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Arakawa–Suzuki Functors and Higher-Level Schur–Weyl Duality
1 · Prerequisites
- Abelian Categories
- Absolute and Conditional Convergence; Rearrangement; Products
- Adjunctions Units and Counits
- Affine Algebraic Sets and Coordinate Rings
- Affine Group Schemes, Hopf Algebras, and Rational Representations
- Affine Schemes and the Structure Sheaf
- Algebraic Closure, Embeddings, and Separability
- Algebraic Differentials Separability and Smooth Local Presentations
- Algebraic Extensions, Extension Degree, and Finite Fields
- Algebraic Group Actions, Orbits, Stabilizers, and Controlled Quotients
- Algebraic Zariski Main for Quasi-Finite Morphisms
- Applications of the Fundamental Group
- Arc Length and Rectifiable Curves
- Artinian Rings and Length
- Associated Primes and Primary Decomposition
- Balanced Triples and Global Crystal Bases
- Binary Operations, Monoids, Groups and Subgroups
- Bounded Bimodule Complexes and Derived Tensor
- Bounded Linear Operators and Quotient Spaces
- Bounded Variation and the Riemann–Stieltjes Integral
- Braided and Symmetric Monoidal Categories
- Bruhat Decomposition and Flags over Finite Fields
- Canonical Roots, Signs, and Faithful Reflections
- Cardinal Arithmetic, Cofinality and the Alephs
- Cartan Subalgebras and Root Space Decompositions
- Categorical Braid Actions and Decategorification
- Categories, Functors and Natural Transformations
- Category O Finiteness Duality and Blocks
- Chain Complexes and Homology
- Chain Conditions, Semisimple Modules and the Wedderburn–Artin Theorem
- Chain Homotopy and the Homotopy Category
- Chains, Antichains, Sperner and Dilworth
- Characters and the Orthogonality Relations
- Classical Affine Varieties: Coordinate Rings, Morphisms, and Rational Maps
- Clifford Theory over Normal Subgroups
- Compactness
- Compactness in Metric Spaces
- Completeness, Completion, and Uniform Continuity
- Complex Differentiability and the Cauchy–Riemann Equations
- Complex Power Series and Analytic Functions
- Composition Series, the Jordan–Hölder Theorem and Solvable Groups
- Congruences, the Integers Modulo n and the Chinese Remainder Theorem
- Conjugacy in Sₙ, Generation, and the Simplicity of Aₙ
- Connectedness
- Constant Rank, Submersions, Immersions and Regular Level Sets
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Continuity, IVT, EVT, and Uniform Continuity
- Contour Integration
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Countability Axioms and Cardinal Functions
- Covering Spaces and Lifting
- Coxeter Presentations, Exchange, and Reduced Word Theorems
- Cyclic Groups and Direct Products
- Dedekind Domains and Ideal Classes
- Delta Functors and Universality
- Depth and Cohen Macaulay Modules
- Derived Categories
- Derived Functors
- Determinants of Matrices over a Commutative Ring
- Diagonalisation and the Minimal Polynomial
- Diagonals Separated Morphisms and Valuative Uniqueness
- Dimension Constructible Images and Dimensions of Fibres
- Distributions Integral Manifolds and the Frobenius Theorem
- Divided Powers, Integral Forms, and Quantum Highest Weights
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Divisibility, Greatest Common Divisors and Bézout's Identity
- Dual Spaces, Bilinear and Quadratic Forms, and Sylvester's Law of Inertia
- Eigenvalues, Eigenvectors and the Characteristic Polynomial
- Euclidean Ordinary Differential Equations with Smooth Dependence
- Exactness and the Member Calculus
- Ext and Balanced Resolutions
- Exterior Powers, Orientation and Hodge Duality
- Fibre Products Base Change and Scheme Theoretic Fibres
- Filters and Ultrafilters
- Finite Averaging and Character-Theory Prerequisites
- Finite Counting, Factorials and Binomial Coefficients
- Finite Dimensional Normed Spaces and Riesz Lemma
- Finite Fields and Cyclotomic Extensions
- Finite Proper and Projective Morphisms
- Finite Weyl Invariants, Bruhat Order, and Kostant Harmonics
- Flat Smooth and Etale Morphisms
- Flatness and Faithful Flatness
- Formal Power Series
- Foundations of the Real Numbers for Analysis
- Free Groups and Presentations
- Free Modules, Exact Sequences, Projective and Injective Modules
- Fubini and Change of Variables
- Fundamental Trigonometric Identities
- Galois Orbits and Descent of Simple Finite-Group Modules
- Garside Structure, Normal Forms, and the Center
- Gaussian Elimination, Elementary Matrices and Reduced Row Echelon Form
- Goursat's Theorem and Cauchy's Theorem in a Convex Domain
- Graded Bimodules and Tensor Functors
- Grothendieck Groups and Graded Cartan Pairings
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Group Homomorphisms and the Isomorphism Theorems
- Group Schemes of Finite Type over a Field
- Groups of Multiplicative Type and Arithmetic Tori
- Harish Chandra Isomorphism Casimir and Central Characters
- Hecke Markov Traces and Polynomial Link Invariants
- Hereditary and Productive Behaviour of the Separation Axioms
- Highest Weight Theory for Complex Semisimple Lie Algebras
- Hilbert Space Geometry and Riesz Representation
- Holomorphic Functions of Several Complex Variables
- Homogeneous Resultants and Projective Intersection Length
- Homological Gaussian Elimination
- Homomorphisms Between Verma Modules and Linkage
- Homotopy and Homotopy Equivalence
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Inner Product Spaces, Gram-Schmidt, Projections and Adjoints
- Integrable Highest Weight Kac Moody Modules
- Integral Extensions and Going Up
- Kac Moody Algebras from Generalized Cartan Matrices
- Kahler Differentials Conormal Sequences and Infinitesimal Lifting
- Kashiwara Operators and Crystal Lattices
- Kazhdan–Lusztig Bases, Polynomials, and Cells
- Koszul Complexes and Regular Sequences
- Krull Dimension and Height Theorems
- Lie Algebra Representations, Enveloping Algebras, and PBW
- Lie Algebras and Infinitesimal Group Schemes
- Lie Groups, Invariant Fields, and the Exponential Map
- Lie Subgroups, Actions, and Homogeneous Spaces
- Limits and Colimits
- Limits of Real Functions
- limsup, liminf, and Subsequential Limits
- Line Integrals and the Gradient Theorem
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Localisation of Modules and Support
- Long Exact Sequences in Homology
- Manifolds with Boundary Collars and Orientations
- Mapping Cones Cylinders and Chain Triangles
- Maschke's Theorem, Complete Reducibility and the Structure of k[G]
- Matrices, the Matrix of a Linear Map, and Change of Basis
- Metric Spaces
- Mixed Partials, Taylor Formulae, and Extrema
- Modular Representations and Projective Covers
- Modules over a Principal Ideal Domain and the Canonical Forms
- Modules, Submodules, Quotient Modules and the Isomorphism Theorems
- Monotone Functions, Discontinuities, and Continuity Sets
- Monotone Sequences, Bolzano-Weierstrass, and Cauchy Completeness
- Morphisms Local Rings and Rational Maps of Affine Varieties
- Noether Normalisation and Nullstellensatz
- Noetherian Rings and Hilbert Basis
- Nonaffine Algebraic Groups, Barsotti-Chevalley, and Abelian Varieties
- Normal Subgroups and Quotient Groups
- Normed and Banach Spaces
- Order, Zorn's Lemma, and the Axiom of Choice
- Ordinal Arithmetic and the First Uncountable Ordinal
- Ordinals, Cardinals, and Transfinite Recursion
- Parabolic Category O and Fock-Space Bases
- Parabolic Subgroups and Double Coset Geometry
- Partitions of Unity and Paracompactness
- Permutation Statistics, Inversions and Eulerian Numbers
- pi: the Equivalent Characterizations
- Picard-Lindelöf and First-Order Ordinary Differential Equations
- Polynomial Rings, the Division Algorithm and Roots
- Power Series and Real-Analytic Functions
- Preadditive and Additive Categories and Biproducts
- Presheaves Sheaves Stalks and Sheafification
- Prime Spectra and Radicals
- Primes, Euclid's Lemma and the Fundamental Theorem of Arithmetic
- Principal Series Representations of GL N over a Finite Field
- Products Segre and Veronese Embeddings and Grassmannians
- Proj Projective Schemes Twisting Sheaves and Ampleness
- Projective Algebraic Sets Projective Morphisms and Cones
- Projective and Injective Resolutions
- Projective Functors and the Soergel Functor in Category O
- Projectives Standard Filtrations and Bgg Reciprocity
- Properties of the Integral and the Working FTC
- Quantized Enveloping Algebras and Quantum Serre Relations
- Quasi Coherent and Coherent Sheaves and Vector Bundles
- Rank Theorems and Embedded Submanifolds
- Real Forms and Reflection Geometry
- Rees Modules Artin Rees and Hilbert Samuel Theory
- Reflective Subcategories and the Adjoint Functor Theorems
- Regular Local Rings and Homological Dimension
- Relations, Functions, and Quotients
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Root Systems, Dynkin Diagrams, and the Cartan-Killing Classification
- Roots, Rational Powers, and Classical Inequalities
- Rouquier Complexes and Categorical Braid Relations
- Schemes Subschemes and Morphisms Locally of Finite Type
- Semisimple Lie Algebras, Cohomology, and Levi Theory
- Separation Axioms: the Hierarchy
- Sequences and Limits
- Sequences and Series of Functions; Uniform Convergence
- Series: Convergence and the Nonnegative Tests
- Sheaf Operations Exactness Ringed Spaces and Module Pullback
- Simple Field Extensions and the Construction of the Complex Numbers
- Sine, Cosine, and the Definition of Pi
- Singular and Parabolic Kazhdan–Lusztig Theory
- Smooth Manifolds and Smooth Maps
- Smooth Partitions of Unity and Exhaustions
- Smooth Vector Bundles and Sections
- Soergel Intersection Forms and Hodge Theory
- Solvability by Radicals and Kummer Theory
- Solvable and Nilpotent Lie Algebras
- Specht Modules and the Irreducibles of the Symmetric Group
- Splitting Fields
- Subobject Lattices Generators and the Grothendieck Axioms
- Subspaces, Products, and Quotients
- Suprema and Infima
- Sylow's Theorems, p-Groups and Nilpotent Groups
- Symmetric Groups, Cycle Decomposition and the Sign Homomorphism
- Symmetric Polynomials and the Fundamental Theorem of Symmetric Functions
- Tangent Cotangent and the Differential
- Tensor Coherence and Algebraic Descent
- Tensor Products of Modules
- Tensor-Product Crystals and Highest-Weight Crystal Uniqueness
- The BGG Resolution
- The Branching Rule and the Young Graph
- The Burau Representations
- The Cantor Set, Baire Category, and Measure Zero in ℝ
- The Complex Exponential and Euler's Formula
- The Derivative and the Mean Value Theorems
- The Determinant of a Linear Operator, Cofactors and Cramer's Rule
- The Diagram Lemmas in an Abelian Category
- The Exponential Function
- The Field of Fractions and Localisation
- The Fundamental Group
- The Fundamental Theorem of Algebra
- The Fundamental Theorem of Finite Abelian Groups
- The Fundamental Theorems of Calculus
- The Galois Correspondence
- The Group Algebra and Representations of Finite Groups
- The Holomorphic Inverse Function Theorem and Weierstrass Preparation
- The Identity Theorem, the Maximum Principle and the Open Mapping Theorem
- The Inverse and Implicit Function Theorems
- The Inverse Function Theorem Completed
- The Kazhdan–Lusztig Character and Multiplicity Theorem
- The Logarithm and General Powers
- The Riemann Integral in Rᵐ and Jordan Content
- The Riemann Integral: Definition and Integrability
- The Spectral Theorem, Positive Operators and Singular Value Decomposition
- The Topology of Euclidean Space
- The Total Derivative in ℝᵐ → ℝⁿ
- The Weyl Kac Character Formula
- The Winding Number and the Global Cauchy Theorem
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topology of ℝ
- Tor Flatness and Global Dimension
- Triangularisation, Generalised Eigenspaces and Jordan Canonical Form
- Triangulated Categories
- Type-A Soergel Bimodules and Hecke Categorification
- Uniform Spaces: the Three Definitions
- Unipotent and Solvable Groups and Borel Fixed Points
- Universal Coefficients and Kunneth Theorems
- Universal Properties, Representables and the Yoneda Lemma
- Valuation Rings and Discrete Valuation Rings
- Vector Fields Flows and Lie Derivatives
- Vector Spaces, Linear Subspaces, Span and Direct Sums
- Verma Modules and Shapovalov Forms
- Weyl Character and Multiplicity Formulas
- Yoneda Extensions and Homological Dimension
- Young Diagrams Tableaux and Permutation Modules
- Zariski Tangent Spaces, Regular Points, Smoothness, and Bertini
- Zariski Topology on Prime Spectra
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 , the stable range and its block-idempotent corner, and the Hecke residue functors with their intertwining with category- translation. Everything is stated over 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 with its ordered monomial basis and filtration, and Arakawa-Suzuki Casimir operators on tensor functors defines the natural operators and on , including the normalization 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 -action on for every -module .
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 , the parabolic subalgebras , the centralizer basis of and the Whittaker character ; The type-A finite W-algebra and the Whittaker category defines the finite W-algebra with its -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 with its bounded monomial basis, central blocks and trace form; The deformed tensor space for the type-A finite W-algebra defines the filtered -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 on this tensor space for 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 on the parabolic summand from the continuous -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 and the distinct whole-summand projective generator , the Schur functor and its right-exact left adjoint, with the boundaries of the left adjoint stated exactly. The higher-level Schur-Weyl endomorphism isomorphism identifies 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 and the central block corner outside it; Hecke induction and restriction functors on degenerate cyclotomic blocks defines the Hecke residue functors 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 , 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
The degenerate affine Hecke algebra
Definition
Work over the field and fix an integer (Algebras over a commutative ring, central structure maps, and algebra homomorphisms, Commutative ring). Let be the free associative unital -algebra on the symbols (for there is only the unit; for only ), with its word basis and universal property (The free associative R-algebra on a set and descent of relations), and let 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:
- for all ;
- for ;
- for ;
- for with ;
- for , , and , for and .
The degenerate affine Hecke algebra is the quotient -algebra with unit element written (For a two-sided ideal , the additive cosets form a ring with identity ). We keep the symbols for their images, and for we write for the image in of any word in the representing ; this is independent of the chosen word once the basis theorem below is proved. For and , the notation means the quotient by the two-sided ideal generated by .
The verification below establishes exactly the structure of used throughout this page: the ordered monomials form a -basis, so that as a vector space with polynomial and group-algebra subalgebras (The polynomial ring as finitely supported coefficient families on monomials, The group ring of finitely supported formal -linear combinations of group elements); and ; for and every there is a unique algebra isomorphism and total polynomial degree is an algebra filtration whose associated graded is the semidirect product in which acts by swapping and . For , the cross relation is inhomogeneous, so it does not turn into a graded algebra with and . For the algebra has its degree-zero grading, and for the algebra has its natural polynomial grading.
Facts & Assumptions
Given: An integer , the field , the free associative -algebra on the symbols , and the two-sided ideal of the Definition.
is the group of bijections of under composition, with ; it is generated by subject to the Coxeter relations , , for (The symmetric group : the bijections of a set under composition, The finite symmetric group , one-line notation, and cycle notation, The symmetric group has the Coxeter presentation).
is a unital -algebra with -basis , product induced by composition and unit the identity permutation (The group ring of finitely supported formal -linear combinations of group elements, The group ring is a unital -algebra with basis , and each is a unit of ).
is a commutative -algebra with -basis the monomials ; it is a domain with fraction field in which every nonzero polynomial is invertible; since as polynomials, is invertible in (The polynomial ring as finitely supported coefficient families on monomials, Commutative ring, A polynomial ring over an integral domain is an integral domain, The field of fractions of an integral domain, is a field and embeds the integral domain ).
has the word basis and universal property, the two-sided ideal generated by a set is the set of finite sums with , and a homomorphism killing factors uniquely through (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 , the additive cosets form a ring with identity ).
For -algebras the tensor product is a -algebra with ; if and are bases, then is a basis (The tensor product of -algebras has multiplication , The elementary tensors of two bases form the product basis of the tensor product).
Algebra homomorphisms are unital ring homomorphisms over the structure map and preserve (Algebras over a commutative ring, central structure maps, and algebra homomorphisms, Ring homomorphism: additive, multiplicative, and required to send to ).
Proof
Given: The data of [F1]-[F6]: the presented algebra , the symmetric group , the group algebra , the polynomial algebra with fraction field , and the tensor-product and quotient structures.
The cases . For there are no symbols, so and , giving . For the only symbol is and the list of relations is empty; the words in are , a -basis of by [F4], so is the polynomial algebra with basis , .
The rational-function model. On the -vector space of [F3] let denote multiplication by , and for let be the operator interchanging the -th and -st arguments. Put (invertible by [F3]), and . For a word in the generators of set and . The operators are well defined by the Coxeter presentation [F1], because the satisfy those relations and the presentation says that any two words for the same are related by them.
The skew algebra. Let , a -subspace. For and the identities and hold (the first expresses the substitution action on functions, the second is word concatenation), so ; hence is a subalgebra of . The set is -linearly independent: suppose with not all zero; multiplying the resulting identity of functions by a common denominator of the , we may assume . Fix integers whose consecutive gaps exceed the total degree of every , and order the finitely many with by the lexicographic order of the vectors ; let be maximal and let be the exponent of a top monomial of . Applying the sum to the monomial gives , because ; the vectors are distinct, and at the first coordinate where differs from the gap exceeds the degree bound, so the monomial occurs exactly once, in the summand , with nonzero coefficient. This contradicts the vanishing of the sum, proving the claim.
Spanning of by ordered monomials. We show that every element of is a -linear combination of the images of ordered monomials ; since words span by [F4], it suffices to treat the image of a word in the symbols. Use strong induction on the pair ordered lexicographically, where is the number of -symbols in and is the number of pairs of positions such that the -th symbol is some and the -th symbol is some . If , then is a word in the ; by the Coxeter presentation [F1] the subalgebra generated by the is spanned by the images of the elements , so the claim holds. If and every -symbol precedes every -symbol in , then is of the form (word in 's)(word in 's), and the claim follows from commutativity of the 's and the case . Otherwise with adjacent symbols; use if , if (the relation solved for ), and if . In every case , where the first word has the same and one fewer -inversion pair, while the second has -symbols; both fall under the induction hypothesis. Hence the images of ordered monomials span .
Jucys-Murphy elements. For put , so . Then (i) for all ; (ii) for ; and (iii) . For (i) with write for the sum of all transpositions in ; is central in because conjugation permutes the transpositions, and . Since for , centrality of in and of in gives . For (ii), conjugation by sends each transposition to ; if both entries are fixed, and if the sum over contains the pairs with and , whose images are interchanged, so the sum is preserved. For (iii), conjugation sends to for and fixes , so ; multiplying on the right by and using gives (iii).
The model satisfies the relations. Since , the operator identity and the rules , hold; hence and . For both and commute with , so . For the cross relations, use , and the two identities and : for the first, while , and their difference is ; the second is the same computation with the roles of and interchanged. Therefore and . For , the variables and swaps in are disjoint, so they commute. For the braid relation put , , , so . The product rule of step 1.3 expands both and with coefficients, in the order , equal to . Here and , both consequences of , give the two shorter-swap coefficients and the common identity coefficient. Thus the braid relation holds. Hence the assignment , preserves all the relations of the Definition, and by the universal properties [F4] it defines an algebra homomorphism .
Triangular expansion. Fix with a reduced word , and put in , with the empty prefix acting as the identity. Every transported factor is nonzero because the prefix is a field automorphism. In the expansion of by the product rule of step 1.3, the term choosing the factor for every contributes after the scalar coefficients are moved left, while every other term is with the product of a proper subword of in the induced order. If denotes the minimal number of generators needed to express a permutation, then such a proper subword has , using subadditivity of and reducedness. Collecting the expansion in the -basis therefore gives with and .
The evaluation homomorphism. Assume . The assignment , defines an algebra homomorphism : the images of the 's commute by step 1.5(i); the images of the satisfy the Coxeter relations by [F1]; and the cross relations follow from step 1.5(ii) and from , , which are step 1.5(iii) read in both directions. Since , the quotient universal property [F4] yields an algebra homomorphism , which is surjective because the generate .
Independence of the monomials in the model. By step 2.2 the change-of-basis matrix from to inside is triangular with nonzero diagonal when permutations are ordered by length, hence invertible over the field ; thus is an -basis of . Suppose in with finitely supported. Grouping by gives with ; -independence of the forces for every , and linear independence of the monomials [F3] then forces . Hence the elements are -linearly independent.
Basis theorem. Let and write using step 1.4. If , applying the homomorphism of step 2.1 gives , and step 3.1 yields . Hence the ordered monomials form a -basis of , and the -linear map , , is an isomorphism by [F5]; in particular and are subalgebras of and the cross relations hold. The elementary cases , were recorded in step 1.1.
The inverse map. Assume . In the relation gives, after left multiplication by and use of , the recursion . Hence in one has and inductively with in the subalgebra generated by the images of the , namely and . By the basis theorem of step 4.1 every element of is a combination of monomials , and replacing each by expresses its image in as an element of the image of the subalgebra generated by the ; by [F1] and [F2] that image is the -span of . Therefore the canonical map , , has image equal to the whole quotient, and it is injective because by construction; hence is an isomorphism. Under it corresponds to , and by step 2.3, so ; in particular corresponds to the scalar , while for the image is not the scalar . The specified images of both the and the determine the homomorphism uniquely because these elements generate the quotient.
The degree filtration. For let be the image of the -span of all words in the symbols containing at most of the symbols . Steps 1.4 and 4.1 identify with the span of the monomials with . The substitution rules of step 1.4 replace an adjacent pair by terms containing at most one -symbol each, so a product of a word with -symbols and a word with -symbols rewrites into words with at most -symbols; hence and is an algebra filtration with .
The associated graded is a semidirect product. Let be the algebra with -basis and product , where ; equivalently, is generated by the symbols and subject to the relations obtained from those of by deleting the inhomogeneous term from both cross relations, i.e. and . In the defining relations of 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 element) (degree element), so their degree- parts are exactly and . Consequently there is a surjective graded algebra homomorphism sending and to the symbols of and . In degree both sides are -spanned by the symbols with : these form a spanning set of by step 5.2 together with the basis theorem of step 4.1, and they form the basis of the degree- part of by construction; a surjection between -vector spaces with a spanning set of the same finite cardinality as a basis of the target is an isomorphism. Hence in every degree, and the associated graded is the semidirect product in which swaps and , as claimed.
Polynomial grading boundaries. For , step 1.1 gives with its degree-zero grading; for , it gives with the usual polynomial grading. For , suppose there were an algebra grading with in degree and in degree . Then the relation would have its left-hand side in degree and its right-hand side in degree , forcing , which is impossible. Hence for 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 has degree and degree and the associated graded is commutative in the polynomial part and is noncommutative overall for ; it is the filtration used for the cyclotomic quotients later on this page.
-
The Arakawa-Suzuki generators used in the tensor constructions on this page are not the of this presentation: on a tensor module they differ by the central endomorphism 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 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.
Type-A nilpotent orbit closures are normal via chain varieties
Statement
Assume the Axiom of Choice. Let be a nilpotent endomorphism of a finite-dimensional complex vector space (Nilpotent endomorphisms and their nilpotency index), let be the closure in of its conjugacy orbit (Classical complex matrix Lie algebras), and let . Then is a reduced irreducible normal domain and . This holds for every Jordan type, not only the regular nilpotent cone.
The proof uses the chain schemes: if the Jordan partition of has column lengths , put and for . Let with coordinates and let be the closed subscheme , . Then is a complete intersection, smooth outside a closed subset of codimension , reduced, irreducible and normal, and the invariant ring under is the coordinate ring of via the end map when . For the empty Jordan diagram (, ) and the single-column diagram (, ), the chain has no variables or equations: take , trivial and ; the equation list above is imposed only on existing links. In these cases is a point, its boundary is empty, and its boundary codimension is .
Facts & Assumptions
Given: AC; a finite-dimensional complex vector space of dimension , a nilpotent of Jordan type with column lengths , , the spaces , , and the chain scheme of the Statement.
Jordan strings: every nilpotent endomorphism has a Jordan-string basis; conjugacy classes in are -orbits, and nilpotent elements form a closed cone; for , the nilpotency index of a type- element is the largest part ; on the least-positive-exponent nilpotency index is 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).
Orbit dimension and boundary: for the orbit of a closed point under a connected smooth group, and 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).
Nilpotent type invariants: for a nilpotent of type , ; the conditions for all are equivalent to (dominance of partitions, equivalently ); and . To compute the stabilizer dimension, each string-pair homomorphism is determined by a top-vector image killed by the source string length, giving parameters; summing gives . Counting that same sum rowwise gives (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).
Jacobian criterion for : at a closed point , is regular iff . Krull's height theorem: every minimal prime over an ideal generated by elements has height at most . Cohen-Macaulay: a quotient of a polynomial ring by a regular sequence is Cohen-Macaulay; a Cohen-Macaulay ring satisfies for all ; 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).
Serre conditions: a Noetherian ring is reduced iff it satisfies and , and normal iff it satisfies and (serre r zero s one characterises reducedness, serre normality criterion).
Invariants: finite-dimensional rational -modules are completely reducible, and the -invariants of tensor powers of and 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
Given: AC, the nilpotent endomorphism , its Jordan columns , and the chain scheme and end map of the Statement, including its empty-chain conventions.
Empty chains. If , take ; if on a nonzero space, its Jordan diagram has a single column and . In either case there are no chain variables or equations, , is trivial and . 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 .
The open chain locus. Put and . The differential of the chain equations is , with the index-zero terms zero. If each is injective or is surjective, these equations can be solved successively for any prescribed right-hand sides: use a left inverse of to choose , or a right inverse of to choose , after the preceding pair is fixed. Thus the open locus with this condition is smooth of dimension by [F4]. It is nonempty: use , inclusions , and restrictions , transported to the fixed spaces. These maps satisfy the equations and have end map .
Alternating strings and their stabilizers. For a nilpotent pair , , the odd operator on 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 from and from . Removing all letters gives the Jordan rows of , and removing all letters gives those of . 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 kills exactly a terminal and misses exactly an initial ; consequently is injective iff every string ends in , and is surjective iff every string begins in .
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 to row increases by and therefore decreases the orbit dimension by that positive even number. Each allowable unit move from row lengths with is realized by a one-parameter degeneration. On chains and of the destination type, keep the usual lowering maps except send to , with . At the type is ; for the ranks of powers are those of (the chain generated by has length , and the remaining chain has length ). 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 for the total sum; individual summands in a difference of square sums need not be even.
The pair-orbit dimension. Write , , and let be the dimensions of the even and odd centralizers of . A homomorphism between Jordan strings of lengths has possible shifts. Counting the parity of those shifts, odd strings of the same endpoint type contribute to the even-minus-odd count, and odd strings of opposite type contribute ; the two opposite Hom directions for an odd/even pair cancel, and even/even pairs contribute zero. Summing gives , because the difference between the numbers of odd -type and odd -type strings is . The pair orbit therefore has dimension , half the dimension of the ordinary orbit of . If a string has letters and letters , then except for equal odd lengths with opposite endpoint types, where the left side is larger by one. Let count the odd strings of length beginning with the two respective letters, and put . Writing and for the ordinary conjugacy orbits, the ordinary Jordan centralizer counts now give . This is a dimension identity for the orbit, not for the full matrix space minus the pair orbit.
Chain strata. Stratify by its compatible alternating-string diagrams at every link. Compatibility means that the -diagram of one link equals the -diagram of the next. These are finitely many locally closed strata. For a link , , projection of its pair orbit to the orbit of has fiber ; projection to the orbit of instead has fiber . 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 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 , where is the type of its final end map.
Dominance and the top stratum. The chain equations make factor through , so and . Thus its type is dominated by by [F3]. For a -diagram , every row must first be filled internally by alternating letters; this requires exactly letters, the size of the diagram obtained by deleting its first column. Over the top diagram , this equals , leaving no extra letters: every string starts and ends in and the lower diagram is exactly the first-column deletion of . Repeat down the chain. There is exactly one top stratum; it has both maximal-rank maps at every link, lies in , and has every . Finally, expanding gives , so its dimension is .
Drops of at least four. By the stratum formula and the nonnegativity of all , a final orbit drop of at least four gives . Every non-top stratum has dimension at most . 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 .
Drops of two and the nonsmooth-locus bound. Suppose is obtained from by moving a box to the next row. Let and denote first-column deletions and let , . At the last link the available number of letters is and its -diagram must be dominated by , since its powers factor through the shorter chain. If the receiving row was nonempty, : internal filling consumes every , all strings begin and end in , and the same next-row degeneration passes to the shorter chain. If a new singleton row is created, . After internal filling there is one extra . It can be attached at either end of the shortened last row, at either end of the new singleton row, or placed in a new singleton row. No earlier row can receive it: its -diagram would gain a box earlier than the removed last-row box and violate dominance by . In the first four placements one map is maximal rank; the lower diagram is either or its next-row degeneration. In the fifth placement both maps fail maximal rank, and singleton strings of both types occur, giving . This remains valid when the shortened row is itself a singleton, when there can be more than one singleton . Inducting through the shorter chain shows that either every link has a maximal-rank map and , or some . In the latter case the dimension formula gives . Together with step 5.1, this proves .
Complete intersection and reducedness. Every irreducible component of the scheme cut out by its equations has dimension at least by [F4]. The top stratum has dimension and all other strata have smaller dimension by step 5.1, so every component has dimension . Thus the equation ideal has height . Its homogeneous generators form a regular sequence in the polynomial ring: at the homogeneous maximal ideal, every prefix of length has height at least , since adjoining the remaining equations raises height by at most ; 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 and . Every component meets the smooth open by step 6.1, so it satisfies ; [F5] implies reducedness.
Irreducibility and normality of the chain. The unique top stratum is irreducible. Its closure contains every component: otherwise a component of dimension would have a nonempty open subset outside that closure, contained in a finite union of strata of dimensions at most , which is impossible. Thus the reduced chain ring is a domain. Its singular locus is contained in , of codimension at least two by step 6.1, so it satisfies ; it satisfies by step 7.1. Serre's criterion [F5] gives normality.
The invariant quotient. For one pair , , invariants under are generated by entries of : the scalar matrices force equal polynomial degrees in , 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 , with possible cyclic traces also polynomials in those entries. For rational finite-dimensional 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 ; an invariant complement then respects the center as well. It respects the group because elementary unipotents and diagonal matrices generate . 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 and the remaining variables; the chain equation replaces by . 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 . Thus is generated by those entries, and is the coordinate ring of the closure of . The rank bounds of step 4.1 put the image in the orbit closure of , while the inclusion/restriction construction of step 1.2, applied to every conjugate of , puts its full orbit in the image. Hence that closure is and .
Normality and boundary of the orbit closure. An element of integral over is also integral over the normal domain , hence belongs to it. Being a fraction of invariant elements it is fixed by , so it belongs to ; no equality between the full invariant fraction field and the fraction field of the invariant ring is needed. Therefore 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
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The chain scheme parametrizes compatible alternating-string data: its smooth open part dominates the conjugacy orbit of through the end map , and the invariant quotient collapses the chain data to the orbit closure. No rational-singularity or Hochster-Roberts input is used.
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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 . Non-top strata may be smooth divisors; it is the complement of that has codimension at least two. The singleton-string case is retained in the five-placement induction.
Arakawa-Suzuki Casimir operators on tensor functors
Definition
Work over (Classical complex matrix Lie algebras, Algebras over a commutative ring, central structure maps, and algebra homomorphisms). Fix , let with its matrix units and the trace form , which is symmetric, nondegenerate and invariant (Trace forms are symmetric and invariant), and let be the central element (the identity matrix). The dual basis of under is , so the invariant Casimir tensor is Its action on a tensor product of two -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 be a -module and the natural module (Representations of Lie algebras). On the tensor product (The tensor product from the additive group underlying the free -module on , elementary tensors, and finite tensor sums, Associativity of tensor products for compatible bimodules) label the factors , with factor equal to . For let denote the operator obtained by applying in the two labelled factors, and for distinct let denote the operator that interchanges the two labelled factors (the flip of on two -factors). Define, for and , Finally put and define the Arakawa-Suzuki normalized operators where denotes the endomorphism of given by the action of on the factor . This is a central endomorphism, and is a scalar only when acts scalarly on .
The verification below records the properties of these operators used on this page: acts on as the flip; the operators and are natural in and commute with the -action; the recursion holds; is the Casimir of relative to the restricted trace form; and the operators are exactly the source operators of [AS, (2.2.2)]. For the family is empty; for the trivial module one has , so and .
Facts & Assumptions
Given: , with matrix units and trace form , the central element , a -module , the natural module , and .
Matrix units multiply by , , and is symmetric and invariant; is central, so its action on any module is an endomorphism commuting with the action (Classical complex matrix Lie algebras, Trace forms are symmetric and invariant).
The Casimir tensor is independent of dual bases and invariant under the diagonal adjoint action: for every . Indeed, for the matrix-unit relations give the cancelling sum , and linearity gives every . Therefore its action on a tensor product of -modules is a -intertwiner. Module actions extend uniquely to (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).
Tensor products of modules are modules with the factorwise action, associative up to canonical isomorphism, and pure-tensor bases multiply to tensor bases (Representations of Lie algebras, The tensor product from the additive group underlying the free -module on , elementary tensors, and finite tensor sums, Associativity of tensor products for compatible bimodules, The elementary tensors of two bases form the product basis of the tensor product).
The degenerate affine Hecke algebra is presented by with the Coxeter relations and the cross relations , ; the recursion holds in (The degenerate affine Hecke algebra).
The source operators: [AS, (2.2.1)-(2.2.2)] define, on for the Casimir, the transposition operators and the generators .
Proof
Given: The data of [F1]-[F5] and the operators of the Definition.
is the flip on . On the tensor basis, by [F1]. Consequently whenever the two labelled factors are both natural factors; in particular on the -factors.
Naturality and commutation with . For a -module map , the map intertwines and : it plainly intertwines the place permutations , and it intertwines because the Casimir operator on a tensor product of modules is an intertwiner by [F2]. For the same reason each and commutes with the -action on , the action on the -factors being the natural one.
The Casimir. The trace form restricts to a nondegenerate form on : because and . Hence is the inverse tensor of : for , contracting the second factor of with gives , while contracting the second factor of with gives ; so contraction with also returns , and by [F2] the dual tensor is unique. Thus is the -Casimir for the restricted trace form.
The recursion. Since and are involutions with and conjugation by replaces the label by in every operator supported on labels , one has , for , and . Hence , using and . 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 ↗.
The source dictionary. Let now denote the -Casimir in the formula (2.2.1) of the source [F5], so that on two natural factors by steps 1.1 and 1.3, i.e. , which is exactly [AS, (2.2.1)]. On the library -Casimir satisfies (the extra term acts on factor as and on factor as the identity on ), while for two natural factors; therefore , which is precisely the source formula (2.2.2) in [F5].
Special cases. For there are no labels , so the family and is empty and the Definition records only the module ; the recursion and the dictionary are vacuous. For the trivial module the action of is zero, so and ; hence , with the empty sum .
Remarks
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The operators are the universal (trace-form) Casimir operators; the operators differ from them by the central endomorphism 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.
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The sign of the shift in the recursion is fixed by the cross relation of The degenerate affine Hecke algebra: the computation of step 2.1 gives , whose right-hand side contains , not .
Nilpotent-orbit tensor covariants extend and polarize
Statement
Assume the Axiom of Choice. Let be a nilpotent endomorphism of a finite-dimensional complex vector space , let be its centralizer, and let .
- Every -fixed endomorphism is the value at of a -equivariant polynomial map (polynomial in the matrix entries of the input, with ).
- Every such equivariant polynomial map is a finite sum with , where is a place permutation of the tensor factors and is an invariant scalar polynomial in (a polynomial in the traces ).
The extension in (1) is proved by Hartogs lifting on the normal codimension- 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 in with and largest Jordan block when , an integer , the orbit closure with dense orbit , and the centralizer .
is the spectrum of a reduced irreducible normal domain , and is its dense open orbit; is the unit group of the full finite-dimensional associative centralizer algebra . Its units are exactly : if commutes with and is invertible on , its inverse also commutes with . This is a nonempty open subset of the affine vector space , containing the identity, so 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).
Hartogs lemma for a normal domain : a fraction regular in codimension lies in . More precisely, if is regular off a closed subset of codimension , then . Proof ingredients: set ; for every height-one prime; if then every associated prime of has height by the normal property and the depth criterion; prime avoidance produces avoiding those primes; from and regularity of modulo one gets , and cancellation gives (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).
Weyl complete reducibility applies to finite-dimensional -modules in characteristic zero; the reduction in step 4.1 gives the required -invariant lifting for the polynomial-map spaces used here. Invariant tensors in mixed tensor powers of are spanned by permutation contractions (Weyl's complete reducibility theorem, The Schur-Weyl mutual centralizer theorem on tensor powers).
The trace form on is symmetric and nondegenerate, and tensor bases identify with (Classical complex matrix Lie algebras, The elementary tensors of two bases form the product basis of the tensor product).
Proof
Given: The data of [F1]-[F4]: the nilpotent , the normal orbit closure with dense orbit , the connected centralizer , the degree , and a -fixed .
The zero-dimensional case. If , its orbit closure is a point and its boundary is empty by [F1]. For , 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 , 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 , so its largest block length exists.
Hartogs lifting. Let and let be regular on , hence regular off a closed subset of ; since has codimension in by the normality lemma [F1], is regular in codimension and therefore extends to by [F2]. Applying this coordinatewise to maps into a finite-dimensional vector space shows that every regular map into a finite-dimensional vector space extends uniquely to a regular map .
The equivariant map on . Fix and define, for , . This is well defined: if , then , so by -invariance, which rearranges to . The map is -equivariant by construction: for .
Regularity of on . The ranks of are constant on . Cover 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 with entries regular in . Let carry a fixed Jordan basis for to this chosen Jordan basis for , with the same ordered string lengths. Then . Restricting to the open chart where the Jordan-basis determinant is nonzero makes both and regular, since their entries have only the fixed nonvanishing minors and determinant as denominators. Thus is the map of step 1.3 and is regular on each chart. These charts cover ; on overlaps , so the expressions agree by -invariance of . Hence is regular on .
Extension to . By steps 1.2 and 2.1 the map is a regular equivariant map on the dense orbit; by step 1.2 it extends uniquely to a regular map . Since and is an affine closed subset of the affine space , the coordinate functions of are restrictions of polynomial functions on ; fixing representatives gives a polynomial map extending .
Equivariance of the polynomial lift. The extension on is equivariant: for every , the two regular maps expressing equivariance agree on the dense orbit by step 1.3 and therefore on . Let be the finite-dimensional rational module of polynomial maps of degree at most , for , with action . Let consist of maps vanishing on . Then is stable and the class of the lift from step 3.1 in is invariant. Scalar matrices act trivially on : they conjugate neither the input nor the output. For , Weyl's theorem [F3] applied to the semisimple Lie algebra gives an -stable complement to . This complement is stable under , since elementary matrices generate that group and their rational representation acts by exponentiating the differential; together with scalar matrices they generate over . For the whole group acts trivially, so any vector-space complement suffices. The quotient map restricted to this complement is thus a -isomorphism and lifts the invariant class to an invariant . It agrees with on and satisfies , proving (1).
Polarization. Write for its homogeneous components of degree ; each is equivariant. Fix and assume for the structure argument that is homogeneous of degree . Polarize the matrix variables of and pair the output in with independent matrices using the nondegenerate trace pairing on each tensor factor; this produces a multilinear -invariant in matrix arguments.
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.
Covariant normal form. Depolarize in the identical variables and read each contraction cycle. A cycle that uses only -arguments contributes a scalar invariant polynomial in ; a cycle that uses some -arguments alternates blocks of 's and single 's, so its trace is precisely the trace pairing of with a place permutation of . By nondegeneracy of the trace pairing, the operator identity follows, with , a place permutation and a scalar invariant polynomial (a polynomial in the traces ); summing over the homogeneous components gives assertion (2).
Evaluation at . Since for the largest Jordan block length of , evaluating the normal form at kills every term with some ; the surviving terms are place permutations applied to a tensor product of nonnegative powers multiplied by the scalar invariants , which are complex constants; since for every positive , the scalar invariant polynomials satisfy . This gives the concrete description of the -fixed endomorphisms used by the double centralizer theorem.
Remarks
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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.
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The scalar invariant coefficients lie in the polynomial ring generated by the traces of powers of ; evaluating at nilpotent gives the complex constants , independent of the chosen nilpotent orbit point.
The type-A nilpotent pyramid, good grading and Whittaker character
Definition
Work over . Let be a partition of with transpose , where for a nonempty row list and for an empty row list. Zero-length rows have no boxes. Let with matrix units in the standard basis (Classical complex matrix Lie algebras). Number the boxes of the diagram of by down columns from the left, and for a box write for its row and column, for the box immediately to its left (or if absent), and for the box immediately to its right (or if absent). Define the nilpotent endomorphism and declare for all , so that with . Put and for rows define the shift if and if , together with the centralizer elements Finally let be , where the trace is the trace of the matrix.
The verification below records the properties of this data that are used throughout this page. has Jordan type ; is a parabolic subalgebra with Levi factor and nilradical , while is the nilradical of the opposite parabolic; the elements with form a basis of the centralizer ; the box set is in bijection with via , and and is a Lie algebra character, . This grading is the type-A pyramid good grading in the degree-one convention: is injective for and surjective for . For it differs from the standard Dynkin grading, in which has degree rather than . For all boxes lie in one column or there are no boxes, and the pyramid grading and the trivial Dynkin grading both concentrate in degree zero. If , take : the box set and both centralizer index sets are empty, , , and . These conventions also permit an empty row list.
Facts & Assumptions
Given: A partition of with transpose , the diagram boxes with row, column, and data, the nilpotent , the grading and the subspaces , and the elements and .
Matrix units satisfy and for , and the trace is (Classical complex matrix Lie algebras).
Jordan strings: a nilpotent endomorphism is described by its strings ; the Jordan type is the partition of the string lengths, and the centralizer of a nilpotent of type has dimension . Indeed its string-pair block is ; the image of is any vector killed by , a subspace of dimension (Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings, Nilpotent endomorphisms and their nilpotency index).
The trace form on is symmetric and invariant, and the degree grading is multiplicative: if and then , and for with (Trace forms are symmetric and invariant, Classical complex matrix Lie algebras).
The enveloping algebra and representations of (Universal enveloping algebra, Representations of Lie algebras).
Proof
Given: The pyramid data of the Definition.
The endomorphism acts on the box basis by and for boxes with ; hence the in one row form a Jordan string of length , because left shifts run from the rightmost box of the row to the first. Consequently is nilpotent of Jordan type , , and the number of columns is when the row list is nonempty, with for the empty row list. Zero-length rows contribute no Jordan strings; for all box-indexed sums and vector spaces are empty or zero.
Parabolic structure. The degree defines a -grading of the associative algebra: when by [F1], and . Hence is a subalgebra, its degree-zero part consists of the matrices with , which is exactly the block-diagonal subalgebra with blocks of sizes , so ; the strictly positive part is a nilpotent ideal and is the nilradical of the opposite parabolic, with .
The centralizer basis. First for boxes , with a term omitted when the relevant neighbour is absent (this is and , while and holds exactly for in the same row). Now write with the box of row in column and the box of row in column , the sum over with and ; here by the defining range, so this index set is exactly . Then where a term is omitted when the neighbour does not exist; shifting the second sum by and using (which exists exactly when ) shows that the two sums run over the same index set , because for every in the defining range one has ; hence the commutator is . The are linearly independent because they are sums over pairwise disjoint matrix units, and their number is , which equals by [F2]. Hence they form a basis of .
The bijection . For put , and . Because is rightmost, ; hence , because , and because . Thus , so the map lands in . The triple determines as the rightmost box of row and as the box of row in column , proving injectivity. Conversely, if , then gives , while gives . Thus those two boxes exist, their columns satisfy , and they give the required preimage. If either row has length zero, the index range in is empty, consistently with the absence of such a box pair.
The character. For one has by step 1.2, and , so and by [F3]. Hence , that is, is a Lie algebra character on : for , .
The good-grading conditions. By step 1.3, the centralizer has a homogeneous basis with , so it has no negative-degree part. The kernel of is , hence this map is injective for . The trace pairing is nondegenerate between and : each matrix unit pairs with , and matrix units of other total degree have zero trace. Invariance gives , so the transpose of the map on degree is, up to sign, . For 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 . They remain valid when , because all nonzero spaces then have degree zero.
The identity . Left shifts of run through the boxes of row in columns , and the corresponding left shifts of run through the boxes of row in columns ; all these exist because and the shifts stop while the row box exists. The pairs obtained are exactly the pairs with column difference and ranging over ; by step 2.1 these are exactly the pairs indexing . Hence the two finite sums coincide, and the two displayed families are the same basis of .
Dynkin normalization and the zero boundary. If , step 1.1 puts this nonzero element in pyramid degree , whereas the standard Dynkin grading defined by an -triple has and puts it in degree ; 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 -weights are and , so matrix units between these strings have odd weights. If , 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 , 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
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The numbering of boxes down columns from the left makes each row a Jordan string of ; this is why the row lengths (weakly increasing) are the Jordan block sizes, while the column heights are the ranks' increments and index the Levi blocks of .
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The shift counts the overlap of the two rows through the identity ; this count is used again in the loop-mode index sets of the finite W-algebra items.
The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations
Statement
Let , let be a -module, let be the natural module, and on use the operators and of Arakawa-Suzuki Casimir operators on tensor functors. Then:
- The operators commute with the -action and are natural in , and satisfy all the defining relations of the degenerate affine Hecke algebra The degenerate affine Hecke algebra: the Coxeter relations for the ; for ; and ; and the polynomial commutation .
- Consequently they define, via the generator-fixing anti-involution of the Hecke algebra, a natural right -action on commuting with the left -action.
The commutation of the is an independent check: it does not follow from the braid relations of the alone.
Facts & Assumptions
Given: , a -module with , the natural module , , and the operators of Arakawa-Suzuki Casimir operators on tensor functors built from the trace-form Casimir .
The operators for are the place permutations of the labelled tensor factors; , and commutes with when (Arakawa-Suzuki Casimir operators on tensor functors, Associativity of tensor products for compatible bimodules).
On two natural factors ; more generally, for any triple of factors the element identity holds in , and whenever the pairs of labels are disjoint (Arakawa-Suzuki Casimir operators on tensor functors, Classical complex matrix Lie algebras).
The Hecke algebra is presented by the Coxeter relations for the and the cross relations , , together with ; the generator-fixing anti-involution of is the anti-automorphism fixing all generators, and a left action of defines a right action by (The degenerate affine Hecke algebra).
The Casimir operator acts as an intertwiner and commutes with the -action; place permutations of natural factors also commute with the -action because the comultiplication is cocommutative (The Casimir operator is basis-independent and intertwining, Representations of Lie algebras).
Proof
Given: The operators and on , and the identities of [F1]-[F5].
The infinitesimal braid identities. For distinct labels one has : expanding and using [F3], the double commutator sum splits into terms and , and the two resulting sums cancel term by term after relabelling; equivalently, this is the identity in , which is the derivative of the invariance of under the diagonal adjoint action. Consequently . In particular, for three natural factors this is the identity for the flips.
The Coxeter relations for . is an involution; for because the pairs of interchanged labels are disjoint; and because both sides are the permutation operator inducing the same permutation of the three labelled factors.
Cross relations. Conjugation by interchanges the labels and in any operator supported on those factors, so and for . Therefore , and symmetrically . For , all labels in are disjoint from , so commutes with every summand. For , and the terms with commute with , while conjugation by interchanges and . Their sum is invariant, so again ; the two overlapping summands need not commute individually.
Polynomial commutation. Fix . Since and , the commutator is . The second sum reduces to the single term (all other are disjoint from the labels ), and the third sum vanishes (all pairs , are disjoint since ). In the fourth sum only the terms with or can fail to vanish, so it equals . Hence . The first bracket vanishes by step 1.1 with , , together with ; each summand of the second bracket vanishes by step 1.1 for the three distinct labels . Therefore .
Naturality, commutation with , and the right action. The place permutations are natural in and commute with ; the Casimir operators are intertwiners by [F5]; hence every and is natural and -linear. The relations established in steps 1.1, 1.2, 2.1 and 2.2 are exactly the defining relations of [F4], so the assignment , defines a left -action. The generator-fixing anti-automorphism of (which preserves each defining relation because the reversed cross relation is also a defining relation) converts it into a right action by ; the anti-automorphism property gives . This proves both assertions.
Remarks
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The two cross relations are not symmetric consequences of the braid relation: the summand has no counterpart in the Coxeter presentation of , and it is exactly the term responsible for the inhomogeneous filtration discussed in The degenerate affine Hecke algebra.
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The computation of step 2.2 uses only on pairs of natural factors; the identities involving the module label are the universal commutation identities of the Casimir element and hold for arbitrary .
The type-A finite W-algebra and the Whittaker category
Definition
Keep the type-A pyramid data of The type-A nilpotent pyramid, good grading and Whittaker character, with , transpose , and on . Let be the algebra automorphism with for all matrix units . Let be the kernel of the algebra homomorphism extending the Lie character , that is, the two-sided ideal generated by , (Universal enveloping algebra, Left, right and two-sided ideals, The ideal generated by a subset and principal ideals), and let be the left ideal it generates in .
The type-A finite W-algebra is It is a subalgebra of , and is a -bimodule with right action . This is a module quotient by a left ideal; no quotient-ring multiplication is imposed.
The Whittaker category is the category of -modules on which acts locally nilpotently for every (Representations of Lie algebras). For the Whittaker vectors form a -module with , and implies .
The verification below establishes the algebra and module structures just stated. The associated graded of the loop filtration on makes a filtered deformation of ; 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 of , the ideal of generated by and the left ideal of .
The grading is multiplicative, , , , and (The type-A nilpotent pyramid, good grading and Whittaker character).
Enveloping algebras: is the quotient of the tensor algebra by the two-sided ideal generated by ; a Lie character on a Lie subalgebra extends to an algebra homomorphism of the enveloping algebra, and is generated by (Universal enveloping algebra, Representations of Lie algebras, Classical complex matrix Lie algebras).
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 , the additive cosets form a ring with identity ).
Proof
Given: The pyramid data, the automorphism , the ideal and the left ideal .
Write . The scalar functional kills : a bracket can have a diagonal component only from , forcing equal columns and equal . Thus preserves brackets and extends to by the enveloping universal property; the negative scalar shift is its inverse.
Put . For and , . Since these shifted generators generate as a left ideal, . Hence for , , using this normalizer property for the first term and the left-ideal property for the second. Additivity, scalar closure and give a unital subalgebra.
Left multiplication makes a left module. Step 2.1 proves that is well defined for . Since , , and left multiplication commutes with this right action. Thus is the stated bimodule, with right-action homomorphism into .
is a -module. Let and . First, for every : this holds for by definition and extends to products by induction, since if then . Hence , because and every element of acts on by its -value, which is zero. Consequently , since a general element of is a sum of products with , , and . Now take , . Then , because by the definition of . Hence , and the map is bilinear and associative by the algebra structure of and step 1.1. Here the character and the parabolic data are those of [F1]. This verifies the module structure; the vanishing statement 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
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The dictionary is the type-A -shift of the source; it is the automorphism used (in the form ) on the deformed tensor space later on this page. The undoubled pyramid grading has in degree ; the doubled Gan-Ginzburg grading used for the Kazhdan filtration has in degree and vanishing degree part.
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The ideal is two-sided by construction: it is the kernel of an algebra homomorphism, and equivalently the two-sided ideal generated by the elements .
The regular coset-dominant Harish–Chandra tensor comparison
Statement
Assume the Axiom of Choice. Let , with upper-triangular Borel, and represent by coordinates of sum zero. For every with , require . Thus is regular and strictly decreasing inside each coordinate coset modulo ; there is no ordering of complex numbers from different cosets. Write for the weight lattice, , and for objects of genuine whose weights belong to .
Let consist of finitely generated -bimodules with and locally finite adjoint -action. For finite-dimensional let , with diagonal left action and ordinary right action. Then is an exact equivalence . Every object on either side has a finite presentation by the respective projective generators and . The induced map is the natural, composition-preserving identification The comparison commutes naturally with finite-dimensional tensoring.
For the corresponding statement uses and finite-dimensional modules with integral coordinate weights; 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].
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 (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).
Every simple is ; objects of have finite length, and subobjects and quotients remain in . For sufficiently large integers , is maximal in its linkage class and is projective with an epimorphism onto (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).
Finite-dimensional tensoring preserves and projectivity and gives a Verma flag with factors of multiplicity . 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).
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 is Noetherian then is Noetherian, Weyl's complete reducibility theorem).
For this weight , the action map is an algebra isomorphism (Duflo–Joseph g-finite endomorphisms of every Verma module).
Proof
In type A the integral reflections are precisely the transpositions of indices whose coordinates differ integrally. Thus is the product of symmetric groups on these coordinate cosets. For 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 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 . This makes greatest, in particular maximal, in its linkage class. By [F1], is projective in , and [F3] makes every projective.
Let be dominant integral and suppose is regular and decreasing within the original coset pattern. Put . The weight set of is Weyl stable: each simple-root decomposition has symmetric finite strings, and the reflections generate . For each weight , move it to a dominant weight . Highest-weight support gives , and dominance of gives . Thus . All weights of differ from by roots; their coordinate residues differ by the same common scalar. If a Verma factor in [F3]'s flag has central character , [F4] says its tensor weight is . Coordinatewise congruences force to preserve the original coset partition. For such , use the complex-bilinear extension of the Euclidean square (the weights themselves are real): The common complex scalar on every coset cancels. The second term is nonnegative by step 1.1 and dominance of , while the first is strictly positive for by regularity. The weight bound excludes these . For the highest weight occurs once. Exact central projection of the flag therefore yields precisely , a direct summand of .
The enveloping algebra 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 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 is abelian and is exact there.
For any simple in choose a sufficiently large even integer and set . The evenness puts in the root lattice in type A. Since , the weight is integral; its simple coroot pairings are those of plus , hence are nonnegative for large . The coordinate differences of inside each original coset become strictly positive in index order for large , since those of strictly decrease. The coordinate coset partition is unchanged, as elements of change residues by one common scalar. Enlarge further to satisfy [F2]'s reach bound. Step 1.2 makes a direct summand of , while [F2] gives an epimorphism . Composing the split projection gives an epimorphism from a finite-dimensional tensor of the fixed onto .
Choose finite bimodule generators of and take their finite-dimensional adjoint-stable span . It also generates as a right module: moving left generators to the right uses , with the adjoint term still in , followed by induction on PBW degree. Therefore is an epimorphism . A bimodule map from is uniquely determined by the adjoint-equivariant map ; conversely every such map extends by right multiplication. Hence , making projective by step 1.3. Present the kernel the same way to obtain a finite presentation of .
Devissage gives an epimorphism from one fixed-source tensor projective onto every object of . 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 by [F2], so a second such epimorphism presents . These arguments impose no central-character condition on .
Tensoring over is right exact, and canonically; using step 2.2's presentation shows that belongs to . For generator Hom spaces, step 2.2 gives . Ordinary finite-dimensional tensor-Hom adjunction gives the other Hom space as . 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 to its action on , exactly the map induced by ; evaluation and composition are preserved because this action is an algebra map.
For any , apply Hom from to a presentation . This yields a right exact sequence of Hom spaces by projectivity; apply Hom from 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 is an isomorphism. For arbitrary , its generator presentation identifies as the kernel of the map between the corresponding two Hom spaces; the same holds for . The just-proved identifications of those spaces identify their kernels. Therefore is fully faithful.
Step 3.1 presents any target object by tensor generators; step 3.2 uniquely lifts its presentation map to a map of the corresponding generators. Its cokernel maps to the given object by right exactness. Thus 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 , associativity identifies ; the identification is natural, and respects associativity, evaluation and composition on elementary tensors.
For , -semisimplicity and finite generation split any object into finitely many scalar -eigenspaces. Each is an object. The finite-dimensional integral-coordinate tensors are the finite-dimensional 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 and even ; then 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 , 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 central quotient, giving exactly the same action isomorphism. All preceding comparisons therefore retain integral coordinate shifts and the genuine scalar centre, proving the stated version. Choice is inherited from the projectivity and finite-length suppliers and from the semisimple module decompositions.
Vust's graded double centralizer for the type-A nilpotent centralizer
Statement
Assume the Axiom of Choice. Let be a finite-dimensional complex vector space, let be nilpotent with largest Jordan string length , let , and put . Let act on by the individual operators (in the -th tensor factor) and the place permutations, and let be the algebra map induced by the diagonal action of and the map encoding the right action. Then for every nilpotent Jordan type and every . If has at least Jordan strings of the maximum length , then is injective. For 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 with largest Jordan length , the algebra acting on by individual -operators and places, and .
is the full associative centralizer algebra, with multiplication given by composition. For a Jordan-string decomposition , with acting as , its block is , of dimension : a homomorphism is determined by the image of , which must be killed by . 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 it is , with nonzero radical . The invertible elements act diagonally on by (Nilpotent endomorphisms and their nilpotency index, Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings, Classical complex matrix Lie algebras).
Tensor matrix units identify with . Extending a basis of in each factor shows that commuting with every individual is exactly membership in . The place-fixed tensors are spanned by symmetrized pure tensors. For , the identity follows by expansion: any term missing a label cancels in the subset sum, and surviving terms use each label once. Thus is spanned by . For both spaces are .
Normality and covariants: the orbit closure of is normal with , and every -fixed endomorphism of is the value at of a -equivariant polynomial map with scalar invariant coefficients (Type-A nilpotent orbit closures are normal via chain varieties, Nilpotent-orbit tensor covariants extend and polarize).
The Hecke operators of Arakawa-Suzuki Casimir operators on tensor functors satisfy the relations of , and acts as the place permutation (The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations).
Proof
Given: The algebra , the truncated algebra , and the maps of the Statement.
The first centralizer. An operator commutes with the action of if and only if it commutes with the individual -operators and with the place permutations: the first condition says by [F2], and then the second says , which is spanned by the elements , . The image of under the diagonal representation is contained in : the diagonal action of commutes with the individual 's and with places. Conversely, for the element equals the product of its individual-position operators; For the commuting individual operators , put and . Formal differentiation and the geometric series for each factor give , so and . Each belongs to the enveloping image because is an associative algebra; here is the matrix power, regarded as an element of the Lie algebra . The recurrence therefore puts in that image. Hence and .
The second centralizer. An operator commutes with the diagonal -action if and only if it is -fixed, as follows. If is -fixed, commuting with for all but finitely many and comparing its linear coefficient gives . Conversely, if commutes with every , it commutes with for all . Newton identities express in these power sums, so commutes with , in particular for every unit . By [F3] every -fixed operator is for an equivariant polynomial covariant ; evaluating at replaces each by , which is a polynomial in the individual -operators of degree less than , so (the truncated algebra contains exactly the polynomials in each factor and the places). Conversely every element of commutes with the diagonal -action: for put ; each individual satisfies , and each place permutation satisfies . These operators generate , so their products and linear combinations also commute with every . Therefore .
Stable injectivity. Suppose has at least Jordan strings of the maximum length , with top vectors on distinct strings. The vectors with (where is the -th vector of the string) are distinct members of the Jordan tensor basis of ; applying the place permutations gives 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 -submodule isomorphic to the regular module (the basis vectors , , multiply exactly as the standard basis of the truncated polynomial/permutation algebra), so the right action is injective. For , , and both identities and injectivity reduce to scalar identities.
Remarks
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The identity is the stable-looking half and is proved without normality; the identity is the converse half where the covariant extension theorem is consumed, allowing arbitrary Jordan type and arbitrary .
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The full polynomial/permutation algebra has the same operator image, since each individual satisfies . Truncation removes this kernel; it does not alter either centralizer.
The shifted Yangian and the pyramid generators of the type-A finite W-algebra
Definition
Work over and fix together with a shift matrix of nonnegative integers satisfying whenever or , and . The shifted Yangian is the associative unital -algebra (Algebras over a commutative ring, central structure maps, and algebra homomorphisms) generated by the shifted Drinfeld generators (, ), (, ), and (, ). For , the higher-root coefficients have range and have range ; they are defined recursively by adjacent-root commutators, not declared as a duplicate independent family. Put , and . The defining relations are the following, for every index for which all displayed generators exist (in particular the and indices exceed their respective shifts):
For , . For impose
The higher roots are specified without new independent generators by , , and, for ,
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 has degree , and the loop filtration, in which it has degree ; their associated graded algebras are different (the canonical one is commutative polynomial, the loop one is a current algebra).
For the pyramid with conjugate (The type-A nilpotent pyramid, good grading and Whittaker character) the relevant shift matrix is for and for , and the type-A finite W-algebra is the quotient of by the two-sided ideal generated by the higher modes of beyond .
Write the Gauss decomposition of the generating matrix, with , , and no additional factor : the coefficient of is the mode . Its modes satisfy for , and in the finite quotient also for , so the finite quotient has the PBW basis of ordered monomials The auxiliary signed path polynomials used in the source to construct the Gauss generators are not all identified with these shifted -modes; the root of is the weight , and the surviving modes have loop leading term in the centralizer basis of the pyramid.
Facts & Assumptions
Given: , a shift matrix as above, the pyramid with row lengths and columns , and the generators and filtrations of the Definition.
The pyramid data: of Jordan type , the centralizer basis with , and the character ; the finite W-algebra is generated by -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).
The RTT presentation: the ordinary Yangian RTT algebra is generated by the matrix coefficients with the RTT relation and ; 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).
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 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
Given: The abstract RTT/shifted Drinfeld data, the original pyramid shift, and the local well-definedness constructions of [F3].
Ranges and shift arithmetic. The monotone shift identities hold by telescoping on increasing indices and by zero lower shifts on decreasing indices. The adjacent positive generators have threshold , the adjacent negative generators threshold , and their higher-root commutator recursions give respectively and . Thus for the asymmetric original pyramid an upper coefficient begins after whereas its lower counterpart begins at mode ; these are distinct ranges. The formal Gauss coefficients are computed by triangular inversion with diagonal constant term .
Infinite filtrations. The RTT relation lowers canonical degree under a commutator, and its degree- 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.
Finite quotient and actual reduction. By [F3], the actual signed path images satisfy the shifted coefficient relations and for . 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 coefficient induction gives zero below the shift and above , and the finite Gauss-to- coordinate change gives the ordered surviving -monomial basis. This uses finite spanning and independent reduction images; restriction of an infinite PBW basis to a quotient would not prove independence. Only is directly truncated: higher diagonal Gauss coefficients remain polynomial expressions.
Weights and actual loop symbols. The path of canonical degree with matrix factors has good degree at most , so only its single-factor part contributes in loop degree . It is , of row weight . 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 coefficients. For the upper threshold is , so the first upper coefficient is with symbol ; the corresponding lower threshold is . This verifies the unrescaled coefficient convention and the asymmetric range.
Remarks
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The index convention is deliberately unshifted: the coefficient of is , no power of is inserted, and the filtrations only change the assignation of degrees. Rescaling the series by would shift the ranges and is not used anywhere on this page.
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The finite quotient keeps the higher diagonal modes as polynomial expressions rather than setting them to zero; only the modes with are truncated.
Gan-Ginzburg and Skryabin inputs for the type-A pyramid good grading
Statement
Keep the pyramid data of The type-A nilpotent pyramid, good grading and Whittaker character and the finite W-algebra , the bimodule and the Whittaker category of The type-A finite W-algebra and the Whittaker category. Double the pyramid grading by declaring the degree of to be ; then has degree and the degree part of is zero. Let in the doubled grading (the strictly negative even part), carrying the character . Then:
- There is a homogeneous transverse complement for a suitable , and the conjugation map , , is a polynomial isomorphism; the Kazhdan associated graded of is and .
- Assuming the Axiom of Choice The Axiom of Choice, for every -module , the twisted -cohomology of vanishes in positive degree and its degree-zero part is .
- Every nonzero module on which all , , act locally nilpotently has a nonzero simultaneous invariant vector; in particular implies for in the Whittaker category.
These assertions use the doubled good grading; no nondegenerate alternating form on the original degree space is asserted.
Facts & Assumptions
Given: The pyramid data, the doubled grading , the subspaces in the doubled grading, the ideals , and the bimodule , and the finite W-algebra . For assertion (2), assume the Axiom of Choice The Axiom of Choice; assertions (1) and (3) do not require it.
In the doubled grading the only nonzero even degrees occur, has degree , and consist of even degrees only, and the string computation of the pyramid gives for an -triple adapted to the grading (The type-A nilpotent pyramid, good grading and Whittaker character, Classical complex matrix Lie algebras).
Chevalley-Eilenberg theory: the -cohomology of a module is computed by the Chevalley-Eilenberg complex, is the space of invariants, and a short exact sequence of -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).
PBW orders the nonnegative-degree algebra before and replaces the rightmost generators by their character in . The resulting Kazhdan filtration is exhaustive, separated and bounded below; its symbols are polynomial functions on . The twisted 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 as finitely supported coefficient families on monomials).
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
Given: The doubled grading, the transverse slice and the bimodule ; assume AC for assertion (2), as in [F4].
Positive-weight transverse product. Choose the usual rowwise triple. On the strings have highest -weight , . Since the pyramid grading element differs from by row scalars, their highest and lowest grading weights are and . Thus the negative-degree part is injected by and gives the direct-sum complement of [F1]. The differential of at is , an isomorphism. Use weight on and weight on the translated slice and target coordinates; these are positive. In homogeneous coordinates of increasing weight, each component of 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.
Detection. The shifted operators form a representation of the nilpotent Lie algebra , because 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 therefore gives a common nonzero invariant. The case is immediate.
The actual graded complex. PBW and [F3] give , with no additional symbol factor. Step 1.1 identifies this with . 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 vector weight makes the twisted Chevalley–Eilenberg differential filtration preserving. Its graded complex is the polynomial de Rham complex of , tensored with : 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 , is a contracting homotopy; constants are the only surviving degree-zero classes.
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 and , since by the defining invariant realization. Using the fixed PBW vector-space identification , take homogeneous coordinate representatives in and form their ordered products there before projecting to . This never multiplies abstract classes in a left-ideal quotient. Their projected ordered monomials, acted on by the right bimodule action, span by finite descending leading-term subtraction. A finite relation among them would give a relation between distinct monomials over ; independence of polynomial monomials rules this out. Thus is right -free. All statements include the independent scalar coordinate of .
Transfer to every module without graded-flatness assumptions. The finite augmented cochain complex , where , is exact by step 3.1 and is a complex of right -modules. Its differentials are right -linear because the right action commutes with the twisted left action. Each term is right -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 . These splittings supply a right -linear contraction of the augmented complex. Tensor the contraction with an arbitrary left -module . This remains a contraction, and the resulting complex is exactly the twisted Chevalley–Eilenberg complex of . Consequently its positive cohomology vanishes and its degree-zero cohomology is via . No filtration or flatness of is assumed. The splittings use exactly [F4].
The preceding steps prove the three assertions with the doubled even grading. In particular there is no degree symplectic or Clifford contribution. If , then and the product, augmentation and all cohomology identities reduce to their degree-zero identities.
Remarks
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The role of the doubling is to put the contracting -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.
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The detection statement is the categorical form of Skryabin's theorem used to identify Whittaker vectors: for in the Whittaker category, loses nothing.
Ordered monomial PBW basis for the shifted Yangian
Statement
For any fixed order on the family (), (, ), and (, ), with each root mode included once, their ordered monomials form a -basis of . 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 ; the two graded algebras are different and non-isomorphic in general. In the finite quotient the ordered monomials in the finite Gauss range form a basis. The Kazhdan/canonical associated graded is commutative, whereas the loop associated graded is noncommutative when is nonabelian and commutative when is abelian. These degree assignments are and , respectively; no unconditional noncommutativity or non-isomorphism is asserted. Equivalently, the finite -coefficients with form an ordered PBW basis, where is the unshifted coefficient index of , not a reindexed value.
Facts & Assumptions
Given: A shift matrix attached to a pyramid with row lengths , the shifted Yangian with its generators and filtrations of The shifted Yangian and the pyramid generators of the type-A finite W-algebra, and the quotient .
The RTT/Drinfeld presentation, the Gauss decomposition , 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 with .
Ordered monomial PBW for enveloping algebras of finite-dimensional Lie algebras: an ordered monomial basis holds for when is finite-dimensional (PBW gives an ordered monomial basis for the enveloping algebra).
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 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
Given: The shifted Yangian generators and the finite quotient .
RTT spanning and the actual coproduct. In the unshifted RTT algebra the commutator of modes has canonical degree at most , so induction on total degree and the number of unordered pairs rewrites every word into ordered monomials. Matrix-unit brackets verify RTT for in the th factor of . 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 . More generally shifted evaluation points give the ordered product , in increasing factor order. Its coefficient when all is , homogeneous of enveloping PBW degree .
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, and . The negative PBW projection applies χ to the right factor. Its elementary rules are and for a negative matrix unit Z and a p-factor B. The bracket is , and at adjacent negative columns, zero at greater distance. Define as the sum of products with total degree , 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 times one minus for every intervening row at most x. Its image replaces each factor by . Equivalently, in the factors its only external sign is one minus for every intervening row at most x, since their product already contributes . Invariance means . If an element B is invariant, then proves ; hence invariant elements form a subalgebra, and products, commutators and coefficients of inverse series with identity constant are invariant.
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, reverse products, and let S on the reflected space be diagonal with . The linear map is a Lie isomorphism, because . It preserves grading degrees, p and m, and the trace pairing. The diagonal-conjugation sign on every positive adjacent arrow is −1, so and . It extends to an ALGEBRA isomorphism of enveloping algebras and takes to . Thus it takes the entire untwisted left reduction to : each defining commutator condition is equivalent under φ. The chart map is the explicit algebra isomorphism . Scalar translations have smaller positive Kazhdan degree, so . 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.
Index and inverse sign in the abstract quotient. Write , so , while the defining relation uses with constant . Thus . Put , , , , . Then and . We use this only for , so is an allowed but HIGH E mode, to be eliminated before the diagonal formula is used. Also , 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.
Product Jacobian and independence. Let be at least the largest coefficient index in a proposed relation. In the commutative symbol algebra of write . At , with nonzero pairwise distinct , the differential on every matrix entry is . The column coefficient polynomials are linearly independent, since evaluating at leaves only column , 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 , , 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 are scalar-matrix points in the symbol space, independently of spectral evaluation parameters.
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, and , the right end recursions, for any fixed bottom row h, are , , and . 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, and , its LEFT recursions are , , and , 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.
Finite spanning: earlier blocks and boundary E/F. In the abstract quotient by , , let contain D modes , , E roots , , and F roots , ; let be their algebra. Induct on c to show every allowed mode with endpoints at most c belongs to with total canonical degree at most its index. The case c=1 is the imposed truncation, including . For the inductive step put and . For , the D–E relation gives . 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 with in the only nonzero diagonal block, hence new E indices at most . An earlier finite root gives and any block-refinement split terms, all with . Earlier negative roots and earlier positive roots without endpoint commute with the lowest boundary E. Thus the expanded commutator is in . In the sum , 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 .
Loop symbols and shifted PBW. Give an RTT mode of index loop degree . 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 . This identifies the loop graded algebra with . The required current-algebra PBW uses only [F2]: any finite relation among ordered current monomials maps to a jet quotient with 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 only by products of at least two positive-index modes with total index , whose loop degree is at most . 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 with , giving ; the reversed lower recursion gives 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 for modes of indices ; 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 , the adjacent relation gives , 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.
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.
Higher roots and the final diagonal elimination. For , the defining root recursions are and . Reduce the earlier endpoint factors by the c−1 hypothesis; the same Leibniz bounds in step 2.3 place every new root in , including high modes, using the finite allowed new roots in . Now use step 1.4 for , . Every inverse earlier coefficient is in and every has smaller index, so induction on r treats its sum. First replace the upper 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 , so its E–F convolution has only indices at most . 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 mode. Thus this commutator uses only indices at most , and the induction closes with the asserted degree control. In particular higher diagonal modes are polynomial expressions, not zero modes.
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 , f bottom and g arbitrary. In D^(2), and in boundary E^(2) when the shift is1, the single bridge contributes scalar . The bottom plus paths contribute and matrix terms for g bottom. The shorter minus paths in B contribute and 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 . In LEFT deletion put , f arbitrary and g bottom. The bridge scalar is ; bottom plus paths give and for f bottom. Shorter minus paths give 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 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.
For a larger boundary shift, or a rectangle, the first two end columns have equal height t. A double dot deletes both and ; replacing K with the corresponding boundary in RIGHT deletion or in LEFT deletion gives the same calculation. In RIGHT deletion call the last positions C,B,A, and write , , , and . Twice expanding step 2.2 expresses the changed r-mode as the sum of eight groups , , , , , , , . For their projected brackets, in that order, are , where and . 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 . K lies in the twice-deleted p and commutes with z. The eight expressions cancel for EVERY r>1.
At a RIGHT jump-one boundary, for a fixed earlier-block row g and r>1 the coefficient recursions in U(p) are and . Here , with order-zero coefficient −I. The corresponding LEFT identities are and . These are algebraic coefficient identities, independent of invariance and generation. Expanding the E identity by the right end recursion gives , its product with L, and its commutator with C; collecting with step 2.2 gives . The left F expansion instead gives , its LEFT product with L and , which collect to . 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 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.
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 , , , , . The eight groups are , , , , , , , . For their projected brackets are , with and . For example , and moving this negative through B gives ; 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 ; the F/H terms cancel because 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.
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 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.
Finite Levi Jacobian. Project to its column Levi enveloping algebra and take canonical symbols. At its diagonal point , let . The diagonal D first variations are . For , set , . A first variation in a common column 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 and 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 and , , are respectively and . For higher roots, the canonical symbol of the adjacent root commutator is the Levi Lie–Poisson bracket. At 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 and , the coefficients from and multiply to when , since . For F the reversed recursion uses , with coefficients one and . Thus induction gives the displayed first variations for all higher roots as well. Choose the 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 . 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.
The whole reduction is generated. Write for the entire quantum Hamiltonian reduction, before any identification with a Yangian quotient. By [F3] its homogeneous Hilbert series is . Each weight is positive, so every coefficient is finite. Step 6.1 places every ordered finite-generator monomial of total degree at most inside . 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 , which is also by [F3] for the original pair and step 1.3 for the reflected pair. Thus their span equals for every . 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.
Relations, finite order and the whole-algebra identification. The end path identities prove the shifted coefficient relations and the 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 , , and ; 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 . 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 . Thus the smallest-row path has no coefficient above , giving the actual 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 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.
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 to . Each displacement is unchanged. A reversed join compares with , so its strict-forward or weak-reverse rule is exactly the original one; its row is , 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 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 , rather than only the image of a path subalgebra.
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.
Actual original prefix coefficient identity. Let be the first m columns of the decreasing-column pyramid, the ordinary UNSHIFTED box embedding, and the box in row j and column a when it exists. Put negative-index coefficients zero and . The original coefficient recursion, for r>0, is , where coefficients inside I belong to and shifts in the sum belong to . The final THREE terms are omitted for , 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 . The precise smaller-block subtraction is , all in the smaller diagram. For a shorter block c and last block b, . Insert these expressions into . Unchanged terms give the first embedded T; the subtractions group by shorter terminal row h into the product with split ; 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.
The two graded algebras. The shifted root relations give the current brackets on the allowed modes , ; shift additivity makes their span a Lie subalgebra. Step 3.1 identifies its ordered enveloping basis with the intrinsic loop-filtered basis, proving . 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 ; 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.
Every coefficient above the bound is zero. For the original decreasing-column diagram 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 , its row length is unchanged on removal, so the only embedded T term vanishes for by induction. If j is a bottom row, , and the first embedded T vanishes for because its smaller target-row length is m−1. In each shorter-row product, is unchanged and , so for ANY i, killing its first factor. In the Levi sum every h has smaller row length m−1, and kills its coefficient. The same inequality kills the T coefficient inside the final commutator. This covers every term, including the boundary , and proves for . The lower zero range follows coefficientwise from FDE and shift additivity. No truncation fact was assumed to prove itself.
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 . 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.
Put . This and ηtail are algebra automorphisms: a matrix bracket can have diagonal part only from , which forces equal columns and equal diagonal shifts, so the scalar functional kills the commutator; the negative scalar translation is the inverse. Reflection gives , hence . Also , by the trace calculation, and , since τ reverses products and sends each shifted negative generator to its reflected one. Therefore . 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 . The induced Gauss transpose also satisfies : apply the coefficientwise reversed FDE factors and their Gauss cut identities. Thus step 11.2 gives the reflected upper cutoff , 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 .
Write and . The identities and prove and for every w∈W. Thus has its actual right action , and its actual left action , commuting with the respective enveloping actions by associativity. These are module quotients, not quotient rings. Right Whittaker vectors act by because they annihilate J_R. Turning a right U(g)-module into a left reflected module by identifies its right Whittaker space and W action with the reflected left ones, using . 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 ; 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
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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.
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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.
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 , , and be as in The type-A finite W-algebra and the Whittaker category. Then the functor is an equivalence of categories, with inverse the Whittaker-vector functor ; in particular is exact and implies for .
For every finite-dimensional -module , the exact functor transports to the exact functor on -mod, and whenever is a -module viewed as a -module by restriction, the natural map is an isomorphism of -modules. The associativity isomorphisms are compatible, and for the one-dimensional -module the resulting isomorphism is independent of the order of the composed associativity isomorphisms.
Facts & Assumptions
Given: The pyramid data, the bimodule and the Whittaker category of The type-A finite W-algebra and the Whittaker category, and a finite-dimensional -module . Assume AC The Axiom of Choice for the arbitrary-module equivalence and transported tensor assertions.
For every -module , the twisted -cohomology of vanishes in positive degrees and its degree-zero part is ; for the invariants detect vanishing (Gan-Ginzburg and Skryabin inputs for the type-A pyramid good grading).
is a -bimodule, and tensoring the canonical element with a -module gives a left adjoint to ; the unit and counit are the natural maps , and , (The type-A finite W-algebra and the Whittaker category, Universal enveloping algebra).
Chevalley-Eilenberg exactness: tensoring with a finite-dimensional -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).
Finite-dimensional -modules have finite -flags with trivial successive sections. Indeed the column-grading diagonal element satisfies on ; negative homogeneous generators shift its finitely many generalized eigenvalues by negative integers. Sufficiently long products from therefore vanish. Induction on the module dimension, choosing a vector in the common kernel and passing to the quotient, gives with (The type-A nilpotent pyramid, good grading and Whittaker character, Classical complex matrix Lie algebras).
Proof
Given: The bimodule , a -module , a finite-dimensional -module , and the maps ; assume AC as specified above.
Unit, membership and counit. The shifted action on lowers the bounded-below Kazhdan filtration: , and for negative doubled degree the commutator lowers filtration by . This proves local nilpotence on too, so the adjunction lands in . By [F1], its unit is an isomorphism. For , the triangle identity makes an isomorphism. Left exactness gives , hence by detection. Now the short exact sequence with this injective counit has of its domain zero by [F1]; its cohomology sequence gives . Detection makes that cokernel zero. Thus the unit and counit are isomorphisms, proving the equivalence without presuming exactness of .
Exactness and detection. Exactness of follows because it is inverse to the exact functor (tensoring with the right-free module proved in the local cohomology supplier [F1]), and the detection statement is the case of [F1].
The transported tensor functor. For -mod and finite-dimensional , the functor is exact in because the composed functors are exact; it is the transport of across the equivalence.
Invertibility of the displayed tensor map. Let be a -module and put . PBW gives representatives , and is balanced because right multiplication by changes to . Hence is a defined linear map. Use [F4]'s finite flag of . Each quotient of by is a finite direct sum of , with trivial action on its finite factor. By [F1] it has vanishing positive twisted cohomology and invariants . Induction and the long exact sequence give the same vanishing on each , and give short exact sequences on their invariant spaces. The map preserves these filtrations. On each successive quotient, the invariants are represented by and sends them to . Thus its quotient maps are identities; induction through the finite short exact sequences makes bijective. This argument holds for arbitrary and needs no cofree realization or completion of .
Associativity. The associativity isomorphisms of the transported functor are obtained by inserting the canonical associativity isomorphisms of the tensor product of -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 .
Balancing and -linearity. PBW gives unique representatives , , in . Define . Since the right action of sends this representative to , the formula is right--balanced: . Moreover for . The shift adds a Lie character on , so on its primitive generators, and hence multiplicatively on , . The action on the source Whittaker subspace is therefore , while the target restricted -module has action . Applying to the displayed coproduct identity proves . Together with step 2.1 this proves the actual stated -module isomorphism. No equality with cofree evaluation or citation-only character-equation argument is used.
Independence of the order. For the isomorphism is the composite of the single-step maps ; 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 ; coassociativity and the displayed shift identity make these maps equal. Therefore the resulting isomorphism is independent of the composed associativity isomorphisms.
Remarks
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The displayed tensor map is the balanced -module evaluation map. Its invertibility follows from the finite -flag and cohomology sequence in step 2.1; no identification with constant evaluation in a cofree model is required.
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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 of a single block, treated later.
The loop filtration on the type-A finite W-algebra has associated graded U(g^e)
Statement
Equip with the loop (good) filtration induced by the pyramid grading 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 is canonically isomorphic to the enveloping algebra , viewed as a graded algebra via the restriction of the pyramid grading, and the isomorphism sends the leading symbol of the generator to , where the are the centralizer basis of the pyramid. In particular is a filtered deformation of , the loop filtration is separated, and the ordered monomials in the generators , , form a basis of .
This filtration is not the Kazhdan filtration: the Kazhdan filtration has associated graded the commutative Slodowy-slice algebra , while here is noncommutative in general.
Facts & Assumptions
Given: The pyramid , the finite W-algebra with its generators and loop filtration, and the centralizer basis , .
The ordered monomials in the finite -modes form a PBW basis of , and the loop degree of is (Ordered monomial PBW basis for the shifted Yangian, The shifted Yangian and the pyramid generators of the type-A finite W-algebra).
The leading symbol of in the loop filtration is ; the elements with form a basis of the centralizer 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).
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).
The Kazhdan filtration of the Gan-Ginzburg construction has associated graded the commutative coordinate ring of the Slodowy slice, not the enveloping algebra of (Ordered monomial PBW basis for the shifted Yangian).
Proof
Given: The PBW basis and leading-symbol data of [F1]-[F2].
Actual ambient leading term. Give a matrix unit its good degree . In the explicit signed path formula a term of canonical degree with matrix-unit factors has good degree at most ; a diagonal scalar replacement only lowers that degree. Therefore only single-factor terms contribute in good degree . Those terms sum to over , , , namely . Products introduced by Gauss factorization or its inverse have at least two factors and have smaller good degree. Thus the leading homogeneous component of in the actual graded algebra is exactly . This proves the leading-symbol claim using the path degrees rather than a claim that Gauss inversion alone supplies its sign.
Independence in the ambient enveloping algebra. The elements form a homogeneous basis of the actual Lie subalgebra . Extend that finite basis to a homogeneous basis of , with an order extending the prescribed order of the centralizer basis. Enveloping PBW implies that the ordered monomials in the are linearly independent in , and that the natural homomorphism 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.
Strictness of the loop basis. The finite monomials form a vector-space basis of by [F1]. For a monomial with total loop degree , step 1.1 says that its degree- homogeneous component in is, up to the product of its displayed signs, the corresponding PBW monomial in . In any nonzero finite linear combination of monomials, take the largest total loop degree . The degree- homogeneous component is nonzero by step 1.2, even when degree-zero generators occur. Thus that combination belongs to and not to . Consequently the intersection filtration in the Statement is exactly the span of monomials of total loop degree at most , and their degree- symbols form a basis of its associated graded. This verifies symbol independence directly, rather than inferring it from independence of filtered elements.
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 is zero it already lies in filtration , and multiplication agrees with multiplication of homogeneous components. Apply this to . Step 2.1 identifies its image with the span of the ordered monomials in , which is precisely the embedded algebra from step 1.2. Hence , and the identification sends the symbol of to as asserted.
Filtration and the second graded algebra. Each generator has finite nonnegative good degree, and each element is a finite sum of monomials, so the loop filtration is exhaustive and bounded below with . The actual homogeneous decomposition in 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 on and has associated graded by [F4]; in the doubled convention its weights are twice these. That graded algebra is commutative, whereas is noncommutative whenever is nonabelian. These are the two claimed filtrations and their respective graded algebras.
Remarks
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The index shift is part of the statement: the generator with loop degree is , and its symbol is . The coefficient index of the source series is , and no additional rescaling is applied.
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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.
The degenerate cyclotomic Hecke algebra
Definition
Let be the degenerate affine Hecke algebra of The degenerate affine Hecke algebra and let be a multiset of complex numbers, . The degenerate cyclotomic Hecke algebra is for , and for is the quotient 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 , the additive cosets form a ring with identity ).
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 used on this page. A -basis is given by the ordered monomials so that ; the polynomial-degree filtration has associated graded the algebra . For integral roots this is the cyclotomic quotient attached to the dominant weight of the integer type-A root system, with ; for general complex roots one uses a separate integer chain in each coset of , and the symbol 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 for the origin and the pyramid columns . If , then in the quotient. The generator-fixing anti-involution of descends to . The top coefficient functional of the monomial basis is a nondegenerate symmetric trace on , and it restricts to a nondegenerate trace on every central block corner.
Facts & Assumptions
Given: The degenerate affine Hecke algebra , a multiset of arbitrary complex numbers with , and its quotient , where and the ideal is two-sided. Assume AC The Axiom of Choice for the Skryabin/tensor realization used in PBW independence.
The affine ordered monomials form a basis, commute, and the cross relations are and . Its generator-fixing anti-involution exists (The degenerate affine Hecke algebra).
The pyramid construction provides and the automorphism . The Whittaker bimodule is with right -action by . PBW identifies it as a vector space with (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).
For any -module and finite-dimensional -module , the tensor-isomorphism of Skryabin's equivalence for the type-A Whittaker pair identifies with by . These identifications are natural and compatible with tensor associativity. No cyclotomic quotient is part of this input.
The Casimir operators on satisfy the affine Hecke relations, commute with , and therefore restrict to Whittaker vectors; their naturality transports them through F3 (The Casimir and place-permutation operators satisfy the degenerate affine Hecke relations).
Filtered leading symbols multiply in the associated graded (Associated graded algebra of a filtered algebra).
Proof
Given: , the polynomial-degree filtration, and F1–F5; assume AC for F3 and the transported representation.
Bounded spanning in every variable. For each , put (and ). In the affine algebra the cross relations give terms of polynomial degree zero. Hence terms of degree at most . This element is zero in . Every affine ordered monomial with an exponent at least can therefore have a factor 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 with . The same induction proves that is spanned by bounded monomials of degree at most .
A realization for arbitrary complex roots. For choose an integer and the rectangular partition with rows, so every column has height and has strings of length . On define the one-dimensional module by . This is a Lie character: it vanishes on the strictly positive nilradical and is times the trace on the th Levi block. In particular no integrality or coset condition on is needed. Restrict this module to and use F3 with . Restrict the affine Hecke operators on to Whittaker vectors, then transport through F3. This defines an affine Hecke action on ; the are place permutations. The following step computes before asserting any quotient factorization.
The transported first operator. Write and define by . It is well defined: the right -relations become multiplication by the restricted character, and PBW gives representatives . For a tensor basis vector write its unique Whittaker preimage under F3 as , with . Then . If , then and , since . If , the Whittaker equation for instead gives , where runs over tensors obtained from by replacing an occurrence of by . Apply to . The terms with give . The term gives , because exactly when . In the negative sum, replacing the first occurrence gives ; replacing an occurrence in position gives exactly when . Consequently the transported right action is Here a nonexistent left-shift term is zero. In our rectangle , so the diagonal coefficient is precisely .
The cyclotomic relation and the leading symbols. Let be the span of tensors whose first entry has column at most , with . Step 1.3 gives : both the left shift and every exchange strictly lower the first column, while preserves . Thus successively applying kills . The factors commute, so and the action factors through . Grade by 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 . The recursion shows by induction that all are filtered of degree one with leading symbol , and that have degree zero with symbols the place permutations.
Independence and the associated graded algebra. The cross relations and the conjugated relations in step 1.1 give a surjection . Its composite with the associated graded tensor representation is , place permutation. Choose the rightmost box in each of distinct rows and let be the tensor of those boxes. For bounded and , the vectors are distinct tensor basis vectors: their row labels identify the permutation, and their columns identify all . Therefore this composite is injective. It follows that . 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 . The longest strings have length , the number of columns, and there are of them; no column height is used as their length. For the algebra, basis and associated graded are all , so the assertions hold directly.
Integral roots and the pyramid dictionary. For integral roots write ; then , the quotient attached to . For arbitrary complex roots the same algebraic definition applies, with integer-chain bookkeeping separately in each coset of . The rectangle above has and , hence ; 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.
Level one and the anti-involution. For , and give by induction; the basis of step 3.1 identifies the quotient with . The generator-fixing anti-involution fixes and preserves its two-sided ideal, so descends to .
The graded top pairing. Put and . Let be the coefficient of . For graded monomials , this coefficient is one exactly when and , and is zero otherwise. The equivalent reversed condition is and ; thus is symmetric. Each basis element pairs with its unique complementary element, so the pairing is perfect, including between degrees and . Define as the coefficient of in the PBW basis. By filtration compatibility on , and it vanishes on . Therefore, if and , then . This establishes cyclicity only under the stated degree bound so far.
Full generator cyclicity. Since permutations have degree zero, step 4.3 gives for every , . To check for all bounded basis monomials , step 4.3 suffices when . The remaining ones are exactly . The polynomial is central: it commutes with the , and the cross relations directly give , while commutes with the other variables. Hence . Applying the already proved permutation cyclicity twice gives . This proves cyclicity with every generator on every element; successively moving generators of a word from the beginning to the end proves for all . It also covers (where and ).
Nondegeneracy and block restriction. For , take its largest filtration degree , so . By the perfect graded pairing of step 4.3 choose homogeneous with , and lift it to . Then . 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 is a central idempotent and , choose as above; then , so the restriction to is nondegenerate and symmetric as well.
Remarks
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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.
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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.
The deformed tensor space for the type-A finite W-algebra
Definition
Fix the pyramid with columns , its box-labelled natural module , an arbitrary origin , and . Assume AC The Axiom of Choice for the imported Skryabin and Vust inputs. For define the column-trace character where is its th column-Levi diagonal block. Write for the resulting automorphism of , so . Let be the corresponding one-dimensional -module and set and , with a separate integer chain for each complex coset as in The degenerate cyclotomic Hecke algebra.
The truncated (deformed) tensor space is with the left -action obtained by composing the ordinary total tensor representation with . Equivalently it is , with one character factor; the origin twist is applied once to the total action. For its right -action is determined by place permutations and with . Here the generator-fixing anti-involution of the Hecke algebra converts the displayed operators into a right action. For there are no , , and .
Grade the box basis by , use the total tensor grading and its induced endomorphism filtration, and use the fixed loop chart of The loop filtration on the type-A finite W-algebra has associated graded U(g^e): , . The coefficient index remains the actual unshifted 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 Consequently the full graded left representation in this fixed chart is where acts in tensor position . In particular its complete mode-symbol dictionary is where is the restricted -action. On the right, and is the place permutation. Thus the graded bimodule is the character-twisted Vust module , 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 ; full -commutation is not asserted. They make a filtered -bimodule. The actual balanced Skryabin map gives a coherent isomorphism of -bimodules. For every complex origin, every pyramid and every , 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, , use and . For all structures are scalar; for , and the empty cyclotomic product is , 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 -index convention, arbitrary , , and the left and right operators in the Definition. Assume AC for the imported equivalence and Vust theorem.
The pyramid gives , , , and over row pair and column displacement ; the bijection retains the physical box labels (The type-A nilpotent pyramid, good grading and Whittaker character).
The finite model uses with . The canonical loop chart is the inclusion identified with , and its mode symbols are , without a 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).
For a -module , Skryabin supplies the actual balanced -linear tensor map , its triangular inverse and coherent associativity. On the ambient genuine -module the trace-form Casimir and places are natural intertwiners satisfying the affine Hecke relations; restriction to Whittaker vectors therefore transports these operators as -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).
The cyclotomic quotient for arbitrary complex roots has its bounded monomial basis and polynomial filtration, with graded algebra ; the generator-fixing anti-involution descends (The degenerate cyclotomic Hecke algebra).
On the untwisted tensor space , the unital image and the operator image of 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
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.
The column-trace function kills : 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 respects Lie brackets and extends to the unital automorphism of , with inverse . It preserves the column grading, since only degree-zero generators receive degree-zero scalars. The coproduct gives , exactly the action on ; no factor multiplies the character. Its restriction to is the stated filtered left action.
Use the actual isomorphism of F3, composed with coherent transported associativity, to identify with . The left action is the one in step 1.1, because the balanced map intertwines on Whittaker vectors with on the target. Indeed and the evaluation map obeys . The ambient universal operators and preserve the Whittaker subspace and commute with its -action; transporting them through this actual map gives a right Hecke action commuting with . Naturality transports the places to ordinary tensor permutations. This argument makes no claim about commutation with the full target -action.
Each has degree . If it contains no diagonal matrix units; if it contains diagonal matrix units only when , and then precisely one in each column . Consequently . Since , the character of step 1.1 restricts to a Lie character on . Thus restricts to the graded unital automorphism of , , with inverse . No assertion that preserves is needed.
To compute the transported , write and . The evaluation is balanced by F3. For a tensor basis vector , write its actual Whittaker preimage as ; then . For , . For , the actual Whittaker equation instead reads . These two identities compute every coefficient of .
The fixed loop chart F2 identifies the graded inclusion of in with the ordinary inclusion of . The ordinary tensor representation and are graded maps. Therefore taking symbols of their restriction gives . This is equality of the full graded representation, not merely equality of its image. It proves and the complete displayed symbol dictionary. The term survives in degree zero; for positive degree it is absent. The coefficient index, sign , finite -range and physical box labels are unchanged.
In that computation the nonnegative-column terms give . The character terms from negative matrices give , since exactly when . In the remaining negative sum, replacement in the first tensor position gives , and replacement in position gives exactly when . Adding yields , precisely the matrix-unit display in the Definition. A nonexistent left neighbour contributes zero. Recursion with the place permutations gives all higher , 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.
For and , let be the span of tensors whose first box has column at most . The preceding formula preserves every and gives . Successively applying the factors from column down to column kills ; they are polynomials in one operator and commute, so . This proves the quotient factorization directly for arbitrary complex origins, including repeated roots. In the total grading , the left-shift part has degree one; the diagonal part and each two-position exchange have total degree zero. Hence . Since the longest Jordan string has length , for on this nonzero tensor space. A monic annihilating polynomial of degree would have that nonzero degree- symbol. Therefore the displayed degree- polynomial is the exact minimal polynomial, consistent with F4.
The right action is filtered with of degree one and places of degree zero: this holds for by step 5.1 and for each by . Taking degree-one symbols gives ; the extra has degree zero. By F4 the resulting graded right map is the ordinary map , on . Together with step 3.2 this identifies the entire graded bimodule with the character-twisted Vust module in the Definition.
Since is an automorphism, as unital graded subalgebras of . 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, and the unchanged right image are mutual centralizers. This proves the required Vust comparison without identifying the two fixed-chart modules.
Let and be the algebra of right Hecke operators, with filtrations induced from . They commute by step 2.1. The symbol maps in steps 3.2 and 6.1 have images , respectively, which are contained in . For any commuting filtered operator algebras, taking the largest homogeneous terms of a commutator gives the inclusions , where denotes the commutant in the relevant endomorphism algebra. Therefore . The same argument with interchanged gives . Every inclusion is equality. This also proves strict equality of the graded image algebras, rather than presuming that an arbitrary filtered representation is strict.
Since and their induced associated graded spaces agree by step 8.1, a member of can have its leading homogeneous term matched by a member of of the same filtration degree. Subtraction lowers the integer degree. The finite grading of bounds the endomorphism filtration below, so iteration terminates and gives . Similarly . Restoring the right-action opposite convention gives and . All arguments hold for arbitrary and every ; no stable injectivity or admissible-origin Morita assertion was used.
For , , and is the identity; the right algebra is . 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 are zero; degree zero is scalar. Thus the exceptional cases stated in the Definition are covered without evaluating a nonexistent or invoking a positive-string Vust hypothesis.
In the one-box case , , , , the fixed-chart loop generator is , and step 3.2 gives its operator ; the untwisted Vust operator is . Both unital images remain , exactly as step 7.1 proves. Separately, for , , and , the displayed is and obeys . This witnesses why the correct commutation claim is the transported -commutation established in steps 2.1, 3.1 and 4.1. The full filtered bimodule, coherent , exact graded character chart and all-origin mutual centralizers have now all been proved.
Remarks
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The prefix-order cross-column sum has total tensor degree zero; it does not lower the total degree by one. The individual operator has degree one. This fixes the filtration while retaining all physical indices and the existing unshifted FDE mode convention.
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Equality of unital image algebras is weaker than equality of fixed-chart representations. The representation here is explicitly ; its degree-zero origin character is retained, including on .
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The origin shift on and the head/tail shift defining the Whittaker model have separate roles. The proof uses the actual balanced and ambient trace-form Casimir to establish the raw right operators and their -linearity.
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 column-flag calculation are choice-free.
Let be a nonempty pyramid with columns , let be arbitrary complex origins, and put for . For consider the raw tensor operator on the truncated tensor space of The deformed tensor space for the type-A finite W-algebra (whose underlying space is and whose is the operator displayed there). Then the minimal polynomial of on is exactly including repeated roots with their multiplicities. Consequently the action of on factors through the cyclotomic quotient of The degenerate cyclotomic Hecke algebra. The same polynomial annihilates the action of the ordinary Casimir operator on , where is the ground induced module with its genuine column filtration.
The statement does not assert that every unrelated standard object , or every parabolic category- object, carries that same tensor action. For there is no operator . The integral-root weight and the arbitrary-root coset bookkeeping are the separate conventions of The degenerate cyclotomic Hecke algebra.
Facts & Assumptions
Given: The nonempty pyramid, arbitrary origins , , , and . 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.
Define the raw operator locally on , , for by . A superscript denotes tensor position . The box-labelled sends to its left neighbour, with a missing neighbour interpreted as zero, and its longest string has length (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.
Put , , and . The ordinary ground module is , where . This is a Lie character, being a scalar trace on each column-Levi block and zero on the positive nilradical. PBW gives free as a right -module by ordering before ; the natural module has the -stable flag spanned by boxes in columns (The type-A nilpotent pyramid, good grading and Whittaker character, PBW gives an ordered monomial basis for the enveloping algebra, Universal enveloping algebra).
Separately, denotes the -character . The actual balanced Skryabin tensor map identifies with . Its formula is , with . 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; is treated separately and is not asserted to belong to that category.
The trace-form Casimir is ; its operator on a tensor product of genuine -modules commutes with diagonal . The universal first Hecke operator is , higher operators are , and places satisfy . 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).
Matrix units act by . For the total grading , an individual 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
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 is used.
Establish the raw affine action without a downstream dependency. Let and write for the balanced evaluation of F3. For a tensor basis vector write its actual Whittaker preimage as , so . If , then . If , the Whittaker equation gives . Apply these identities to . The nonnegative-column terms give the displayed diagonal scalar before subtraction; the negative character terms give the left neighbour of ; replacement in the first position subtracts , while replacement in any later position contributes the negative swap precisely when . 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 , independently of the lemma's downstream consumer.
On a tensor basis vector the full local formula is . Let be the span of tensors whose first box has column at most , with . The left shift and every negative swap strictly lower the first column; the diagonal term preserves it. Hence every is stable and . Starting with , apply the factors from down to . Their product kills , and the factors commute since all are polynomials in . Thus for , including coincident roots with all their repeated factors.
For the ordinary ground module, PBW gives an exact induction functor , since is right-free over . The tensor identity is the -linear map , , where . The matrix-unit relations show that extends multiplicatively to , and its formula gives the required balancing over . On the PBW basis of , has leading term ; all other terms have smaller PBW degree in the first factor. Finite descending subtraction proves it is bijective. Exact induction and carry the flag to a genuine -submodule flag . This is the column flag of the tensor product, not a finite flag of itself.
Give the total tensor grading of F5. The left shift raises this degree by one. The diagonal terms have degree zero, and has degree , regardless of the column gap. Therefore . For a nonzero polynomial of degree with leading coefficient , the degree- symbol of is : a top vector in a longest row has a nonzero th left shift, and the remaining tensor positions can be any nonzero basis vectors. This includes , whose symbol is a nonzero scalar identity. Consequently no polynomial of degree less than annihilates . Together with step 1.2, this proves that is the exact minimal polynomial, even when roots coincide.
Put and choose a box in column . By the matrix-unit action, . For , , so only survives and contributes . For each earlier-column box , the primitive coproduct formula in step 1.3 gives . The first term belongs to and the second is . There are exactly such boxes. Hence . Since is -linear and is generated by these ground tensors in columns at most , this also proves that it preserves the full flag and acts by on .
The raw affine action in step 1.1 kills by step 1.2, so its right representation kills the two-sided ideal generated by this polynomial and descends to . The generator-fixing anti-involution fixes , 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- object.
Apply successively to the flag of step 2.2. Each factor moves the relevant flag piece down one column, so their product annihilates . The factors commute and their order is immaterial. On the first ordinary Hecke/Casimir operator is tensored with the identity on the remaining natural factors. Tensoring the annihilating operator identity therefore gives on this entire module. No irreducibility, integral-origin identification or ordinary-to-Whittaker transfer was used.
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 and every nonempty pyramid. For there are no , so there is no or minimal polynomial to assert; the Hecke algebra is . The integral-root weight and arbitrary-complex coset conventions remain those of the cyclotomic definition and play no role in either local calculation.
Remarks
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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.
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The raw proof and the ordinary ground-module proof are separate. The raw action comes from the genuine module via the actual balanced Skryabin map, whereas the ordinary ground module is induced from with .
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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.
Separated integral cosets give typed parabolic category equivalences
Statement
Assume AC. Work in genuine type- parabolic category for with its fixed Borel. Its column Levi has ordered blocks of heights . All entries in column lie in , where the original admissibility condition is . Use the source highest-weight convention and half-sum , with the column reading prescribed by the source Borel. For each occurring entry coset retain its columns in their original order. Fix an order on the finite set of cosets; no order on is used.
Subject to the local HC tensor-projective comparison stated in [F1], stable sorting of the coordinates by 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 , where . 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 rows put . The component integral entry dictionary is exactly Thus , 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 sorted coordinates, its Levi highest weight and the integral highest weight differ by the scalar trace-character shift This shift is a Lie algebra character and requires no integrality of . 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.
The local tensor-projective comparison The regular coset-dominant Harish–Chandra tensor comparison: for a regular weight decreasing within each integral shifted-coordinate coset, finite integral-coordinate tensors and their direct summands give projective generators of ; for finite their Hom spaces are naturally , with evaluation and composition. Its same all-weight Duflo input is required for 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.
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 splits off from the semisimple theory.
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 , the integral roots are exactly differences of shifted coordinates in the same coset; their group permutes those coordinates.
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.
AC The Axiom of Choice, with the exact inherited/projective use recorded above.
Proof
Given: Use the data of the Statement and [F1]–[F5]. Normalize Chevalley matrices by , and . Twist by with twisted action .
Every -weight in the relevant weight-coset category is nonintegral when the adjacent shifted coordinates belong to different entry cosets: , and weight changes are integral. This holds in every subquotient. If for a weight vector of weight , choose maximal with , using positive-root local nilpotence in . The relation gives , a contradiction. Thus is injective on every object and subquotient of that category.
Powers of satisfy both Ore conditions in : iterating gives the finite binomial commutation formula, since is locally nilpotent on each enveloping element. PBW makes a domain. Its localization is a directed union of free right -modules; consequently localization is exact. Step 1.1 makes injective, and the diagram of short exact sequences proves exactness of . Therefore is exact. The adjoint exponentials defining are finite on every ; they send to and act as the adjacent permutation on the Cartan.
Let be the normalized highest vector of . The class becomes a highest vector of weight : its new is , whose value lies in ; the other transformed positive roots are positive roots distinct from , and commuting them through leaves positive-root terms killing . The new sends to , with every scalar nonzero. PBW, ordered with first, gives the basis of the localized quotient with -powers ; reflection permutes the remaining positive roots. Hence the displayed vector generates the quotient. Its character is . The highest-vector surjection is an isomorphism by equality of each finite weight dimension. This fixes its scalar by .
For finite-dimensional , localization commutes with tensoring. On the total operator has inverse ; the sum is finite since is nilpotent. The localization universal property identifies with and identifies the embedded . Quotienting and the Weyl matrix identify naturally with . For two finite tensor factors, , 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.
Choose regular coset-dominant in the weight-coset category. Crossing distinct cosets preserves each coset's internal order, so meets the same regular coset-dominance hypotheses; its central character equals . For a generator map encoded by , its action is the finite sum of finite-tensor matrix entries followed by enveloping operators on . The invariant matrix map commutes with the total 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 by simultaneous Weyl conjugation in its three factors. Each lies in a finite adjoint submodule, so that conjugation is and fixes , since its diagonal -action is zero. Thus induces exactly the common Hom identification of [F1], respecting composition and identity. The scalar from step 3.1 is the same on all generators , so it cancels on every generator Hom space; an arbitrary unnormalized scalar is not treated as a literal equality of highest vectors.
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 image is the cokernel of a map between target generators, hence belongs to the target category . 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 is an exact category equivalence, established on actual maps and presentations.
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 to and therefore sends its unique simple head to . 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.
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 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.
After sorting let have contiguous coset Levi and positive outside radical . In a fixed linkage block , [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 . For each initial union of coset blocks, write for its diagonal trace and for the common highest-label value. Every module weight satisfies : 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 is therefore a Levi module and is annihilated by . 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.
In fact . 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 . That Levi highest vector is thus a full 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 detects nonzero objects: every simple of has a nonzero highest vector in its top section, and exactness plus a composition series proves the assertion for every nonzero finite-length object.
Let be the product integral-reflection orbit for the Levi highest weights with these fixed scalar centres, and define , with acting by zero. PBW makes exact and identifies naturally: every outside negative PBW monomial lowers some prefix, so only its degree-zero term contributes. For a Levi simple , induction is a quotient of the ordinary Verma of label , hence lies in by [F3] and has finite length by [F2]. Every composition factor has nonzero top section by step 10.1; exactness and imply that there is only one factor. Thus is simple. Exactness extends block membership and finite length to for every finite-length by a Levi composition series.
Induction and radical invariants are adjoint, and step 10.1 identifies the latter with . Their unit is PBW's top-section isomorphism . For the counit , applying exact gives this identity, so its kernel and cokernel have zero top section; both are finite-length objects of and vanish by detection in step 10.1. Hence and 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 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.
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- 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 , 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.
The original tableau convention gives , so dot sorting is literally stable sorting of the . In the sorted block the Levi coordinate is . The integral coordinate from the Statement is ; their difference is exactly . Tensoring with the one-dimensional Lie algebra representation is an exact inverse equivalence with inverse shift , 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 is , its integral image is ; these are the actual bottom-aligned integral ground rows. The retained heights give nonincreasing and . 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.
For clarity about tensor transport, the ordinary induction tensor identity is ; it follows from the coproduct and antipode and is natural in . The restricted vector representation has its actual prefix- filtration whose sections are the coset vector modules with outside radical zero. Exact induction therefore gives a filtration of with sections . A projected linkage/entry-multiset tensor summand admitting an entry change in coset kills the other sections: their highest labels change a different coset multiset, so their central characters or linkage classes differ by [F3]. Only the 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.
The trace-character shift changes the relevant vector Casimir eigenvalue by its scalar: for , replacing the first-factor action by adds 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 , the quadratic central element has value , while its value on the vector is . Taking half the difference gives the global tensor-Casimir eigenvalue . For the Levi coordinate , the same calculation gives , greater by . Hence the trace shift contributes to the original residue: . 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.
The Whittaker functor from the relevant parabolic category-O summand
Definition
Work over and assume the Axiom of Choice where projective covers, duality and locally unital assemblies enter. Let be a pyramid with columns , let be admissible in the sense that implies , and let be the relevant summand of the genuine parabolic category attached to the labels and the degree : 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 -diagram content 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 -finitely-generated object of genuine parabolic , the Whittaker functor is the covariant finite-dimensional dual Its action is obtained from the continuous -part of the right linear dual, then the reflected head/tail identification proved below. In the notation , the middle Whittaker operation is performed on this continuous -part, not on the uncompleted ordinary row-restricted dual. Write for source standard objects, for source simples, and for the resulting nonzero simple -modules. These namespaces are distinct.
The verification below records the properties used on this page: is exact on the -finitely-generated objects of genuine parabolic and intertwines tensoring with finite-dimensional Cartan-semisimple -modules, the Casimir and the flips; is distinct from the Hecke quotient constructed later; for the ground simple projective-injective and one has and ; and is the simple -module for standard labels and zero otherwise. Nonintegral origins use the typed equivalence of the all-weight Harish-Chandra comparison of the source; no arbitrary complex is identified with an integral block. After fixing the ground identification , the compatible functor and the maps are unique up to the normalized unique natural isomorphism; without this normalization scalar automorphisms prevent literal uniqueness.
Facts & Assumptions
Given: The pyramid , admissible origins , the categories and the Whittaker data; assume AC The Axiom of Choice for the stated imported constructions and Baer/vector-space splittings.
The parabolic and genuine-category-O interfaces: is the ground simple projective-injective, the standard objects and simple objects 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).
The finite W-algebra, its Whittaker category and Skryabin's equivalence, including the filtration and the tensor identification on restricted -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).
The truncated tensor space is a filtered -bimodule with the explicit generators, and the tensor compatibility preserves the generators (The deformed tensor space for the type-A finite W-algebra).
The typed nonintegral category comparison and admitted-ground coset dictionaries are supplied by The regular coset-dominant Harish–Chandra tensor comparison and Separated integral cosets give typed parabolic category equivalences. Standard/Casimir/Fock interfaces: the highest-weight truncation, the Specht-to-permutation dominance comparison, the Weyl character formula computation, BGG reciprocity and the Fock-basis dictionaries on the source side (Schur-Weyl decomposition and highest weights, Homomorphisms from Specht to Young permutation modules obey dominance, The Weyl character formula, BGG reciprocity, Standard tableau monomials form a basis of the highest weight Fock submodule, The parabolic category-O Grothendieck group is the integral Fock module, Simples, projectives and tiltings map to the three distinguished Fock bases, Duflo–Joseph g-finite endomorphisms of every Verma module, Projective functors on a regular integral block, Base change, freeness and specialization in the deformed family, The Grothendieck group and character of O).
Noetherianity, Baer injectivity, complete reducibility and Hilbert basis inputs used to make the functorial constructions finite and exact (Hilbert basis theorem: if is Noetherian then is Noetherian, Baer's criterion for injective modules, Weyl's complete reducibility theorem, Standard parabolic and Levi subalgebras from a subset of simple roots).
The SAME original finite-W algebra has both its tail/left and head/right normalizer descriptions for every initial-column prefix, with ; the proved original prefix 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 , 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.
The normalized highest-component projection is an actual module map with saturated integral kernel spanned exactly by off-standard source dual-canonical and independent image basis ; the original-order source upper ground component is exactly (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.
In the actual tensor box grading, the original loop/PBW symbols identify with ; the graded left representation is , with its actual degree-zero origin character, while the graded right generators are 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 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
Given: Assume AC. Use and . The source standards are , source simples (abbreviated in the computations), and output simples . The finite tensor/Hopf comparisons use the actual Skryabin displayed map, not cofree constant evaluation.
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.
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.
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.
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
(F·u)(v)(r)=lambda(u r v),
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.
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.
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.
For the natural box module define when , and otherwise. These are the actual prefix coefficients, not reindexed series. They give a unitriangular matrix. For with , establish both and . If , disjoint supports give zero. If , the original left/right normalizer theorems for prefix give both containments; a whole-pyramid shift differs from the corresponding prefix shift only by a uniform trace character, which fixes , and both ideals. For , expand the actual prefix last-column recursion [F6]. Its embedded prefix- terms and its final commutator with the positive previous-to-last matrix commute with . Only the column-Levi sum contributes. Its bracket is . The negative bridge commutes with the prefix- coefficient, so its left and right reductions both give . The two consecutive displacement signs differ by minus one, giving precisely . Diagonal shifts add commuting scalars, so this boundary calculation works for both head and tail.
Finite-Levi Weyl gives, on row variables z_(n−q+1),…,z_n,
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)).
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.
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.
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).
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.
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.
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.
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.
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.
The actual highest-component projection is module-linear and, in its integral bases, is the coordinate projection with off and on . Its kernel is therefore a direct summand, and specialization at parameter one gives exactly , with no extra specialization kernel. For a nonstandard simple, exact residue translation and the source dictionary give and . Expanding these actual modules in their simple classes and projecting gives a sum of independent 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 . 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.
Every standard embeds in an iterated lowering translate of a standard simple. To construct the monomorphism, shift the entries of column upwards by an integer , choosing these successively so that every shifted entry in that column is greater than every earlier-column entry in the same coset. The resulting is standard and minimal in its fixed-multiset Bruhat orbit; the triangular standard/simple multiplicity matrix gives . For each column , list its original entries increasingly and lower its smallest entry from to , then its next entry, and so on, using in that chronological order. At each step the distinguished change in column 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 is filtered by standards with , while unless , since a nonzero image has its head as a composition factor of . Thus for largest and smaller , every map from that projective kernel to vanishes; the projective-cover exact sequence gives . 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 . For mixed cosets the same construction is performed only among comparable entries; the typed standard and tensor equivalence transports the inclusion.
Prove the raw centralizers here before using any Morita conclusion. Give its finite box grading, let be the image of and the right Hecke image regarded as operator algebras, and give them the induced integer filtrations in . They commute by the actual tensor model. The loop/PBW symbol dictionary [F8] gives for the unital image of the character-twisted representation, and the Hecke symbol dictionary gives for the truncated polynomial/permutation image. The character defines the automorphism on primitive centralizer generators, with inverse given by , so is EXACTLY the untwisted unital Vust image; the degree-zero scalar origin terms remain present in the full representation. Vust gives and . Taking leading terms of commuting operators yields , and interchanging gives . 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.
Put with the RIGHT action proved above, and . The original-head right-normalizer theorem [F6] gives for the SAME original , not an unidentified reflected algebra. Thus preserves , since its commutator error starts with a shifted generator killed by . Finite duality now defines the genuine covariant left action on . Precomposition with a source morphism intertwines this action, proving functoriality. The numerical identity is consistent with the two column counts, but the actual original-head normalizer theorem supplies the algebra identification.
The inverse is the finite sum of descending-column paths, with a length- path product multiplied by . Prove directly from this path sum. Before the unique possible column- vertex, every factor belongs to a larger prefix and therefore normalizes the right ideal; after it, the factors have disjoint support from . Reduction of the product commutator is consequently legitimate. The surviving bracket replaces a factor starting at by its factor starting at . Pair the path which next visits with the path omitting that visit; the products coincide because and their signs are opposite. Only the terminating visit remains, with sum . This proves the right inverse equation without multiplying arbitrary right-ideal congruences on their left. Adjacent negative matrices generate , so the commutator rule propagates both matrix equations to every negative generator.
The ordinary finite tensor pairing restricts to as right modules. Continuity is checked on both sides: take an Engel flag with successive factors on which acts trivially. If kills each coefficient functional on , expanding the diagonal shifted action shows that 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 . This establishes equality of the continuous subspaces as well as the uncompleted tensor-dual equality.
If a simple embeds in , compose with the monomorphism of step 1.21 and use repeated biadjunction to obtain a nonzero, hence surjective, map with standard. Step 1.20 excludes this when 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 . This is a statement about actual submodules, not about its entire list of composition factors.
An operator in has, by step 1.22, the same largest homogeneous symbol as a member of . Subtract that member to lower its integer degree. The finite grading of bounds the endomorphism filtration below, so this procedure terminates and gives . Interchanging the two images gives . Restoring the right-action opposite convention proves and , where is the cyclotomic IMAGE algebra. For tensor degree both images are scalar; for an empty pyramid and positive degree both images and both commutants in are zero. No admissibility, stable injectivity, projectivity or Morita assertion entered this raw filtered argument.
For with finite-dimensional , PBW gives . Restriction identifies with ; its inverse is . Moreover . Hence is -linear for the head-twisted action . For every -map , makes the restriction square commute, so is the ACTUAL map under these identifications. This proves induced quotient and antisymmetrizer naturality without using equality of characters or presuming right-Hecke linearity. In particular is the finite-Levi standard ; a source standard is not asserted simple.
The two matrix equations persist under direct sums and summands by an adapted basis and uniqueness of the triangular left lift. For tensor factors put , and . Inserting the two successive left/right Whittaker lifts proves their equations, and these displayed products are inverse. Modules with trivial derived action use identity matrices, including central Jordan multiplicity spaces. Complete reducibility of 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 -module has these double-admissible matrices. This algebraic construction also allows central Jordan multiplicities; the category- tensor compatibility below requires a Cartan-semisimple tensor factor. The usual left contragredient and the right vector-space dual , defined by , keep their separate action conventions; no identification is used.
The ground central-character multiset determines a unique column-strict label. Within each charge coset its smallest entry 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 , the coordinates show that the central character is precisely this entry multiset. Hence the ground block has the sole column-strict label . The generalized standard has diagonal simple multiplicity one and no other simple label in this block, so . Actual BGG reciprocity and the projective standard flag give and no other section, so . 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 is projective-injective. Simple-preserving restricted transposition duality fixes and the natural module and commutes with this tensor product; hence 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- standard label is an incoming crystal move from a degree- standard label, except ground in degree zero. Inducting from the ground quotient, exact gives using the ACTUAL simple-head theorem; is a summand of , so is a quotient of . Lift any such quotient through its projective cover. Essentiality of the cover makes the lift surjective, and projectivity of splits it. Therefore the projective summands of are exactly the covers of the standard-label simples, with positive multiplicities; they are injective as summands of . It follows that every nonzero submodule has a nonzero standard-label simple socle. Exact and the nonvanishing already proved in step 1.18 then give . This proves the required detector; it does not assert that every composition factor of is standard or that generates the whole parabolic category.
For a finite-dimensional left module , the left Whittaker lift of is ; the right lift of is . 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 ; the tensor, direct-sum and summand constructions of step 3.2 retain a finite flag with trivial sections. The local cohomology supplier gives vanishing positive twisted cohomology on . On its tensor product with this flag, the long exact sequence therefore makes invariants exact on successive sections, identifying each section with 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 . Left Whittaker invariance makes its entries elements of the ORIGINAL . The identity gives ; gives . The head/tail shifts add Lie characters, so their coproduct identities reduce both computations to the same unshifted . Therefore the perfect finite pairing is a MODULE pairing: . This is the necessary algebra-action argument, rather than a vector-space duality substituted for it.
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.
Let be a finite-dimensional Cartan-semisimple -module. Then is again a genuine parabolic object: its weights are sums of weights of and , and local finiteness for follows from being finite-dimensional for each . It is finitely generated over by tensors of generators of with a basis of : induction on word length uses . Thus its image is defined on the stated domain. Apply the original-head right Skryabin counit , . Tensor it with , apply right Wh and use step 2.3 to obtain . Combine this actual counit with the module pairing of step 4.1 and take finite duals. This gives the natural isomorphism for EVERY genuine parabolic object , 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.
Compute the actual Casimir coefficients in ordinary box matrix units. On the LEFT lift, the coefficient at after is . Positive matrices give after undoing the shift. Negative matrices give by step 1.9. Their total scalar is . On the RIGHT lift the coefficient at is ; step 2.2 moves negative matrices left, giving , and the total scalar is . Multiplying by on the left or on the right therefore gives the SAME entries . There is no extra displacement sign on the ordinary ; signs are already in . The entries lie in 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 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.
Fix the head-normalized ground map obtained from step 3.1 and the finite-Levi character calculation below. Iterate on to obtain , and compose with the proved ACTUAL balanced tensor map to get . Casimir and flip compatibility prove -bimodule linearity. Any source endomorphism is transported as ; in particular a native Casimir/place word representing right multiplication by becomes the actual map . 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.
acts on by the universal tensor Casimir and places. At the first tensor step the actual finite flag of the natural module has one standard section per column. On the th section, the ordinary quadratic-Casimir identity gives eigenvalue . Successively applying the factors in the column-order flag makes annihilate ; subsequent tensor factors leave this first-step relation intact. Hence the source action factors through the genuine cyclotomic algebra, not only its image. Step 7.1 transports it to as the actual bimodule action.
maps into by step 2.5, and its image contains because every target Hecke operator is the transport of its actual source Casimir/place operator. A nonzero source endomorphism has a nonzero image . Step 3.3 proves , and exactness identifies with the image of its transported endomorphism. Hence the endomorphism map is injective as well as surjective, giving . Detection uses the standard-label SOCLE criterion, never a claim that all composition factors of are standard.
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.
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.
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 and . The preceding kernel/Morita construction proves for standard labels and zero otherwise; it never asserts that the image of a source standard 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
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The proof uses the continuous -dual and its right action; plain row-restricted duality does not make an ordinary category- object Whittaker. Source simples and standard objects have separate names throughout.
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The definition deliberately separates three functors that are often conflated: the genuine Whittaker functor on category , the Hecke Hom quotient , and the Morita equivalence on the finite-W side. Only the first is defined here; the quotient is defined two items later.
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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.
The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer
Statement
Assume the Axiom of Choice. Fix the pyramid with columns , an origin , and , and let be the truncated tensor space of The deformed tensor space for the type-A finite W-algebra. Let be the image of the finite W-algebra and let be the image of the cyclotomic Hecke algebra of The degenerate cyclotomic Hecke algebra under the right action. Then:
- and are mutual centralizers on , for every complex origin and every , and their associated graded image algebras are the corresponding images of and of the truncated polynomial/permutation algebra.
- For a nonempty pyramid, if , then the action of the full cyclotomic algebra is faithful.
- If is admissible (that is, implies ), then the tensor module is a progenerator and is a Morita equivalence between -mod and -mod.
Mutual centralizers alone do not imply Morita for arbitrary : the explicit example with , , in step 7.1 below has a nonprojective left -module.
Facts & Assumptions
Given: The pyramid , an origin , the truncated tensor space , and the image algebras , .
In the fixed loop chart, the associated graded left representation is the character-twisted Vust representation . Its unital image is exactly the untwisted Vust image, because it is obtained by the automorphism of . 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).
has a separated loop filtration with associated graded , and the cyclotomic quotient has the bounded monomial basis with ; 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).
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).
The genuine standard/Casimir interfaces proved in The Whittaker functor from the relevant parabolic category-O summand supply the admissible character/quotient computations.
Proof
Given: The filtered bimodule , its actual character-twisted graded representation and its unchanged unital Vust image algebras.
The graded unital images. Write , , and for the right Hecke image viewed as an algebra of operators on . The supplied actual tensor model in F1 gives commuting filtered operator algebras, with the graded symbols containing the unital images of and of the truncated polynomial/permutation algebra. The character automorphism in F1 gives exactly the same as the untwisted representation; no equality of the fixed-chart twisted and untwisted modules is inferred. Since are mutual centralizers, taking leading homogeneous terms of commuting operators gives , where is the commutant in . Interchanging gives . Thus every inclusion is equality, establishing strict equality of both graded images as well as their commutants.
The exact ordinary-dual adjoint. For a finite rational -module , Skryabin transports ordinary evaluation and coevaluation to the tensor functors . The ordinary zigzag identities give both adjunctions between and . 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 : 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 to degree . For , also , and the exterior power is a summand of a tensor power by the antisymmetrizer. Determinant shifts therefore give closure under too. Consequently preserves projectives in the entire rational category through its exact right adjoint . Here is the ordinary contragredient natural module, distinct from ; the transpose contravariant duality of category is not this adjoint.
The filtered centralizers. For an operator in , equality of the induced graded spaces in step 1.1 supplies a member of with the same leading symbol. Subtracting lowers its integer filtration degree. The finite grading of bounds the induced endomorphism filtration below, so this terminates, proving . The same procedure proves . 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 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.
Stable injectivity. For a nonempty pyramid with , choose distinct terminal boxes on length- Jordan strings. In the associated graded tensor action each bounded PBW word , , sends their ordered terminal tensor to the tensor with those distinct strings permuted by and each box moved places left. These 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 .
The finite-image row projectives. Assume admissible. A row occupancy determines a tuple of terminal row boxes and the diagonal row-multiset projection . Since the right tensor matrices preserve row multisets, by step 2.1; these orthogonal idempotents sum to one. Here is the actual basis of their projective left ideals. For a commuting matrix , place permutations identify diagonal -orbits, and the image forces when some source column is smaller than its output column. Comparing its coefficients with and replacing by expresses each nonterminal coefficient in coefficients with larger total source column sum: the first term is , the diagonal term is , and the two remaining sums run over swaps with respectively both columns at most, or both columns greater than, the th 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 be the normalized preimages. Evaluation on gives exactly the orbit sums under , which form the monomial basis of with its actual -twist. Thus as actual modules, and the regular module is their sum. This proves these projectivities in the finite image, without invoking Morita.
Projectivity of the ground object. For , take degree and the one-dimensional determinant-shifted ground object , with tableau . 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 is one. Indeed, the Levi decomposition of uses semistandard tableaux of shapes given by the column partitions of ground differences, with the alphabet in column 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 -filtration by these Levi sections. For the shapes are rectangles and the allowed alphabet has exactly letters. Each length- strictly increasing tableau column must contain every letter in order. There is exactly one tuple, and its row- multiplicity is . Thus the coefficient is one for and zero for every other occupancy. Other standards cannot contain because their scalar central characters differ. The supported regular summand has length one and is itself, so is projective over . For a surjection in the rational finite-W category , 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 becomes a map from into the degree- summand, where it lifts by the projectivity just proved. The inverse determinant twist gives the original lift. Hence is projective in , without claiming projectivity in arbitrary -mod.
The finite-W projective covers. Write for the genuine continuous-dual functor of The Whittaker functor from the relevant parabolic category-O summand, and put for standard labels. At degree zero this is the ground object, projective by step 4.1. For a positive-degree standard , the actual standard-label crystal supplies and a quotient . Lifting along the projective cover and splitting proves is a summand of . The genuine tensor comparison sends this to a summand of , projective by step 1.2. To identify its head, write with standard , using the independently proved detector head/socle property in F3. Exact gives . On the other hand ordinary-dual adjunction, the induction hypothesis and the genuine simple/tensor comparison give . Comparing this equality with the sum over forces for every summand with . Thus each is the genuine projective cover of . Exhaustion of finite-image simples and occurrence of every standard cover in the detecting tensor object now show that is a projective generator of -mod. This uses the actual simple-image and tensor maps of F3, rather than inferring covers from characters or mutual centralizers.
Morita for the finite images. Since is a finite projective generator of -mod, every module admits a presentation by finite sums of . The evaluation maps from the tensor-Hom adjunction are isomorphisms on 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 gives the inverse evaluation. Thus is an equivalence with inverse , and step 2.1 identifies its target algebra with the genuine Hecke image . 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.
The nonadmissible boundary. For , , , use the basis . The raw formula gives , , , and swaps and fixes . Put , let and , and let , , . Solving the two linear commutation equations with gives . Indeed , , and direct coefficient comparison gives precisely these three free parameters. By step 2.1 this is , . Its module decomposes as , , where acts by . The basis identifies . The last summand is not projective: a section of would send to an element killed by , hence to , 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 has at least strings of maximum length , 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).
The Whittaker functor is exact and fully faithful on the required projectives
Statement
Assume the Axiom of Choice. For admissible origins the genuine Whittaker functor of The Whittaker functor from the relevant parabolic category-O summand is exact on , and is a natural isomorphism, where . Both and the Hecke quotient are fully faithful on all projective objects of the relevant summand, and the quotient is also fully faithful on tiltings. 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- summand. is a projective generator of -mod, and preserves projectivity on ; it need not send every projective of to a projective -module. The composite of with the Morita equivalence is the Serre quotient killing exactly the off-standard simples.
Facts & Assumptions
Given: Assume AC. Fix admissible , the finite whole-block summand , its standards , simples , restricted duality , ground , detector , genuine Whittaker functor , tensor image , and right Hecke image .
The genuine continuous-dual Whittaker construction is exact, sends to its finite-Levi -standard, kills precisely off- simples, and has a coherent bimodule isomorphism . 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 ; its exact faithful factor through the corner has the form 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.
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, vanishes unless , and unless . PBW and ordinary polynomial Schur modules are PBW gives an ordered monomial basis for the enveloping algebra and Schur-Weyl decomposition and highest weights.
The actual integral normalized Fock projection is module-linear, with coordinate kernel spanned by the dual-canonical for off- labels and independent images for ; the simple-class dictionary at parameter 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.
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 and on , so their tensor product supplies , with the Casimir and crossings self-adjoint. This is transposition duality, not an assertion .
Proof
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 ; all positive-degree categories and tensor objects are zero. Every asserted comparison and copresentation is then immediate. The construction below treats the nonempty pyramid.
The categorical nonstandard kernel. In the Fock bases the normalized projection is a coordinate projection with coefficients , so specialization at has precisely the off-standard span as kernel. Module-linearity makes this kernel stable under every . Under [F3], expand for off-standard as , where are actual composition multiplicities. Projecting gives , and independence forces every such ; the same holds for . Exactness extends this to the entire off-standard Serre subcategory. For complex , apply the product of the component projections with entry and residue shift , ; 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 or the standard predicate.
Maximal ground-column induction. Split off the last column, with two-block Levi and upper radical , and define , , and right adjoint . PBW gives exact and . 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 -invariants, since moving opposite-radical PBW monomials across the nondegenerate contravariant form pairs a lower invariant to zero against every vector. Hence . For a costandard, invariant functionals vanish on all positive-degree opposite-radical monomials, giving . Taking the exact top eigenvalue slice of the first-block trace, when have the same degree split, now gives : smaller top eigenvalues contribute nothing and the top Levi simple determines its concatenated label uniquely.
Actual standard embeddings. Given , shift columns upward by integers , chosen successively so each shifted entry in column exceeds every earlier-column entry in its coset. The resulting is standard and Bruhat-minimal, hence by [F2]. Write column of as and set , composing rightmost first. Apply , then , through : 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 . If , biadjunction gives a surjection from an iterated image of onto the standard simple ; step 1.1 forbids this for off-standard . Every standard therefore has standard-labelled socle.
An actual cover isomorphism. Append the ground last column to . Every 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 have degree split . Adjointness and step 1.2 show that has simple head . Lift the cover map to obtain , whose image is all of 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 ; an equality of characters has only been used to kill the kernel of an already constructed map.
The detector and the injective hulls it contains. The ground simple is projective-injective. Tensoring by preserves both projectives and injectives because the distinct tensor functor is exact and adjoint on both sides. The tensor product contravariant form gives . 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 . Duality gives standard head for . Every standard label of positive degree is for a lower-degree standard label by [F3]; induction using the actual crystal head of gives . Lift this epimorphism through ; essentiality makes the lift surjective and projectivity splits it. Thus the indecomposable summands of are exactly the standard-labelled covers, all with positive multiplicity and all injective. Moreover for every standard . This hull membership does not presume individual summand self-duality.
Cumulative-column projectives. Put and , with degree , and . Induct on the number of columns. One column is completely reducible. Removing the last column and using tensor identity gives . 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 is genuinely projective.
Every cover occurs and the quotient has a standard flag. For a label , take . Project each prefix onto its last-column Levi quotient. The tensor product of the resulting row symmetric powers surjects onto : 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 , and projectivity plus essentiality of the cover makes a split summand of . Averaging symmetrizers embed as a -submodule of ; PBW preserves this injection and identifies the ambient induction with . Its finite -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 .
All-projective copresentations. For an indecomposable projective , choose a splitting from step 4.1 and view as its actual submodule of . The sequence gives a standard flag of , since is projective and has its BGG flag. Its socle is standard by step 2.1, so its finite injective hull belongs to by step 3.1. Compose to obtain , exact at . Finite sums give every projective a two-step copresentation with both . The last arrow need not be surjective.
The right-adjoint unit. Choose a full finite projective generator of the entire category-O summand containing as an explicit summand, with algebra , and let be the projector onto this actual . Thus , retaining all its multiplicities. For , , the right adjoint is with unit . The restriction is an isomorphism, so its kernel and cokernel are annihilated by . If has standard socle then is monic. In particular is monic and splits since its source is injective. A complementary summand has , but adjunction gives , forcing its inclusion to vanish and . Thus is an isomorphism on . Apply exact and left-exact to step 5.1; the comparison of kernels gives an isomorphism for every projective. Adjunction therefore proves fully faithful on all projectives, while left-adjoint recovery has only been asserted on .
Tilting full faithfulness. If has standard head and standard socle, then is monic and its cokernel is annihilated by . Every map from to that cokernel vanishes: a nonzero image would have a standard simple head because it is a quotient of , while all its factors would be off-standard. By adjunction each -map gives , which therefore factors uniquely through . 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.
The actual Whittaker comparison and quotient. By [F1] the exact Whittaker functor factors through as the actual equivalence , with a right -progenerator and . Its inverse is , and its unit on is . Under the source action this is precisely , since the counit on is evaluation; thus the comparison is a natural isomorphism of actual maps and Hecke modules. In particular is a left -progenerator, and is fully faithful on projectives by step 6.1. The corner functor is the Serre quotient with kernel consisting of objects with only off-standard factors; applying the genuine equivalence identifies the same quotient for . Projectivity is preserved on , whose image consists of the corresponding projective covers. This does not assert preservation for other ambient projectives.
Simple images and standard heads. The exact corner functor kills precisely off-standard simples and identifies its other simple images with the distinct exhaustive -simples; the genuine equivalence of step 8.1 transports these to the corresponding finite-W simples . For standard , , so is an indecomposable -projective with head : its Hom to each simple is the corresponding Hom from by the elementary add equivalence. Lift through ; the image surjects onto the standard's head and is therefore the whole standard. Applying exact makes a nonzero quotient of this indecomposable projective, so it has the same unique simple head. Through Morita, the actual finite-Levi standard likewise has unique simple head . This does not assert that a specified finite-Levi highest vector generates it.
Independent row compression. Add full ground rows until the enlarged smallest column has height at least ; all roots remain fixed. For each row , the normalized coefficient is its row-Cartan operator, with ground scalar . On the actual tensor space and every finite-Levi standard of degree its eigenvalues are , , since the remaining weight is polynomial row occupancy. Thus the SAME finite-image element is the zero-deleted-occupancy projector on both tensor space and all these standards. In it selects tensors using only retained rows. The actual dot formula preserves row multisets, so 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 is unchanged. Therefore as right Hecke modules. Extending a commuting endomorphism of by zero shows , where are the large and small left image algebras. For the finite-Levi standard, the zero-deleted-occupancy part of is 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 changes by , cancelling the retained source-reading shift ; its normalized highest weight remains the entry plus row index minus one. The corner action and its Gauss coefficients consequently give for contractible labels and zero for noncontractible labels, as actual module identifications.
Simple contraction without highest-vector assumptions. Every noncontractible standard simple is killed by , because it is a quotient of the standard annihilated in step 9.2. For a finite algebra and an idempotent , restriction gives a bijection between its simple modules surviving and the simples of : any nonzero vector in generates , and for a small simple the module has a unique simple quotient surviving . Indeed its -part is ; every proper submodule has zero -part, since a submodule containing that part generates the whole induced module. The sum of all such proper submodules is still annihilated by 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 , which has the unique head from step 9.1, hence .
Fullness and the central Hecke corner. If a contractible 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 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 be their central support in ; then , since kills all complementary simples. Every simple of survives by step 10.1. If were proper, its nonzero quotient would have a simple killed by , a contradiction. Hence . Multiplication has inverse ; balancing and this identity verify both composites. This gives a faithful Morita equivalence on all supported-block modules. The operator belongs to the right centralizer and is central there, so restriction identifies with . To verify enlarged stable faithfulness directly, choose distinct terminal boxes on length- Jordan strings. In the associated graded tensor action each bounded PBW word , , sends their ordered terminal tensor to the tensor in which those distinct strings have been permuted by and the box on string moved places left. These 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 . Its trace is therefore symmetric and nondegenerate by [F4]. This local proof precedes, and does not depend on, a later stable-range definition.
The actual duality comparison. Let be the tensor contravariant form. Put with , and with the same twist. Transposition gives the natural isomorphism , , whose inverse is . This uses only , not individual projective self-duality. Tensor-Hom gives , and the symmetric trace of step 11.1 gives by . Define by . The form identity makes this balanced and -linear. Applying gives a natural map between exact functors; exactness of follows from the symmetric algebra's injective regular module. On it is the regular trace-duality isomorphism, and hence is invertible on add. 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 .
Individual standard prinjectives are self-dual. For standard , by step 3.1. Step 12.1 gives and fixes its simple label because . In a symmetric algebra the primitive projective 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, . Both and are projectives, so full faithfulness of step 6.1 lifts this isomorphism and its inverse; their composites are identities by faithfulness. Hence , 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 and their copresentations. The object 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 .
The higher-level Schur-Weyl projective generator and Schur functor
Definition
Keep the pyramid and admissible origins of The Whittaker functor from the relevant parabolic category-O summand, the ground object , the tensor object and its central decomposition. For a charge with let be the finite set of residue sequences of content , and let be the corresponding central component of ; in the integral model the sum of the residue-induction images of the ground object. Put the corresponding central component of the Hecke image algebra (the opposite convention is fixed here), and define the Schur functor of the block by Its left adjoint is .
For the whole polynomial summand, use the distinct finite projective generator with actual prefix symmetric modules 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 ; every embeds in with a standard-filtered quotient. Exact projection gives on the entire central block. The tensor detector remains the object defining ; generates all Col labels, while 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: is exact, being Hom from a projective object; its left adjoint is right exact but not exact in general; it sends -projectives to projective objects and recovers , including every standard-labelled prinjective; neither exactness of nor recovery of every category- 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 , remain in the category .
Facts & Assumptions
Given: The ground object , the tensor object with its central decomposition, a charge , and the objects , , .
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).
The residue-induction construction produces the central components as images of the ground object, and the Hecke action endomorphisms give 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).
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).
The actual prefix modules are projective in the whole finite Col summand, contain each projective cover as a direct summand, and embed in 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
Given: The component and the functor .
Exactness of . is a direct summand of the projective object by [F1]; is exact for projective , and passing to a direct summand preserves exactness, so is exact.
The left adjoint. The tensor-Hom adjunction gives as left adjoint of ; 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 -modules map to direct sums of copies of , which are projective, and direct summands of projective objects are projective, so sends -projectives to projectives.
The whole-summand generator. By [F4], the finite sum is projective and contains every Col-labelled cover; exact central projection gives the projective generator of the whole block. The same supplier gives actual inclusions of each prefix summand in with standard-filtered quotients, providing the projective-copresentation prerequisite without identifying with the detector .
Recovery on . The evaluation 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 recovers every object of , in particular every standard-labelled prinjective contained in .
The rank-one boundary. Take , and . The ground highest weight is , and its natural tensor gives the regular-block detector . The rank-one Verma formula gives the nonsplit sequence and . BGG reciprocity in [F1] gives and the nonsplit flag ; the flag cannot have on top because the cover has head . Thus has head and socle and middle factor . Let be its head-to-socle endomorphism. Then , and the level-two endomorphism algebra is by the supplied Hecke identification. Any map has image in : its composite to is zero. Hence , and has head , whereas has head , so recovery fails. Moreover tensoring the injection with gives , with nonzero kernel . Thus is not exact. All modules lie in this fixed regular block and retain its scalar centre.
Assembly. Since the charges decompose into finitely many central components in each degree and the categories are locally unital in the infinite case, the functors assemble to the locally unital sum; the ambient category retains all labels, including those killed by the functors.
Remarks
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The opposite convention in 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.
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The two-term copresentations of the exactness theorem show that every projective has a copresentation by objects of , but a copresentation does not imply recovery by the left adjoint: the left adjoint is only right exact.
Stable range and block idempotent corner for higher-level Schur-Weyl duality
Definition
Assume the Axiom of Choice. Keep a nonempty pyramid with columns of heights , the origin , and of The deformed tensor space for the type-A finite W-algebra. The stable range is : there are at least rows of maximum length . Put , and .
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 implies , the following construction defines the central support outside that range. Append full ground rows of length until , keeping and fixed. Then and every increase by , so every stays fixed. In the enlarged tensor space , let 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 in row and column . The supporting central idempotent 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 , and
This is a sum of entire supporting central blocks. Individual residue idempotents 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 , the convention is separate: in degree zero the tensor and image algebras are with the identity corner ; in positive degree the tensor, image algebras and their module categories are zero and . No 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.
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.
The genuine original-head standard/simple comparison identifies as the head-normalized inducing Levi module, with scalar central character given by the content ; a standard-labelled has unique simple quotient 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.
Finite algebras have projective covers and every nonzero finite module has a simple subquotient (Every finite-dimensional module has a projective cover, unique up to isomorphism over the target, The regular module is a direct sum of the projective covers of the simple modules, with the split-field multiplicities).
Proof
Given: , , the retained-box embedding , and admissible for the central-support claims.
The retained projection is an actual left-image idempotent. The matrix commutes with the right and : left-neighbour moves, place swaps and scalar terms preserve the row multiset, so none changes zero deleted-row occupancy. Thus by the independent first centralizer. Every term of the right tensor formula restricts identically under , because row and column positions and left neighbours agree and . This proves the actual right-bimodule identification and a surjective restriction map . Extending a commuting operator on by zero on shows . No Morita conclusion is used.
The standard contraction has the same corner action. In column the finite Levi module is , with the partition of the ground differences. The zero-occupancy part is , by the tensor Young-symmetrizer realization; it is zero precisely when a removed-row partition entry is nonzero. For the original 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 in column , while a retained box's ordinary source reading position changes by . Its source highest weight therefore cancels that shift: the normalized weight is in both diagrams. Hence the complete retained matrix action, and then formal Gauss elimination, gives for contractible , and zero otherwise, with the corner identification of step 1.1.
The simple contraction and central saturation. The same projector acts on all standards: let be the row Cartan and . Its head-normalized action on a degree- Levi standard has equal to polynomial row occupancy with eigenvalues . Hence is exactly zero removed-row occupancy on every standard and equals step 1.1's image idempotent; for the inner product is one. Exactness of and step 2.1 therefore kill every noncontractible simple. For a surviving big simple , each nonzero generates , so is simple. Conversely for a corner simple , every proper submodule of is killed by : one with image generates that whole induced module. The sum of proper submodules is thus proper and is its unique maximal submodule. Its simple quotient has -image . 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 , whose already proved unique head gives . If and is contractible, separate the charge cosets. Admissibility makes all charges in one coset equal. The minimal bottom entry occurs once in every column of that coset; strictness and nonnegative ground differences force these occurrences into the same bottom row of . Remove that row and repeat for all deleted rows. Then is contractible. Scalar central characters therefore separate contractible from noncontractible simples, so generalized central-character decomposition gives a central idempotent with exactly that support. Since kills all complementary simples, : a nonzero idempotent acts nontrivially on some simple of a finite algebra. Hence .
Fullness and the supported module equivalence. Set . Every simple -module survives . If were proper, the nonzero finite quotient would have a simple killed by , a contradiction. Thus write . Multiplication has inverse ; the fullness identity and tensor balancing verify both composites. Also is the canonical isomorphism. These actual maps give inverse equivalences on all supported-block modules. In particular the functor is faithful on that summand, and its kernel on all large finite-image modules is exactly the complementary summand.
The simultaneous central corner and both kernels. The operator commutes with , hence belongs to by the second centralizer. It is central there because every right operator commutes with every left operator. The equivalence of step 4.1 identifies with , so the restriction of is an isomorphism . Its kernel on is . The enlarged stable action is faithful by F1, giving and . On the left, has annihilator , and is faithful for its corner ; the latter need not be a module for all of . Infinite-W kernels are the inverse images of these finite-image kernels.
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 fixed and add full rows, preserving 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.
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 with , allowing repeated roots. Write and for The degenerate cyclotomic Hecke algebra. The generator-preserving tower map embeds in .
For every generalized eigenvalue of in the regular representation of , let be its polynomial generalized-eigenspace projector. All such eigenvalues lie in . These are additive residue chains, separately indexed in each coset of ; coincident roots do not give extra projectors. The are mutually orthogonal, sum to one, commute with and satisfy . They need not be central in .
For finite-dimensional left modules define the residue functors Here the first functor takes its -action from the tower inclusion and the second takes its -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 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 and for . The map is the zero homomorphism , 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 with , the algebras and , finite-dimensional left modules, and inherited AC for the PBW supplier. We prove the nonzero-level assertions and then the level-zero convention.
The bounded PBW basis, polynomial-degree filtration and associated graded algebra are . The generator-fixing anti-involution and the nondegenerate symmetric trace given by the coefficient of are supplied by The degenerate cyclotomic Hecke algebra. These hold for every complex root multiset, including repeated roots.
Finite Chinese remainder interpolation gives the generalized-eigenspace polynomial projectors for a finite-dimensional operator (Chinese remainder theorem for pairwise comaximal ideals).
Proof
The tower map and both finite free structures. The first dot and crossing generators in satisfy the relations of , including the same cyclotomic polynomial in . Their bounded PBW words are a subset of the bounded basis of , so the generator-preserving homomorphism is injective. Let for and ; these are the minimal right coset representatives in , with . The elements , , form a right -basis of . Indeed multiply them by the bounded PBW basis of . In the associated graded algebra their symbols are the distinct bounded words obtained by permuting the first dot exponents by and placing exponent in the omitted position , with permutation , . These run over exactly all bounded words of , so filtered leading-degree induction proves that the products form a basis of . Applying gives the left -basis . Thus both ranks are , and this is valid without any separation of roots.
An actual relative Frobenius trace. Use the two symmetric traces to define uniquely by for every . Nondegeneracy of proves existence and uniqueness. Cyclicity of both traces gives , so is a -bimodule map. The map , , is an -bimodule isomorphism, where the left action on Hom is and its right action is multiplication on the output. To see invertibility directly, identifies this Hom space with : given , define by , which is uniquely determined and -linear. The symmetric -trace identifies with by . Their composite is precisely , 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.
The projectors and residue chains. For each regular-spectrum eigenvalue of , apply [F2] to its annihilating polynomial to obtain . 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 commutes with , so centralizes and is fixed by . Their products and sum give the stated orthogonality and identity. For the root-coset claim use joint dot projectors and , which satisfies and swaps the adjacent dot operators. On a weight with adjacent entries differing by neither nor , this square is invertible by a finite nilpotent geometric series. A leftmost eigenvalue outside 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.
Induction equals coinduction, with explicit inverse. Index the left basis from step 1.1 by and let be its left-coordinate maps, so . Put . Then and . Finite freeness makes the natural map an isomorphism: it sends to and its inverse sends to . Composing with gives the natural -module isomorphism , , with inverse . 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.
The residue Frobenius isomorphism and two adjunctions. Write . For every , one has : pairing either side with under gives by and trace cyclicity. Hence right multiplication by on corresponds under to precomposition by left multiplication by . Restricting the isomorphism of step 3.1 therefore gives as left -modules, with the same explicit relative-trace formula on . The usual tensor-Hom adjunction gives , and the usual restriction-coinduction adjunction gives . Together these prove . The functor is exact as an idempotent summand of restriction; is a right- direct summand of the free module , so 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.
The correct dual tensor comparison. For a left -module write with action twisted by , and write for the same construction on the left -module . The actual natural isomorphism is . It sends a linear functional to , with inverse . The balancing relation and show -linearity and -linearity directly. Composing its inverse with the genuine induction/coinduction isomorphism of step 3.1 gives . The same formulas for the summands give , since and step 4.1 applies. Restriction similarly gives by restricting functionals, with inverse extending by zero on . Thus each residue functor commutes with ordinary -duality. This proof does not identify with its linear dual as an unqualified bimodule.
Projectives and Grothendieck operators. Exact biadjunction proves projective preservation: for projective , is exact, and is exact for projective . The Hom pairing descends to split of projectives and of finite-dimensional modules, because Hom is additive on projective direct sums and exact in its second variable. The two adjunctions compute and . 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.
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 the empty cyclotomic polynomial is , so every positive-degree algebra is zero; the map 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 . Symmetry of alone neither gives the residue bimodule 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.
The higher-level Schur-Weyl endomorphism isomorphism
Statement
Assume the Axiom of Choice. Let be a pyramid with columns , let be an admissible origin, let be the ground simple projective-injective of the relevant summand of the parabolic category of The integral parabolic category-O blocks for higher-level Schur-Weyl duality, and let with . Write for the image of the right cyclotomic Hecke action of The degenerate cyclotomic Hecke algebra and for its central components. Then the right Hecke action gives an algebra isomorphism and on each central component, cut by the central idempotents of acting on , where is the corresponding block of the cyclotomic Hecke algebra. For a nonempty pyramid, in the stable range the image is the full cyclotomic algebra, and ; a single component is not identified with the entire degree- 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 are surjective in all cases, and the full action is injective precisely when for a nonempty pyramid. For the empty pyramid , the degree-zero objects and algebras are , and for they are . All endomorphism identities hold there, and the raw action is faithful in every degree, including the zero-algebra action; is not defined in this branch.
Facts & Assumptions
Given: The pyramid , an admissible origin , the ground object , the tensor object with its central decomposition, and the Hecke image .
The right Hecke action on exists and its generators are natural endomorphisms of the tensor functor, commuting with ; the image is , and the Whittaker functor sends to (Arakawa-Suzuki Casimir operators on tensor functors, The degenerate cyclotomic Hecke algebra, The higher-level Schur-Weyl projective generator and Schur functor).
The Whittaker functor is exact on , its kernel is the Serre subcategory generated by the off-standard simples, 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 (The Whittaker functor is exact and fully faithful on the required projectives, The higher-level Schur-Weyl projective generator and Schur functor).
The filtered double centralizer identifies the two image algebras on for every complex origin: and are mutual centralizers, and in particular ; for a nonempty pyramid, if the full action of is faithful (The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer).
Outside the stable range the image of the Hecke action is a central block corner for admissible origins, and in the stable range (Stable range and block idempotent corner for higher-level Schur-Weyl duality).
Proof
Given: The objects , , the Hecke image , and the admissible-origin hypotheses.
The Hecke action lies in the g-endomorphisms. For the empty pyramid, the empty tensor in degree zero and its ground object give . In positive degree gives , and the level-zero cyclotomic relation is the empty product , so . The stated endomorphism identities and faithfulness follow directly, with the unique zero-algebra map injective; the remaining argument assumes a nonempty pyramid. Each generator of the truncated tensor action is built from the trace Casimir and place permutations and commutes with the diagonal -action; the place permutations are natural in the module variable, so the resulting right -action on consists of -endomorphisms, and its image is by definition. Hence there is a surjection and an inclusion , with the opposite convention fixed by the right action.
The Whittaker comparison is injective. Let be nonzero and put , a nonzero submodule of the finite-length object . Choose a simple submodule ; because , [F2] gives . Exactness gives an injection , and the first module is nonzero, so . Exactness also identifies with the image of , hence . This proves injectivity of . No restriction on all composition factors of is used.
The image of the comparison. On the induced map lands in the centralizer of the finite-W action, ; by the filtered double centralizer [F3] this centralizer equals ; and the induced map contains because every Hecke generator on arises from the corresponding endomorphism of by [F1]. Since is the whole target, the injective map of step 1.2 is also surjective, so .
Stable range. For a nonempty pyramid, if then the action of is faithful by [F3] and the image is the full algebra ; a single central component is correspondingly a block , not the whole algebra. Outside the stable range the corner identification of [F4] applies for admissible origins, while the map remains surjective by step 1.1.
Central components. The central idempotents of the finite-dimensional algebra decompose and ; applying the isomorphism of step 2.1 componentwise gives . The component sits inside the cyclotomic block as the corner by [F4]; it is not the entire degree- algebra.
Failure of raw faithfulness below the stable range. For a nonempty pyramid, suppose and use an enlargement by full ground rows with smallest height at least . In its last column, raise the first entries above their ground values by ; raise its top entry further by , and leave every other entry ground. This is column strict, has total degree , 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 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 of [F4] is proper; the faithful large tensor progenerator makes nonzero also in the large Hecke algebra. The small raw action has the nonzero kernel 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 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 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 on the modules of the Schur functor.
The higher-level Schur-Weyl double centralizer and Schur quotient
Statement
Assume the Axiom of Choice. Fix the pyramid with columns , an origin , a degree , and let be the truncated tensor space with its finite W-algebra image and cyclotomic Hecke image . Then:
- and are mutual centralizers on , for every complex origin ; this is the raw double centralizer.
- For admissible origins, is a progenerator and is a Morita equivalence between -mod and -mod.
- 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 but need not recover every projective.
- For a nonempty pyramid, in the stable range the algebra is the full cyclotomic algebra ; outside the stable range and for admissible origins the central-corner identification is used.
Mutual centralizers alone do not give the Morita statement: the nonadmissible origin example with , and has a nonprojective tensor module while the mutual centralizer identities still hold.
Facts & Assumptions
Given: The pyramid, the origin , the tensor space , the image algebras , , and the tensor object of the relevant parabolic summand.
The raw filtered double centralizer holds for every complex origin; for admissible origins the tensor space is a progenerator and is a Morita equivalence ; the nonadmissible counterexample with , , separates the two assertions (The finite W and degenerate cyclotomic Hecke actions satisfy a double centralizer).
and, componentwise, for admissible origins; the map is surjective with injectivity exactly in the nonempty stable range and also in the trivial empty branch (The higher-level Schur-Weyl endomorphism isomorphism).
The Whittaker quotient 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 is right exact, and recovers 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).
The stable range is ; in it , and outside it the admissible-origin image is the central block corner (Stable range and block idempotent corner for higher-level Schur-Weyl duality, The degenerate cyclotomic Hecke algebra).
Proof
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].
The raw double centralizer. For arbitrary complex origin the filtered leading-symbol lifting argument of [F1] gives and on , with associated graded images the Vust centralizers; this is the all-origin clause and does not use admissibility.
Admissible Morita equivalence. Assume admissible. By the progenerator clause of [F1], is a progenerator for and is a Morita equivalence; by the component clause of [F2] its endomorphism algebra is , so the equivalence is the standard one attached to the -bimodule , identifying -mod with -mod.
The Schur Serre quotient. The composite of the genuine Whittaker functor with the equivalence of step 1.2 is 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.
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 is only right exact and recovers but need not recover every projective; these boundaries are part of the statement and are not repaired by changing conventions.
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 in degree zero and in positive degree. For a nonempty pyramid, if then 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 of [F4], with the component corners 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 (step 4.1). Each consumes a different supplier.
- The left adjoint is used only where it is exact enough: recovering on standard-labelled prinjectives, never for arbitrary projectives.
Schur functor images of standard, simple, projective and tilting objects
Statement
Assume the Axiom of Choice and fix an admissible origin . Let be the Schur functor of The higher-level Schur-Weyl projective generator and Schur functor, . Use the current category-O namespace: is the generalized standard, the costandard, the category-O simple and its projective cover, as in The integral parabolic category-O blocks for higher-level Schur-Weyl duality. The source17 symbol denotes our , not our costandard . Let denote the genuine continuous-dual functor of The Whittaker functor from the relevant parabolic category-O summand, and write for the finite-W image of the category-O simple; for 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 -Hom below takes a finite-W module as its second argument. Let be the standard labels. Then:
- For every label , the Schur image of the standard object is the intrinsic affine-induced Specht module where is the partition of read from the nonnegative ground differences in the -th column of and the factors are induced along the affine Young subalgebra . Its affine action factors through the cyclotomic image , so the same module is obtained by replacing in this tensor product by .
- For the module is simple, the modules , , form a complete set of pairwise non-isomorphic simples of the Hecke image , and for .
- For , is the projective cover of , and ; ambient off-standard projectives still have their genuine images, and no projective-preservation assertion is made for them.
- Images of tiltings carry the opposite-parabolic standard/Specht flag coefficients, and is fully faithful on tiltings.
- For and , , where is the typed canonical-basis coefficient of the Fock-space dictionary; for the symbol is not a Hecke simple. All interfaces are ungraded at parameter .
Facts & Assumptions
Given: The admissible origin , the tensor object , the Schur functor , the standard and costandard objects , the simples , the projectives , and the Hecke image .
In the actual category-O namespace the generalized standards are , the simples are , projective covers are and costandards are . 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 ; they are not standard-flag multiplicities against a costandard.
The Schur functor is exact, kills exactly the off-standard simples, recovers under , and is fully faithful on all projectives and on all tiltings; 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).
The filtered double centralizer identifies , and the Schur quotient is the composite of the genuine Whittaker functor with the Morita equivalence; the stable range gives (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).
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 computes the corresponding multiplicity at parameter (The dual-canonical, canonical and quasi-canonical Fock bases, Simples, projectives and tiltings map to the three distinguished Fock bases).
The cyclotomic Hecke algebra has the bounded monomial basis and the affine evaluation homomorphisms , (The degenerate cyclotomic Hecke algebra).
For each finite-dimensional complex column space , classical Schur–Weyl duality identifies its polynomial highest-weight multiplicity spaces with the ordinary Specht modules, with the length cutoff (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 realizes the corresponding product of symmetric powers; its Young-symmetrizer quotient has the Specht fibre.
Proof
Given: The standard , the costandard , the labels of , 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 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.
A regular corner in the stable realization. Add full ground rows until there are distinct rows of length , and choose one rightmost box in each such row; let be their ordered tensor and 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 , , , 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 by triangularity, and its cardinality is . Thus identifies with the right regular -module. Put . Since is regular, by evaluation at . Consequently , characterized by , is an algebra isomorphism, and identifies with for every finite-image module . The left Hecke action on this corner is , not the naive right action on .
The cyclic symmetric generator and its bottom quotient. Write , retaining exclusively for the cyclotomic roots, and form the actual cumulative-column -module . Its bottom column degree is ; the higher-degree part is a -submodule, and is the inflated Levi module . Put and . Apply these commuting factors one tensor place at a time, starting with the first place, and within each place in descending column order . The actual dot formula gives , where has the ordered rows of and column sequence prescribed by ; subtracting cancels the scalar at column and moves that box one column left. Hence . More generally the vectors , with and ranging over cosets of , have distinct leading symmetrized tensors and span by the ordinary symmetric-tensor basis. Thus this vector generates as a corner module, and its image generates . These are actual vector identities and triangular basis statements, rather than a character identification.
The affine colour fibre. Ordinary Levi Schur-Weyl gives on the canonical colour fibre, where is the symmetric-group permutation module. Its vectors in the corner are with . For , the identity and commutativity of dots give . In the bottom quotient the dot formula has scalar : 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 acts as on that canonical fibre. The affine cross relations then determine the remaining dots as plus their within-block Jucys-Murphy sums. This proves that the fibre inclusion is a homomorphism for the affine Young subalgebra , with module , and its image generates the entire corner by step 2.1.
The genuine Specht isomorphism. The Levi Young-symmetrizer map gives an actual quotient and hence a -quotient . The canonical colour fibre quotient is , by ordinary Levi Schur-Weyl. The affine fibre map in step 3.1 descends through this actual quotient and still generates: is exact and the generating vector of its source maps onto a generator of its quotient. Affine induction therefore gives a surjection . The multilinear row-weight part of has one summand for each allocation of the distinct rows into ordered colour subsets of sizes , and on each subset its weight space is the polytabloid Specht space. Its dimension is . 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 , preserving the actual Hecke maps.
Descent to the original pyramid. Extend the original label by the added ground rows, producing a contractible large label . Its column partitions and roots are unchanged. The actual original-path/zero-occupancy compression in [F3] gives and , with the faithful supporting-block Morita equivalence and natural Hom comparison. Every simple constituent of has the same entry-multiset central character as ; the bottom-row minimum argument forces every such label to be contractible. Hence the supporting central idempotent satisfies , and the Hom comparison identifies the original 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.
Tilting images and full faithfulness. The opposite-parabolic flag coefficients are the actual tilting-character coefficients of [F1] and [F4]; exact 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 , is equivalent to and has right adjoint . 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.
Simple images and heads. Here uses the genuine continuous-dual functor, rather than raw Whittaker vectors in . The finite-W simple-image classification and the genuine Morita equivalence in [F2] and [F3] imply that is simple for , that these are distinct and exhaustive, and that otherwise. For a standard label , the cover is an indecomposable summand of , so is an indecomposable projective. Its simple quotients are determined by , which has dimension ; this is the ordinary equivalence on and the simple-image computation. Thus has head . Lift the cover through using projectivity; the lift is surjective since the latter is the simple-head quotient and any proper submodule of lies in its radical. Exactness yields . Every nonzero quotient of the indecomposable projective has the same simple head : its kernel is contained in the unique maximal submodule. Therefore has head .
Projective images. For , the preceding step shows that is the indecomposable projective with simple head , hence its projective cover. Evaluation is an isomorphism because : this is checked on and restricted to its idempotent summands. Thus . Off-standard projectives retain their actual images, and no projective-preservation assertion follows for them.
Multiplicities. Since is exact and its kernel is generated by the off-standard simples, the composition multiplicities of are the multiplicities of the simple in for ; by the Fock-space dictionary [F4] the typed coefficient of the dual-canonical/canonical pairing equals , so ; for the module is zero and is not a simple Hecke label. All the identifications above are ungraded and taken at parameter .
Remarks
- The intrinsic definition of by parabolic induction replaces the faulty direct identification of the source with the corner/regular-vector computation: the canonical colour fibre is only one of several fibres of , 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.
Category-O translation intertwines residue induction and restriction
Statement
Assume the Axiom of Choice and fix an admissible origin ; let be the residue translation functors on the sum of parabolic blocks of The residue translation functors on the sum of parabolic blocks and put , the tensor image algebra of Stable range and block idempotent corner for higher-level Schur-Weyl duality. Use its generator-preserving image-tower map . If is the generalized- projector of the last dot in , define the image residue functors by 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 where 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 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 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 , the tensor objects and , the Schur functors , and the residue functors on both sides.
The O-side residue functors are exact, biadjoint, preserve projectives and injectives, commute with restricted duality, and agree with the generalized Casimir eigencomponents; their 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).
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 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.
The Schur functor is exact, kills exactly the off-standard simples and sends standards to intrinsic Specht modules. Its tensor detector is prinjective, its Hecke endomorphism algebra is , and its Whittaker image is a projective generator of the corresponding finite-W image category. There are natural identifications and the coherent tensor isomorphisms , with intertwining the tower generators. In the stable realization is the full cyclotomic algebra, while content projections give the supported blocks. Every category-O projective has a copresentation with . 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.
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
Given: The tensor identity , the actual Whittaker/Morita tensor data of [F3], and the two pairs of residue functors.
Restriction uses the dual natural module. For in the degree- summand and a basis of with dual basis , tensor adjunction gives the natural map , . Its inverse sends to . These maps are basis-independent by coevaluation and evaluation and commute with the first tower generators, acting on the factors. Thus they identify restriction of with after the appropriate degree/block projection. The natural and dual natural modules are distinct -modules; no identification between them is used.
The induction map is an actual tensor map. Tensoring an endomorphism of with gives the image-tower homomorphism ; it sends the unit to the unit and the first generators to their tensor actions. For of degree , put , , where is the right action on . The first generators act on , so this expression is balanced over and is -linear for the left-module convention; naturality follows by postcomposition. To prove it invertible, on the finite-W side form . For this is the regular-module isomorphism . 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 , and both sides are right exact: induction is right exact, tensoring with is exact and Hom from is exact. Passing to cokernels proves invertible for all . 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 square of [F3] sends by either route to ; -linearity then makes the square commute on every . Consequently is invertible for every . This presentation argument takes place in the finite-W image category, where is a full projective generator; it does not assert that is a full category-O generator.
The two residue projectors. The tower's last dot on is the tensor Casimir, with the normalization of [F1]. Hence intertwines its generalized- eigenprojector with the projector defining . On the dual tensor factor one has the actual operator identity . Indeed and equivariance of give the first term and the second term , exactly that identity. Thus the last-dot generalized- projector corresponds to the dual-Casimir generalized- projector, including its nilpotent part. This is the actual adjunction mate and agrees with the flag normalization in [F1]. Under the last-dot projector therefore corresponds to the generalized- projector defining . Applying the source content projector and target projector to steps 1.1–1.2 gives and . Polynomial generalized-eigenspace projectors commute with these natural maps because the maps intertwine the operators, proving the asserted residue compatibility.
The natural duality comparison. The ordinary category-O duality 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 ; the Casimir, crossings and content projectors are self-adjoint. Put with and with the same twist. The detector form gives an actual isomorphism , . Exact restricted contravariant duality, with its canonical bidual map, consequently gives . Its explicit map is ; its inverse sends to . 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 , while the symmetric trace of [F2] gives by . Define by . The displayed form identity makes it balanced over and -linear. Applying gives a natural transformation between exact functors. It is an isomorphism on 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 . 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 separately. Thus and . None of this identifies the usual tensor dual with .
Grothendieck operators and quotient. Exactness of and of the residue functors makes the natural isomorphisms of step 2.1 induce and . On , the source simple-class basis shows that is exactly the span of the off-standard simple classes, and the induced map from this quotient onto is an isomorphism. No isomorphism from the entire category-O Grothendieck group is asserted. On split projective groups only 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 . When the selected contents are fully supported, is their full cyclotomic cut, so the same comparisons apply to that cut.
Adjunction maps. The first tensor unit is the coevaluation , and the tensor counit is evaluation. The induction/restriction unit is , and the counit is . Substituting these formulas into and gives the same composite maps, term by term: coevaluation is precisely the sum in , and evaluation cancels that sum by . Restricting the commuting squares by the content and residue projectors proves compatibility for . 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.
Filtrations and boundaries. Applying exact 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 and the lowering tensor factor is . 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.
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