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Finitary Ringel–Hall Algebras
1 · Prerequisites
- Abelian Categories
- Adjunctions Units and Counits
- Binary Operations, Monoids, Groups and Subgroups
- Cardinal Arithmetic, Cofinality and the Alephs
- Categories, Functors and Natural Transformations
- Congruences, the Integers Modulo n and the Chinese Remainder Theorem
- Construction of the Natural Numbers
- Construction of the Real Numbers via Cauchy Sequences
- Construction of the Real Numbers via Dedekind Cuts
- Cosets, Index and Lagrange's Theorem
- Countability and Uncountability
- Determinants of Matrices over a Commutative Ring
- Diagonalisation and the Minimal Polynomial
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Divisibility, Greatest Common Divisors and Bézout's Identity
- Eigenvalues, Eigenvectors and the Characteristic Polynomial
- Exactness and the Member Calculus
- Finite Counting, Factorials and Binomial Coefficients
- Formal Power Series
- Foundations of the Real Numbers for Analysis
- Fundamental Trigonometric Identities
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Limits and Colimits
- Linear Independence, Bases and Dimension
- Linear Transformations, Rank-Nullity and Quotient Spaces
- Matrices, the Matrix of a Linear Map, and Change of Basis
- Normal Subgroups and Quotient Groups
- Order, Zorn's Lemma, and the Axiom of Choice
- Ordinal Arithmetic and the First Uncountable Ordinal
- Ordinals, Cardinals, and Transfinite Recursion
- Polynomial Rings, the Division Algorithm and Roots
- Preadditive and Additive Categories and Biproducts
- Primes, Euclid's Lemma and the Fundamental Theorem of Arithmetic
- Reflective Subcategories and the Adjoint Functor Theorems
- Relations, Functions, and Quotients
- Rings, Subrings, Integral Domains and Fields
- Roots, Rational Powers, and Classical Inequalities
- Simple Field Extensions and the Construction of the Complex Numbers
- Splitting Fields
- Subobject Lattices Generators and the Grothendieck Axioms
- Symmetric Functions, the Hall Inner Product, and Schur Bases
- Symmetric Groups, Cycle Decomposition and the Sign Homomorphism
- Symmetric Polynomials and the Fundamental Theorem of Symmetric Functions
- The Determinant of a Linear Operator, Cofactors and Cramer's Rule
- The Diagram Lemmas in an Abelian Category
- The ZFC Axioms and the Basic Set Constructions
- Triangularisation, Generalised Eigenspaces and Jordan Canonical Form
- Vector Spaces, Linear Subspaces, Span and Direct Sums
- Yoneda Extensions and Homological Dimension
- Young Diagrams Tableaux and Permutation Modules
2 · Summary
Objective
This page constructs the untwisted Hall algebra of a small finitary abelian category over an arbitrary commutative coefficient ring. With the fixed convention that counts subobjects isomorphic to with quotient isomorphic to , its local proofs establish finite coefficients, finite support, the zero-object unit, and associativity by counting two-step flags. They use finite Hom sets and finite Yoneda sets; they do not assume finite-field linearity, enough projectives or injectives, or a finite-subobject condition for every object.
A separate finite-field specialization develops the Jordan-quiver Hall algebra. It proves the partition classification, Hall-polynomial structure constants, and the generator-normalized isomorphism from its generic algebra to the stable symmetric-function ring. The normalized partition basis is identified with the monic Hall–Littlewood functions, and the inverse- automorphism Green pairing is computed in power-sum coordinates by an independent pair-of-flags count. The companion examples page records worked examples and the degree-two normalization checks.
Reading route and logical suppliers
The canonical plan declares three page-level reading prerequisites: algebraic-representation-and-tensor-symmetry-map, cyclotomic-klr-algebras-and-highest-weight-categorification, and symmetric-functions-hall-inner-product-and-schur-bases. The first two give broader algebra and categorification context and are not item-level premises. Results from the symmetric-functions page enter through their individually cited item dependencies. In particular, the published quiver-flag/KLR convolution theorem is a distinct construction and does not establish Hall product associativity.
Normalization and scope
The coefficient is an integer count of subobject classes. Its image in the coefficient ring is formed by repeated addition; no automorphism cardinality is divided out. The square-root Euler twist, Green coproduct and quantum-group comparison have additional hypotheses and belong to later pages.
The Hall product is a multiplication on the Hall module. The Hall inner product on symmetric functions is a separate bilinear form, defined by The Hall inner product on symmetric functions. The generic ring isomorphism uses . The local Jordan Hall classes are Hall–Littlewood functions with the transported Green pairing proves . The transported Green form on degree is times the standard Hall–Littlewood form at parameter ; its power-sum norms are . These are distinct from the ordinary Hall inner product. This Jordan pairing computation requires no general Green coproduct theorem.
3 · Logical flowchart
4 · Definitions, theorems and proofs
Small finitary abelian categories for Hall multiplication
Definition
A small finitary abelian category for Hall multiplication is a small abelian category (its object and morphism collections are sets, by Small, locally small, and large categories), with abelian structure as in Abelian category, in which the following sets are finite for every pair of objects :
- ;
- , the set of Yoneda classes of short exact sequences . Equivalence is the one-fold instance of the generated endpoint-fixed chain-map relation in Equivalence of n-fold extensions: chain maps are the identity on and , and the relation is closed under reflexivity, symmetry and transitivity. A short exact sequence and its endpoint order use Exact sequence and short exact sequence in an abelian category, An extension of an object by an object in an abelian category and An n-fold Yoneda extension.
One may instead supply a small skeleton of an essentially small abelian category and perform the construction on . Here “essentially small” means that such a small equivalent category is part of the given data; the construction does not select representatives by an unstated choice principle. The isomorphism classes then form a set.
No -linear structure, enough projectives or injectives, finite number of subobjects of every object, or identification with derived is included in this definition. Subobjects are the monomorphism classes of Subobject and quotient object as mutual-factorisation classes of monomorphisms and epimorphisms, and quotients are the cokernels specified in The quotient of an object by a subobject.
Flags lift uniquely through a quotient in an abelian category
Statement
Let be a subobject in an abelian category, and let be the quotient map. Inverse image along is an order isomorphism from the subobjects of to the interval of subobjects with . Its inverse sends to the image , canonically isomorphic to . Under this correspondence,
Facts & Assumptions
Given: An abelian category, subobjects , and the quotient map .
A subobject is a mutual-factorisation class of monomorphisms; its quotient is the cokernel of a representing monomorphism (Subobject and quotient object as mutual-factorisation classes of monomorphisms and epimorphisms, The quotient of an object by a subobject).
Direct image is the image of the composite with the given map, and inverse image is its pullback (Direct and inverse image of a subobject).
Direct and inverse image form the Galois connection (Direct and inverse image of subobjects form a Galois connection).
Pulling back an epimorphism in an abelian category gives an epimorphism (The pullback of an epimorphism is an epimorphism).
For every morphism , is canonically isomorphic to (First isomorphism theorem in an abelian category).
For nested subobjects , (Third isomorphism theorem in an abelian category).
Every monomorphism is the kernel of its cokernel (Every monomorphism is the kernel of its cokernel, and dually every epimorphism is the cokernel of its kernel).
Proof
Given a subobject , let be its inverse image. Since , [F3] gives . The pullback square defining has a projection that is epic by [F4]; its kernel is the kernel of . By [F5], its image is canonically . Since is epic, any cokernel satisfies , so by cancellation. Its universal property makes its codomain initial, because the only morphism out of annihilating is zero; hence the cokernel object is zero. By the image definition, . Thus and .
Conversely let . The restriction has kernel , so [F5] identifies its image with . By [F6], the quotient map , composed with , is the quotient map . Its kernel is by [F1] and [F7], hence the inverse image of along is exactly .
Steps 1.1 and 1.2 show that the two assignments are inverse on subobject classes. Both assignments preserve inclusion by the Galois connection [F3], and [F6] gives the stated quotient identification. Thus inverse image along is the claimed order isomorphism.
Diagram
The quotient correspondence is represented by the following exact rows and the induced inclusion:
The vertical middle map is the subobject inclusion, and the right-hand map is the map induced by . The diagram explains the correspondence; the proof above uses the categorical universal properties and the third isomorphism theorem, not the picture.
Nilpotent representations of the Jordan quiver
Definition
The Jordan quiver has one vertex and one loop, labelled :
A finite-dimensional representation over a field is a pair , where is a finite-dimensional -vector space and is nilpotent (Nilpotent endomorphisms and their nilpotency index). A morphism is a linear map satisfying , encoded by the commutative square
For this page, denotes the small model whose objects are , for , with a nilpotent matrix, and whose morphisms are all matrices intertwining the endomorphisms. Every finite- dimensional vector space is isomorphic to a standard , so the model represents all finite-dimensional nilpotent representations. For any field , write for the one-dimensional object and for the length- Jordan block, using Jordan blocks, Jordan strings, and their endpoints. For a partition (Partitions, English diagrams, and conjugation), write for the block-diagonal representation with blocks . Use for the zero object.
The untwisted Hall algebra of a finitary abelian category
Definition
Let be a small finitary abelian category in the sense of Small finitary abelian categories for Hall multiplication, and let be a commutative ring with unit. Define the free -module where is a basis symbol for the isomorphism class of . For objects , let This is a finite set by the Hom condition in Small finitary abelian categories for Hall multiplication. For in this set, write when for an isomorphism ; this is an equivalence relation by Isomorphism, groupoid, and connected category. The quotient set represents exactly the subobjects of isomorphic to : each class gives the usual subobject class from Subobject and quotient object as mutual-factorisation classes of monomorphisms and epimorphisms, and the mutual- factorisation theorem says two such monomorphisms give the same subobject exactly when they differ by such an isomorphism (Mutual factorisation is an equivalence relation on monomorphisms into an object and dually on epimorphisms out of it). Every subobject class with domain isomorphic to is represented by composing its monomorphism with an isomorphism from , one class at a time. The cokernel quotient is independent of that representative by The quotient by a subobject is independent of the chosen representing monomorphism and The quotient of an object by a subobject. Define to be the number of classes for which . The finiteness lemma below also proves that the resulting product has finite support. Extend the operation -bilinearly, mapping each natural number coefficient to its multiple of . The order is fixed: the counted short exact sequence is
This is the untwisted Hall product. It does not use an Euler form, a square root of a field size, or division by automorphism cardinalities. The finite coefficient and finite-support claims needed for the operation to define a bilinear product are established in Untwisted Hall structure constants and products are finite ↗.
Jordan-quiver categories are abelian; finite-field models are finitary
Statement
For every field , the category of Nilpotent representations of the Jordan quiver is abelian, and its subobjects are exactly the -invariant subspaces of each object . When is finite, is small and its Hom sets and Yoneda sets are finite. Thus it satisfies the finitary hypotheses of Small finitary abelian categories for Hall multiplication.
Facts & Assumptions
Given: A field and the category ; when is finite, two fixed objects for the extension-count argument.
Objects are finite-dimensional vector spaces with nilpotent endomorphisms; morphisms are the intertwining linear maps satisfying (Nilpotent representations of the Jordan quiver).
Finitary means that the category is small or is supplied with a small skeleton and that Hom and Yoneda sets are finite (Small finitary abelian categories for Hall multiplication).
An abelian category is additive, has kernels and cokernels, and its canonical coimage-to-image maps are isomorphisms (Abelian category).
Here a monomorphism is a morphism cancellable on the left.
A subobject is a mutual-factorisation class of monomorphisms into its target (Small finitary abelian categories for Hall multiplication).
Proof
Fix a morphism intertwining two nilpotent endomorphisms. Its kernel and image are invariant, and the induced endomorphism on its cokernel is nilpotent. Intertwining maps are closed under addition, composition is bilinear, and the ordinary finite direct sums with diagonal endomorphisms and the zero object have their vector-space biproduct universal properties. Choose bases for the kernel, image, and cokernel of this one map and transport them to standard objects; their universal properties are preserved. The coimage-to-image isomorphism is an intertwiner because commutes with the endomorphisms. This verifies the abelian-category clauses in [F3].
For any field , the standard-coordinate objects and matrices between them form sets, since they are a union indexed by pairs of natural numbers of sets of matrices over ; hence is small. If is finite, there are finitely many matrices of each size, and each Hom set is a subset of a finite set of matrices, so Hom sets are finite.
Now suppose is finite and fix objects and . In a short exact sequence , the middle space has dimension . After identifying it with , only finitely many nilpotent matrices and endpoint maps are possible. Thus the set of such sequences, and its quotient by Yoneda equivalence, are finite.
A monic intertwiner is injective: if has a nonzero kernel vector , the source nilpotent operator preserves . Choose the least with ; then is nonzero, lies in the kernel, and satisfies . The map sending to is nonzero and intertwines, but its composite with is zero, contradicting left cancellation [F4]. Conversely, every injective intertwiner is monic by linear injectivity.
By step 1.4, every monomorphism identifies its domain with an invariant subspace of its target. Conversely, every invariant subspace carries the restricted nilpotent endomorphism; choosing a basis for this single finite-dimensional subspace and transporting the endomorphism to represents its inclusion by a monic map in the standard-coordinate model. Two such monic maps have the same image exactly when they mutually factor: maps with the same image are related by the induced intertwining isomorphism of their domains, and mutual factorisation forces both image inclusions. By [F5], this is precisely equality of subobject classes.
The category is abelian by step 1.1 and small by step 1.2. For finite , its Hom and Yoneda extension sets are finite by steps 1.2 and 1.3, exactly the finitary conditions in [F2]; step 2.1 proves the stated subobject description for every field.
Jordan-quiver isomorphism classes are indexed by partitions
Statement
Every object of is isomorphic to a unique direct sum , where is a partition. The unique simple object is .
Facts & Assumptions
Given: A field and a finite-dimensional vector space with a nilpotent endomorphism , defining an object of .
Every finite-dimensional nilpotent endomorphism has a basis that is a concatenation of Jordan strings, including the empty basis on the zero space (Every finite-dimensional nilpotent endomorphism has a basis of Jordan strings).
For a nilpotent endomorphism, the numbers of Jordan blocks of each size are determined by the ranks of its powers (Ranks of shifted powers determine Jordan form up to block order).
In a Jordan string of length , and for ; its matrix is (Jordan blocks, Jordan strings, and their endpoints).
A partition is a finite weakly decreasing sequence of positive integers; its parts record a multiset uniquely (Partitions, English diagrams, and conjugation).
is a category whose objects and morphisms are finite-dimensional nilpotent representations and their intertwiners (Nilpotent representations of the Jordan quiver).
Here a simple object means a nonzero object whose only subobjects are the zero subobject and the identity subobject.
Subobjects in correspond to invariant subspaces, via their images (Jordan-quiver categories are abelian; finite-field models are finitary).
Proof
Apply [F1] to . The spans of its Jordan strings are invariant, their concatenation is a basis of , and by [F3] each span is isomorphic as a representation to the block whose length is that string's length. Sorting these finitely many positive lengths weakly decreasing gives a partition by [F4] and an isomorphism . The zero space gives the empty partition.
If , the intertwining isomorphism conjugates their nilpotent matrices, so the ranks of every power agree. By [F2], the multiplicities of blocks of each length agree; hence the multisets of parts and the partitions are equal.
If a string has length , the span of its initial vector is a nonzero proper invariant subspace, hence a proper nonzero subobject by [F7]; therefore is not simple by [F6]. The object is nonzero and has only the zero and whole subspaces, so it is simple by [F6] and [F7]. Any decomposition in step 1.1 with at least two summands has a proper nonzero invariant summand and hence is not simple. A single summand is simple only when it has length one. Thus is the unique simple object.
Untwisted Hall structure constants and products are finite
Statement
For a finitary abelian category, each untwisted Hall coefficient is finite and depends only on the isomorphism classes of . For fixed , only finitely many isomorphism classes have . Hence the basis formula in The untwisted Hall algebra of a finitary abelian category is a finite sum in its direct-sum module.
Facts & Assumptions
Given: A finitary abelian category , objects , and the coefficient from the untwisted Hall product.
For every pair , the sets and are finite; the latter consists of Yoneda classes of short exact sequences with the displayed endpoints (Small finitary abelian categories for Hall multiplication).
counts equivalence classes of monomorphisms under precomposition by isomorphisms of , retaining those whose cokernel is isomorphic to (The untwisted Hall algebra of a finitary abelian category).
A morphism between short exact sequences that is the identity on both endpoints is an isomorphism on the middle object, by the short five lemma (Short five lemma in an abelian category).
Proof
An isomorphism of middle objects transports subobjects and induces an isomorphism of their cokernel quotients; replacing either endpoint by an isomorphic object preserves the two type conditions. Thus the count in [F2] depends only on .
For fixed , the equivalence classes counted by [F2] are a quotient of the finite set from [F1]. The subset whose cokernel is isomorphic to is therefore finite.
Every elementary map in the generating relation for [F1] preserves the middle-object isomorphism class by [F3], and so does its reflexive, symmetric and transitive closure. Thus taking the middle-object class defines a map from the finite set . If , a counted subobject and quotient give a short exact sequence after transporting its endpoints by isomorphisms, so lies in the image. That image is finite, proving finite support without simultaneous choices of extension representatives.
Each coefficient is a natural number and the support is finite by steps 1.2–1.3. Mapping an integer to therefore gives a well-defined element of the direct sum in [F2], with no automorphism denominator or additional finiteness condition.
The untwisted Hall product is associative and unital
Statement
For every small finitary abelian category and commutative coefficient ring , the operation of The untwisted Hall algebra of a finitary abelian category is a well-defined associative -bilinear multiplication on , with unit , the basis symbol of the zero object.
Facts & Assumptions
Given: A small finitary abelian category , a commutative ring with unit, and the product convention .
The product coefficient counts subobjects with quotient , and the natural-number counts are mapped to (The untwisted Hall algebra of a finitary abelian category).
Each coefficient is finite and, for fixed , only finitely many middle-object classes occur (Untwisted Hall structure constants and products are finite).
For a fixed quotient , subobjects of it correspond bijectively to flags , with (Flags lift uniquely through a quotient in an abelian category).
Every monomorphism in an abelian category is the kernel of its cokernel (Every monomorphism is the kernel of its cokernel, and dually every epimorphism is the cokernel of its kernel).
Proof
Fix basis objects . The coefficient of in is the sum over isomorphism classes of . By [F1], this counts a subobject with and , together with a subobject with and . The quotient class is uniquely determined by , so this sum counts exactly these pairs.
By [F3], each such pair corresponds to exactly one flag with , , and . The coefficient of in counts the same flags: first choose with , , then choose with , , summing over the uniquely determined class .
The only subobject isomorphic to zero is the zero subobject, and the only subobject with zero quotient is the whole object: in the latter case the inclusion has zero cokernel and hence is an isomorphism by [F4]. Thus exactly when , while exactly when . The zero-object symbol is a two-sided unit.
The two parenthesizations therefore have the same coefficient at every basis vector , so for basis elements.
Basis products have finite support by [F2]. Every element of is a finite linear combination of basis vectors, so bilinearity extends the basis calculation in step 2.1 to all triples and preserves finite support. Step 1.3 supplies the unit, proving the statement.
The generic Jordan-quiver Hall algebra is the symmetric-function ring
Statement
Let , and let denote the nilpotent Jordan-quiver representation indexed by a partition , as in Jordan-quiver isomorphism classes are indexed by partitions. For partitions , let be the coefficient of in the untwisted product . There are polynomials , independent of the finite field, with A coefficient is zero unless .
Define the generic Jordan-quiver Hall algebra by giving degree and degree . The size condition above makes this a graded algebra. Then is a commutative associative unital algebra and a free polynomial algebra over on the classes , . After extending scalars to , the assignment for every , and , extends uniquely to a graded algebra isomorphism where is the stable graded ring of symmetric functions.
Facts & Assumptions
Given: A finite field , its cardinality , the Jordan-quiver category , and an integer when a simple direct-sum multiplicity is used.
The untwisted product coefficient counts subobjects with quotient , and its structure constants lie in the natural numbers before their image in a coefficient ring (The untwisted Hall algebra of a finitary abelian category).
The product is finite-support and associative, with zero-object unit (Untwisted Hall structure constants and products are finite, The untwisted Hall product is associative and unital).
The category is finitary over every finite field, and its subobjects are the invariant subspaces (Jordan-quiver categories are abelian; finite-field models are finitary).
Isomorphism classes are the partition-indexed objects , and each is a direct sum of Jordan blocks (Jordan-quiver isomorphism classes are indexed by partitions).
Flags in a quotient lift to flags between the kernel subobject and the whole object (Flags lift uniquely through a quotient in an abelian category).
A nonzero real polynomial of degree has at most distinct real roots (A nonzero real polynomial of degree has no more than distinct real roots).
Partition conjugation is a bijection on partitions (Partitions, English diagrams, and conjugation).
The stable symmetric-function ring is , freely generated by its elementary symmetric functions (The stable graded ring of symmetric functions, Elementary and complete families freely generate the stable ring).
For each prime , is a field with exactly elements (For every prime , the two operations on make it a field, For , every class in has one representative with , so ; while is in bijection with ).
There are infinitely many primes (Euclid's theorem: for every and every list of primes there is a prime not among ; consequently the set of primes is not finite).
Proof
If , then : the coefficient of in is when and , and is otherwise, so it is a constant polynomial. Now suppose is nonempty, with its largest part, and let act on , with . By [F1], the coefficient of in counts subobjects isomorphic to with quotient type . By [F3], these are exactly the -dimensional subspaces , since acts as zero on .
The Gaussian counts are polynomial in : for , fixing a hyperplane gives , with boundary values . In the second term, after choosing the -dimensional intersection with the hyperplane, the remaining one-dimensional subspace in the quotient has choices outside the quotient hyperplane. Induction on gives polynomials in .
Finite-dimensional duality sends to . If is -invariant, its annihilator is -invariant, and dualizing exchanges the subobject and quotient. A Jordan block is isomorphic to its transpose by reversing its Jordan-string basis, so [F4] gives . This bijection proves ; each finite-field Hall algebra is commutative.
For the nonempty partition in step 1.1, put for , with and . Each Jordan block of size contributes one dimension to exactly when , so . For a counted subspace set , , and . Let be the operator induced by on . Write . The map is onto with kernel ; also . Since , quotienting by gives For a nilpotent Jordan type with block multiplicities , the number of blocks of size is the second difference . Applying this formula to shows that its multiplicity of blocks of size is with all beyond .
Let . For a valid profile, . Choosing the graded subspaces contributes possibilities. For fixed graded subspaces, build their lifts from the top of the flag down: at level , each lift is the graph of a linear map from an -dimensional space to , giving choices. Multiplying these independent choices gives Thus this power of times the displayed product counts all subspaces with the chosen intersection dimensions.
For fixed , each profile has integers with , so there are finitely many profiles. Keep exactly those whose block multiplicities from step 2.1 equal for every . These constraints are independent of the field by [F3]–[F4]. Summing the polynomial counts from steps 3.1 and 1.2 over the retained profiles proves that every coefficient in is a universal polynomial in .
For the empty partition define , the empty product; its only nonzero coefficient is the unit coefficient at . For a nonempty partition , put and form By step 4.1 and associativity [F2], every coefficient is a polynomial in . Parenthesize the product as . For the coefficient is the single one-step flag counted by the basis coefficient. For , the induction hypothesis says the inner coefficient counts flags of length in an intermediate object . The outer product [F1] chooses with ; an isomorphism identifies the inner flags with flags in this quotient, and any such isomorphism induces a bijection, so the count is independent of the isomorphism chosen. By [F5] each quotient flag lifts uniquely to a flag containing , and its quotient clause identifies each lifted successive quotient with the corresponding quotient in the quotient flag. Thus the coefficient of counts exactly flags with .
For every such flag, , hence . Each Jordan block of length contributes to , so . For the type itself, the kernels form a valid flag: each induced endomorphism on is zero and the quotient has dimension , so it is isomorphic to . If all these kernel dimensions agree for another type , their block multiplicities agree by second differences, so ; the flag is then forced to be the kernel flag just constructed and is unique. On partitions of a fixed total size, order types by componentwise comparison of these kernel dimensions; antisymmetry follows from the second-difference formula. Therefore where means all kernel dimensions are at least those of , with at least one strict inequality.
In each fixed total dimension there are finitely many partitions. The transition matrix in step 6.1 is triangular with diagonal entries one and polynomial entries from steps 4.1 and 5.1, so it is invertible over by recursive substitution. Thus every is a polynomial combination of monomials in the semisimple classes. For each finite field, use associativity [F2] and commutativity from step 1.3 to parenthesize and reorder a product of two such monomials so that one basis term is successively multiplied by simple-sum factors on the right. Induction on the number of factors and step 4.1 then show that every structure constant is the value at of a polynomial .
Each coefficient polynomial is unique: the difference of two candidates vanishes at every field cardinality, and by [F9]–[F10] this includes infinitely many distinct prime cardinalities. A nonzero polynomial in remains nonzero in because is injective; by [F6], it cannot have infinitely many distinct real roots. Thus is well-defined. Each product is finite because a short exact sequence adds vector-space dimensions, and only finitely many partitions have a fixed size. For a fixed triple of basis classes, the associativity defect is therefore a polynomial in ; it vanishes at every field-cardinality specialization by [F2], hence at infinitely many distinct prime cardinalities by [F9]–[F10]. Its coefficients embed injectively from into , so [F6] implies that the defect is the zero polynomial. The same argument using step 1.3 proves commutativity. The unit equations likewise hold as polynomial identities because they hold at every field-cardinality specialization by [F2], so is the generic unit.
The monomial in step 5.1 uses the generators with exponents , which are exactly the parts of the conjugate partition . Since partition conjugation is a bijection, these run through every polynomial monomial in the generators . Their unitriangular expansions in step 6.1 show that they are also a -basis. Together with the coefficient polynomials from step 7.1, this proves the natural map from to is an isomorphism.
By [F8], the target symmetric-function ring is the polynomial ring . After adjoining , each scalar is a unit. Define and send each free generator to ; this defines an isomorphism of polynomial algebras, with inverse sending to . Each generator and its image have degree , and has degree zero, so the isomorphism preserves the grading.
Hall–Littlewood scalar product and monic functions
Definition
Let be an indeterminate and work in , the scalar extension of The stable graded ring of symmetric functions. For a partition , let be the multiplicity of its part , and put The Hall–Littlewood scalar product is the symmetric bilinear form with This defines a nondegenerate form, because the power sums are a rational basis (Power sums form a rational but not integral stable basis) and all displayed diagonal entries are nonzero. Different degrees are orthogonal; empty products are , so .
The monic Hall–Littlewood functions are characterized by where is strict dominance (Dominance order on partitions) and the monomials use The monomial symmetric functions form the integral stable basis. Existence, uniqueness, and the norm formula are proved in Jordan Hall classes are Hall–Littlewood functions with the transported Green pairing ↗, rather than assumed in this definition. Set . For a real parameter the same formulas specialize wherever used below; the theorem proves their regularity there. This form differs from the ordinary symmetric-function Hall inner product, whose power-sum norms are .
Automorphism counts for nilpotent Jordan representations
Statement
For the nilpotent Jordan representation over , write and . Then In particular .
Facts & Assumptions
Given: A finite field of cardinality , a partition , and with its nilpotent operator denoted .
The representation is the direct sum of blocks with multiplicities (Jordan-quiver isomorphism classes are indexed by partitions).
Conjugate partition columns have heights (Partitions, English diagrams, and conjugation).
In a nilpotent Jordan-string basis , the operator satisfies and for ; its matrix is (Jordan blocks, Jordan strings, and their endpoints).
Proof
For the Jordan-string basis of , we have and for . Give the -module structure in which acts by its nilpotent operator. The linear map sending to for is a bijection commuting with , hence a module isomorphism. Intertwining linear maps are exactly module homomorphisms. A module homomorphism is determined by the image of , which may be any vector killed by ; that space has dimension . Thus the endomorphism algebra of has dimension . Counting each column's ordered pairs of boxes gives : in a column of height , its square is .
Consider the induced map of an endomorphism on . Ordered by block length, its matrix is block triangular: a homomorphism from length to a larger length has image of divisible by and hence has zero reduction in the target head. Its diagonal blocks are arbitrary matrices ; all choices occur independently by constant matrices between blocks of the same length. The linear map from the -dimensional endomorphism space to these diagonal blocks is onto, with every fiber of size .
The map is invertible exactly when all are invertible. Necessity follows from invertibility on the quotient. Conversely those blocks make the triangular head map surjective, so . Since commutes with , iteration gives for every , and nilpotence makes the last summand zero for large . Thus is onto and, on a finite-dimensional vector space, bijective; its inverse commutes with .
Successively choosing linearly independent columns gives , including . Hence the two preceding steps count the automorphisms as . Substitute from step 1.1. For the space is zero and its sole automorphism is the identity.
Jordan Hall classes are Hall–Littlewood functions with the transported Green pairing
Statement
Extend the generic Jordan Hall algebra of The generic Jordan-quiver Hall algebra is the symmetric-function ring to , and use that theorem's exact map . Let and have the conventions of Hall–Littlewood scalar product and monic functions, and put Define the Jordan Green pairing to be the bilinear form It is nondegenerate and equals inverse automorphism counting at every finite-field specialization . Then the Hall–Littlewood functions exist uniquely in the monic orthogonal convention specified there, and More precisely, if , then Different degrees are orthogonal. In particular the transported pairing on power sums is The empty partition gives , with norm . All the displayed basis and pairing identities specialize at and at . The pairing normalization is a degree scaling of the standard Hall–Littlewood form; it is not the ordinary symmetric-function Hall inner product.
Facts & Assumptions
Given: The generic Jordan Hall algebra, its exact generator-normalized map , a finite field of size for counting steps, and partitions. All generating series below are formal: every coefficient used involves only finite-dimensional homogeneous spaces.
The generic map is an algebra isomorphism with ; its proof establishes the Hall flag formula and the unitriangular expansion of the monomials in Jordan classes, ordered by kernel dimensions (The generic Jordan-quiver Hall algebra is the symmetric-function ring).
The automorphism count is as displayed above (Automorphism counts for nilpotent Jordan representations).
Power sums are a basis over and monomial symmetric functions are an integral stable basis (Power sums form a rational but not integral stable basis, The monomial symmetric functions form the integral stable basis).
Dominance compares row prefix sums, and conjugation reverses dominance (Dominance order on partitions, Conjugation reverses dominance).
The Hall–Littlewood form has power-sum diagonal , and its desired monic basis is specified by orthogonality and dominance triangularity (Hall–Littlewood scalar product and monic functions).
Infinitely many prime cardinalities give finite fields, and a nonzero polynomial has only finitely many real roots (Euclid's theorem: for every and every list of primes there is a prime not among ; consequently the set of primes is not finite, For every prime , the two operations on make it a field, For , every class in has one representative with , so ; while is in bijection with , A nonzero real polynomial of degree has no more than distinct real roots).
In any commutative -algebra , the series and for are defined by their coefficientwise finite power expansions and are inverse group homomorphisms; in particular for units with constant term (Formal exponential, logarithm, and binomial powers over a commutative -algebra, Formal and are inverse homomorphisms and formal binomial powers obey the expected addition laws).
Proof
For a composition of , allowing zero parts, let and . By the Hall flag formula [F1], the coefficient of in at counts flags with and , when has type . A repeated subspace is permitted exactly when the corresponding part is zero. Product order reverses the quotient order, but the Jordan Hall algebra is commutative by [F1], so these flags give the stated coefficient.
Put . The identity follows by counting pairs of boxes in each column. The unitriangular Hall relation in [F1], using , and dominance reversal [F4], gives Here , and strict kernel inequalities are exactly strict dominance in the opposite row direction.
Consequently at equals , where counts all actual flags of type lowered by a fixed operator , and is one operator of each Jordan type. To rewrite this as a count of all such triples on , fix and let act on its conjugates. The stabilizer of is , of order by [F2]. The map , , is surjective, and two elements have the same image exactly when . Thus each fiber is a coset of , so this conjugacy class has elements. Conjugation transports the lowered flags bijectively, so is constant on the class. Therefore the weighted sum over Jordan types is exactly times the number of all such triples. Lowering either finite flag makes nilpotent.
Two flags have a common splitting with . Construct this by choosing a complement of inside successively in increasing ; the intersection of those two summands is , so induction verifies the direct-sum description. Put . These nonnegative integers have row sums and column sums . Conversely every such matrix is realized by standard coordinate blocks. Sending adapted bases to one another shows that is transitive on pairs of flags with the same matrix. This is finite-dimensional basis selection only.
Expanding in monomials gives with coefficient and only terms for besides it. Indeed each factor selects distinct variables. For a resulting exponent vector arranged decreasingly, the sum of its first exponents is at most , giving the dominance bound. For the specific monomial , equality holds in this bound for every , so the variables selected in column must be exactly ; this is the unique selection. Inverting the finite unitriangular system in step 1.2 now proves .
Fix that splitting. The algebra of endomorphisms preserving both flags consists of blocks from to with and . Its off-diagonal blocks form a nilpotent ideal: each nonzero off-diagonal multiplication strictly decreases . Thus an element is invertible exactly when every diagonal block is invertible, either by a finite geometric-series inverse after removing its invertible diagonal or by triangularity. If , the stabilizer of the flags has order . A map lowering both flags has blocks with , so the space of such maps has dimension .
The contribution of this matrix to the mass in step 2.1 is therefore . Subtracting the block sums gives . Since , multiplication by turns that contribution into . Using , already proved in [F2], it follows that the transported form satisfies This includes , whose only matrix has zero entries and mass .
Let , where . The recurrence is equivalent to . For in , [F7] and substitution give . Substitution commutes with these power-series definitions because every coefficient is a finite sum. Comparing coefficients, using , gives For , apply [F7] in the commutative -algebra : the logarithm of the finite product is . Applying the inverse exponential and passing coefficientwise through the stable rank projections yields in . Step 4.1 therefore says Only finitely many are used. To apply the univariate identities [F7] to this last multivariable expression, replace each by for an auxiliary variable and work in , with equal to or as appropriate. These are commutative -algebras; all exponential arguments have positive -order and all logarithm arguments have constant term . Each coefficient of is a finite homogeneous polynomial, so comparison recovers precisely the total-degree formal identities. The same observation applies to the following exponential comparison. All these coefficient-ring hypotheses also hold over .
Define a form on the power-sum basis by . Expanding the two exponentials for in step 5.1 and using this diagonal rule yields the same final exponential: for each , the equal multiplicities contribute , since the two signs cancel. Thus and agree on every product of elementary functions in both arguments, which spans by [F1]. They are equal. On degree , the displayed power-sum diagonal of is times that of .
For each fixed degree the entries of the generic transported form are rational functions of : [F1] gives Laurent-polynomial images and inverse generator formulas, and [F2] gives the rational diagonal denominators , none vanishing at . Step 6.1 proves the desired pairing identity at every finite-field cardinality. Clearing denominators, its difference is a polynomial vanishing at infinitely many prime cardinalities, hence zero by [F6]. It follows that on degree , and the asserted generic power-sum formula holds.
The are pairwise orthogonal for , since the are so by its definition; step 7.1 makes them orthogonal for the Hall–Littlewood form as well. Their norms are which are nonzero. Replace the indeterminate by to obtain existence of the basis required in [F5]. For uniqueness, choose a linear extension of dominance in each finite degree, placing dominated partitions first. Inductively two monic triangular orthogonal bases agree on earlier indices; their difference at the next index lies in the span of these earlier basis vectors and is orthogonal to each. Each earlier norm is nonzero, so every coefficient of the difference is zero. This proves uniqueness and identifies .
The triangular system in step 1.2 has Laurent-polynomial entries and diagonal , so its finite-degree inverse has Laurent-polynomial entries. Hence the constructed and thus have no poles for , in particular at . The pairing denominators also remain nonzero there. All identities therefore specialize as stated. The zero partition is the empty flag, , , and , so its image and norm are . This proves every asserted normalization and boundary case without assuming a Green coproduct theorem or a physical interpretation.
5 · Examples, counterexamples and false statements
None yet.
Sources
- Olivier Schiffmann, Lectures on Hall Algebras, arXiv:math/0611617v2, §§1.1 and 1.3
- Matthew B. Young, Degenerate versions of Green’s theorem for Hall modules, arXiv:1810.08238v2, §2.1
- Saunders Mac Lane, Categories for the Working Mathematician, VIII.3
- Olivier Schiffmann, Lectures on Hall Algebras, arXiv:math/0611617v2, §1.3
- Olivier Schiffmann, Lectures on Hall Algebras, arXiv:math/0611617v2, §2.1
- S. Treil, Linear Algebra Done Wrong, Chapter 9, Theorems 4.2–4.3
- Olivier Schiffmann, Lectures on Hall Algebras, arXiv:math/0611617v2, §§2.1–2.4
- I. G. Macdonald, Symmetric Functions and Hall Polynomials, second edition, III §4 (4.11), VI §1 introductory characterization
- Olivier Schiffmann, Lectures on Hall Algebras, §2.3, Lemma 2.8
- Olivier Schiffmann, Lectures on Hall Algebras, §§2.3–2.4, Lemma 2.8 and (2.9)
- I. G. Macdonald, Symmetric Functions and Hall Polynomials, III §§2–4 and VI §1