent to e(−) and has right adjoint G(X)=Hom⁡eAe(eA,X). Its unit on a target with standard socle is injective and has off-standard cokernel. A tilting has standard socle from its standard flag and standard head from its costandard flag and simple-preserving restricted duality. Any map from it to the off-standard cokernel vanishes, since a nonzero quotient would have standard head. Adjunction therefore factors every map between its Schur images uniquely through the original target, proving full faithfulness on tiltings.

6.2F1F2F3step 5.1algebra

Simple images and heads. Here L(A)=V ⁣Wh(L(A)) uses the genuine continuous-dual functor, rather than raw Whittaker vectors in L(A). The finite-W simple-image classification and the genuine Morita equivalence in [F2] and [F3] imply that D(A)=π(L(A))≅Hom⁡Wd(Vc⊗d,L(A)) is simple for A∈Std, that these are distinct and exhaustive, and that π(L(A))=0 otherwise. For a standard label A, the cover P(A) is an indecomposable summand of T, so Y(A)=π(P(A)) is an indecomposable projective. Its simple quotients are determined by Hom⁡Bd(Y(A),D(B))≅Hom⁡g(P(A),L(B)), which has dimension δA,B; this is the ordinary equivalence on add⁡(T) and the simple-image computation. Thus Y(A) has head D(A). Lift the cover P(A)→L(A) through N(A)→L(A) using projectivity; the lift is surjective since the latter is the simple-head quotient and any proper submodule of N(A) lies in its radical. Exactness yields Y(A)↠S(A)↠D(A). Every nonzero quotient of the indecomposable projective Y(A) has the same simple head D(A): its kernel is contained in the unique maximal submodule. Therefore S(A) has head D(A).

7.1F2step 6.2algebra

Projective images. For A∈Std, the preceding step shows that Y(A)=π(P(A)) is the indecomposable projective with simple head D(A), hence its projective cover. Evaluation T⊗Bdπ(P(A))→P(A) is an isomorphism because P(A)∈add⁡(T): this is checked on T and restricted to its idempotent summands. Thus π∗π(P(A))≅P(A). Off-standard projectives retain their actual images, and no projective-preservation assertion follows for them.

8.1F2F4step 6.2algebra∎

Multiplicities. Since π is exact and its kernel is generated by the off-standard simples, the composition multiplicities of S(A)=π(N(A)) are the multiplicities of the simple L(B) in N(A) for B∈Std; by the Fock-space dictionary [F4] the typed coefficient of the dual-canonical/canonical pairing equals dB,A(1), so [S(A):D(B)]=[N(A):L(B)]=dB,A(1); for B∉Std the module D(B) is zero and is not a simple Hecke label. All the identifications above are ungraded and taken at parameter 1.

Remarks

  • The intrinsic definition of S(A) by parabolic induction replaces the faulty direct Hom⁡p identification of the source with the corner/regular-vector computation: the canonical colour fibre is only one of several fibres of eSV(A), and the corner operators supply the correct extension.
  • The proof deliberately separates the stable-range corner computation (steps 1.1–5.1) from the exact-quotient consequences (steps 6.1–8.1); the latter only use exactness, the kernel description and the Fock dictionary, so they are insensitive to the choice of stable realization.
TheoremStatement: Literature-sourcedProof: AI-adaptedprecheck passOpen item page →

Category-O translation intertwines residue induction and restriction

Statement

Assume the Axiom of Choice and fix an admissible origin c; let fiO,eiO be the residue translation functors on the sum of parabolic blocks of The residue translation functors on the sum of parabolic blocks and put Bd=End⁡g(Td)op, the tensor image algebra of Stable range and block idempotent corner for higher-level Schur-Weyl duality. Use its generator-preserving image-tower map Bd→Bd+1. If ui is the generalized-i projector of the last dot in Bd+1, define the image residue functors by fiH(X)=Bd+1ui⊗BdX,eiH(Y)=uiY, with the corresponding source and target content projections. These are the full cyclotomic residue functors of Hecke induction and restriction functors on degenerate cyclotomic blocks whenever both selected algebras are faithfully realized, or the compatible central cuts on the selected contents are fully supported. Then there are natural isomorphisms fiHπ≅πfiO,eiHπ≅πeiO, where π=Hom⁡g(T,−) is the Schur functor of The higher-level Schur-Weyl projective generator and Schur functor, compatible with the residue eigenvalue projectors, the units and counits of the evaluation/coevaluation adjunction and its dual transported reverse adjunction, and with ordinary restricted duality and the ∗-duality of the Hecke side. Consequently the ungraded Grothendieck operators at parameter 1 agree. On the admitted residue intervals of the Fock realization, these operators give the enveloping-algebra Chevalley action and the Schur quotient is a homomorphism for that action. For admissible nonintegral origins the category O side uses the genuine typed coset realization, not an unqualified integer block. The statement preserves the actual residue and standard filtrations; no graded parity or Koszul lift is asserted by these ungraded suppliers.

Facts & Assumptions

Given: The admissible origin c, the tensor objects Td=Pc⊗V⊗d and Td+1=Td⊗V, the Schur functors πd,πd+1, and the residue functors on both sides.

[F1]

The O-side residue functors are exact, biadjoint, preserve projectives and injectives, commute with restricted duality, and agree with the generalized Casimir eigencomponents; their K0 operators are the integrable Fock Chevalley action (The residue translation functors on the sum of parabolic blocks, Residue Casimir operators and local affine-Hecke actions, The residue translation functors give the integrable Fock-space action).

[F2]

The full cyclotomic residue functors are exact, biadjoint and commute with the ∗-duality (Hecke induction and restriction functors on degenerate cyclotomic blocks). The image algebra Bd is the supporting central summand of that algebra for an admissible origin, and inherits its nondegenerate symmetric trace (Stable range and block idempotent corner for higher-level Schur-Weyl duality). Exactness, duality and biadjunction for the image functors defined above are proved below, rather than inferred for an arbitrary quotient tower.

[F3]

The Schur functor is exact, kills exactly the off-standard simples and sends standards to intrinsic Specht modules. Its tensor detector Td is prinjective, its Hecke endomorphism algebra is Bd, and its Whittaker image Ud is a projective generator of the corresponding finite-W image category. There are natural identifications γM:πdM≅Hom⁡Wd(Ud,V ⁣WhM) and the coherent tensor isomorphisms νM:V ⁣Wh(M⊗V)≅V ⁣Wh(M)⊛V, with μd:Ud⊛V≅Ud+1 intertwining the tower generators. In the stable realization Bd is the full cyclotomic algebra, while content projections give the supported blocks. Every category-O projective has a copresentation 0→P→T1→T2 with T1,T2∈add⁡(Td). These are the actual Whittaker/Morita, copresentation and tensor contracts of The Whittaker functor is exact and fully faithful on the required projectives, The Whittaker functor from the relevant parabolic category-O summand, The higher-level Schur-Weyl endomorphism isomorphism and Schur functor images of standard, simple, projective and tilting objects.

[F4]

The parabolic and genuine category-O interfaces with the typed coset realization for admissible nonintegral origins (The integral parabolic category-O blocks for higher-level Schur-Weyl duality).

Proof

technique · direct

Given: The tensor identity Td+1=Td⊗V, the actual Whittaker/Morita tensor data of [F3], and the two pairs of residue functors.

1.1F1F3constructalgebra

Restriction uses the dual natural module. For N in the degree-(d+1) summand and a basis va of V with dual basis va, tensor adjunction gives the natural map ρN:Hom⁡g(Td+1,N)→Hom⁡g(Td,N⊗V∗), ρN(h)(t)=∑ah(t⊗va)⊗va. Its inverse sends g to (t⊗v)↦(1⊗ev⁡v)g(t). These maps are basis-independent by coevaluation and evaluation and commute with the first d tower generators, acting on the Td factors. Thus they identify restriction of πd+1N with πd(N⊗V∗) after the appropriate degree/block projection. The natural and dual natural modules are distinct gln-modules; no identification between them is used.

1.2F3constructalgebra

The induction map is an actual tensor map. Tensoring an endomorphism of Td with idV gives the image-tower homomorphism Bd→Bd+1; it sends the unit to the unit and the first d generators to their tensor actions. For M of degree d, put τM:Bd+1⊗BdπdM→πd+1(M⊗V), b⊗f↦(f⊗idV)∘Rb, where Rb is the right action on Td+1. The first d generators act on Td, so this expression is balanced over Bd and is Bd+1-linear for the left-module convention; naturality follows by postcomposition. To prove it invertible, on the finite-W side form σX(b⊗g)=(g⊛idV)∘μd−1∘Rb. For X=Ud this is the regular-module isomorphism Bd+1⊗BdBd≅Bd+1. It remains an isomorphism on finite sums and summands. Every finite-W image object has a finite projective presentation by summands of finite sums of Ud, and both sides are right exact: induction is right exact, tensoring with V is exact and Hom from Ud,Ud+1 is exact. Passing to cokernels proves σX invertible for all X. Since the Morita functors and tensoring are exact, this also proves image induction exact; its residue summands are exact as well. Image restriction is exact directly. The coherent γ,ν,μ square of [F3] sends 1⊗f by either route to (V ⁣Wh(f)⊛idV)μd−1; Bd+1-linearity then makes the square commute on every b⊗f. Consequently τM is invertible for every M. This presentation argument takes place in the finite-W image category, where Ud is a full projective generator; it does not assert that Td is a full category-O generator.

2.1F1F2step 1.1step 1.2algebra

The two residue projectors. The tower's last dot on Td⊗V is the tensor Casimir, with the normalization of [F1]. Hence τ intertwines its generalized-i eigenprojector with the projector defining fiO. On the dual tensor factor one has the actual operator identity ΩN,V∗ρN(h)=−ρN(hΩTd,V)−nρN(h). Indeed Ebavc=−δbcva and equivariance of h give the first term −∑a,bh(Eabt⊗vb)⊗va and the second term −n∑ah(t⊗va)⊗va, exactly that identity. Thus the last-dot generalized-i projector corresponds to the dual-Casimir generalized-(−n−i) projector, including its nilpotent part. This is the actual adjunction mate and agrees with the flag normalization in [F1]. Under ρ the last-dot projector therefore corresponds to the generalized-(−n−i) projector defining eiO. Applying the source content projector eα and target projector eα+αi to steps 1.1–1.2 gives uα,iπα+αiN≅παeiON and Bα+αiuα,i⊗BαπαM≅πα+αifiOM. Polynomial generalized-eigenspace projectors commute with these natural maps because the maps intertwine the operators, proving the asserted residue compatibility.

3.1F1F2F3step 2.1constructalgebra

The natural duality comparison. The ordinary category-O duality D uses matrix transpose and restricted weight-space duals. The product of the ground contravariant form and the natural-factor forms gives a nondegenerate detector form (xtb,t′)=(t,xtrt′b∗); the Casimir, crossings and content projectors are self-adjoint. Put δM=Hom⁡g(M,Td) with (bf)(m)=f(m)b∗ and X#=Hom⁡Bd(X,Bd) with the same twist. The detector form gives an actual isomorphism β:Td≅DTd, β(t)(t′)=(t,t′). Exact restricted contravariant duality, with its canonical bidual map, consequently gives δM=Hom⁡g(M,Td)≅Hom⁡g(M,DTd)≅Hom⁡g(Td,DM)=πdDM. Its explicit map is f↦[t↦(m↦(t,f(m)))]; its inverse sends g:Td→DM to β−1∘Dg∘bidual⁡M:M→Td. These maps are inverse by the symmetry and nondegeneracy of the form and the bidual identities, and the form's ∗-invariance makes them Hecke-linear. This is a canonical natural Hom-duality isomorphism; it requires neither dimensions of simple images nor self-duality of individual projective summands. Tensor-Hom gives δπd∗≅#, while the symmetric trace of [F2] gives #≅DH by h↦tr∘h. Define θM:M→Dπd∗δM by θM(m)(t⊗f)=(t,f(m)). The displayed form identity makes it balanced over Bd and g-linear. Applying πd gives a natural transformation πd→πdDπd∗δ≅#πdD between exact functors. It is an isomorphism on Td and hence on its finite sums and summands. Apply the copresentations in [F3] to prove it an isomorphism on every projective, by exactness and kernels; then apply projective presentations to prove it on every object, by cokernels. Dualizing yields the natural comparison πdD≅DHπd. The product forms, tensor evaluation and trace form are the same forms used for the dual adjunctions; consequently this comparison identifies their dual unit/counit squares. Since the residue projectors are self-adjoint, it also commutes with each fi,ei separately. Thus Dfi≅fiD and Dei≅eiD. None of this identifies the usual tensor dual V∗ with V.

3.2F1F2F3step 2.1algebra

Grothendieck operators and quotient. Exactness of π and of the residue functors makes the natural isomorphisms of step 2.1 induce [fiH][π]=[π][fiO] and [eiH][π]=[π][eiO]. On G0, the source simple-class basis shows that ker⁡[π] is exactly the span of the off-standard simple classes, and the induced map from this quotient onto G0(B) is an isomorphism. No isomorphism from the entire category-O Grothendieck group is asserted. On split projective groups only add⁡(T) is equivalent to Hecke projectives; an ambient off-standard projective need not have projective image. These distinctions leave the displayed operator equalities intact. On the admitted Fock residue intervals, [F1] supplies the Chevalley relations, and the quotient operator equalities transport them to G0(B). When the selected contents are fully supported, B is their full cyclotomic cut, so the same comparisons apply to that cut.

4.1F1F2step 1.1step 1.2step 2.1step 3.1constructalgebra

Adjunction maps. The first tensor unit is the coevaluation m↦∑a(m⊗va)⊗va, and the tensor counit is evaluation. The induction/restriction unit is z↦1⊗z, and the counit is b⊗z↦bz. Substituting these formulas into τ and ρ gives the same composite maps, term by term: coevaluation is precisely the sum in ρ, and evaluation cancels that sum by va(vb)=δab. Restricting the commuting squares by the content and residue projectors proves compatibility for fi⊣ei. For the reverse adjunction use the biadjoint mate maps supplied by [F1]. By step 3.1 both image functors commute with duality, so dualizing their first adjunction gives the reverse one. Define its unit and counit by these dual mates, with the same normalization as the O-side maps. The first commuting squares then dualize to the reverse commuting squares. The two pairs are thus compared with their transported normalizations; this is stronger than asserting abstract uniqueness of adjoints across a quotient.

5.1F1F3F4step 2.1step 4.1step 3.1step 3.2given∎

Filtrations and boundaries. Applying exact π to the O-side residue standard flags preserves their successive quotients, and the intertwined generalized-eigenvalue projectors select the corresponding residue pieces. Admissible nonintegral origins retain the typed coset realization of [F4]; an integral highest-weight Fock interpretation is used only on its actual integral residue component. All comparisons here are ungraded at parameter one. Together with steps 2.1–3.2 this proves the statement.

Remarks

The raising tensor factor is V and the lowering tensor factor is V∗. Their adjunction is evaluation/coevaluation. Restricted transpose duality fixes the natural factor and commutes with each residue functor; these are different constructions.

5 · Examples, counterexamples and false statements

None yet.

Sources