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Hall Integration, Stability, DT/BPS Invariants, and Wall Crossing
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 Spaces, Stacks, and Derived Algebraic Geometry Foundations
- Analytic Constructible Sheaf Foundations
- Analytic Derived Six Operations And Duality
- Analyticity of Holomorphic Functions; Liouville and Morera
- Arc Length and Rectifiable Curves
- Artinian Rings and Length
- Associated Primes and Primary Decomposition
- Binary Operations, Monoids, Groups and Subgroups
- Blowups, Exceptional Divisors, and Strict Transforms
- Bounded Variation and the Riemann–Stieltjes Integral
- Cardinal Arithmetic, Cofinality and the Alephs
- Categories, Functors and Natural Transformations
- Chain Complexes and Homology
- Chain Conditions, Semisimple Modules and the Wedderburn–Artin Theorem
- Chain Homotopy and the Homotopy Category
- Classical Affine Varieties: Coordinate Rings, Morphisms, and Rational Maps
- Cohomological Hall Algebras and Quiver Correspondences
- Cohomology of Quasi Coherent Sheaves on Affine and Projective Schemes
- Compact Support Sheaf Calculus
- Compactness
- Compactness in Metric Spaces
- Completeness, Completion, and Uniform Continuity
- Complex Algebraic Stratified Topology
- Complex Coordinate and Path Transport
- 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
- Connectedness
- Constant Rank, Submersions, Immersions and Regular Level Sets
- Constructible Incidence And Cochain Models
- 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
- Cup Cap Cross Products and Cohomology Rings
- Cw Complexes and Cellular Homology
- Cyclic Groups and Direct Products
- Dedekind Domains and Ideal Classes
- Delta Functors and Universality
- Depth and Cohen Macaulay Modules
- Derived Categories
- Derived Functors
- Derived Hall Algebras from dg-Enhanced Categories
- Determinants of Matrices over a Commutative Ring
- Diagonalisation and the Minimal Polynomial
- Diagonals Separated Morphisms and Valuative Uniqueness
- Differential Graded Algebras and Homological Foundations
- Dimension Constructible Images and Dimensions of Fibres
- Divisibility, Euclidean Domains, Principal Ideal Domains and Unique Factorisation
- Divisibility, Greatest Common Divisors and Bézout's Identity
- Double Complexes Exact Couples and Convergence
- Dual Spaces, Bilinear and Quadratic Forms, and Sylvester's Law of Inertia
- Eigenvalues, Eigenvectors and the Characteristic Polynomial
- Equivariant Borel–Moore Correspondence Convolution and Constructible Ext
- Equivariant Constructible Perverse Foundations
- Euclidean Ordinary Differential Equations with Smooth Dependence
- Exactness and the Member Calculus
- Ext and Balanced Resolutions
- Exterior Powers, Orientation and Hodge Duality
- Fibrations Fiber Bundles and Homotopy Exact Sequences
- Fibre Products Base Change and Scheme Theoretic Fibres
- Filters and Ultrafilters
- Finitary Ringel–Hall Algebras
- Finite Counting, Factorials and Binomial Coefficients
- Finite Fields and Cyclotomic Extensions
- Finite Proper and Projective Morphisms
- Flat Smooth and Etale Morphisms
- Flatness and Faithful Flatness
- Foundations of the Real Numbers for Analysis
- Free Modules, Exact Sequences, Projective and Injective Modules
- Fubini and Change of Variables
- Function Space Topologies and the Exponential Law
- Fundamental Trigonometric Identities
- Gaussian Elimination, Elementary Matrices and Reduced Row Echelon Form
- Goursat's Theorem and Cauchy's Theorem in a Convex Domain
- Graded Quiver Algebras and Derived Tensor Functors
- Group Actions, Orbits, Stabilisers and Cayley's Theorem
- Group Homomorphisms and the Isomorphism Theorems
- Group Schemes of Finite Type over a Field
- Hall Algebra Modules, Fock Spaces, and Geometric Actions
- Hausdorff via the Diagonal
- Hereditary and Productive Behaviour of the Separation Axioms
- Higher Homotopy Groups and Cofiber Sequences
- Holomorphic Functions of Several Complex Variables
- Homogeneous Resultants and Projective Intersection Length
- Homology Axioms Degree and Classical Applications
- Homotopy and Homotopy Equivalence
- Hurewicz Whitehead Freudenthal and Cw Approximation
- Ideals, Quotient Rings and the Isomorphism Theorems for Rings
- Inner Product Spaces, Gram-Schmidt, Projections and Adjoints
- Integral Extensions and Going Up
- Isolated Singularities and Laurent Series
- Kahler Differentials Conormal Sequences and Infinitesimal Lifting
- Koszul Complexes and Regular Sequences
- Krull Dimension and Height Theorems
- Leray–Hirsch, the Thom Isomorphism, and Gysin Sequences
- 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
- Local Coefficients, Twisted Homology, and Duality
- Localisation of Modules and Support
- Long Exact Sequences in Homology
- Mapping Cones Cylinders and Chain Triangles
- Matrices, the Matrix of a Linear Map, and Change of Basis
- Metric Spaces
- Mixed Partials, Taylor Formulae, and Extrema
- 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
- Motivic Hall Algebras and Integration Maps
- Noether Normalisation and Nullstellensatz
- Noetherian Rings and Hilbert Basis
- Nonaffine Algebraic Groups, Barsotti-Chevalley, and Abelian Varieties
- Normal Subgroups and Quotient Groups
- Normalization Finiteness for Affine Domains
- Obstruction Theory, Postnikov Towers, and Classifying Spaces
- Order, Zorn's Lemma, and the Axiom of Choice
- Ordinal Arithmetic and the First Uncountable Ordinal
- Ordinals, Cardinals, and Transfinite Recursion
- Partitions of Unity and Paracompactness
- 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
- 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
- Properties of the Integral and the Working FTC
- Quasi Coherent and Coherent Sheaves and Vector Bundles
- Rank Theorems and Embedded Submanifolds
- 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
- Relative Homology Excision and Mayer Vietoris
- Relative smooth triangulation and bundle fitting
- Riemann Surfaces, Branched Maps, and Differentials
- Rings, Subrings, Integral Domains and Fields
- Rⁿ as a Normed Space; Vector-Valued Functions
- Roots, Rational Powers, and Classical Inequalities
- Schemes Subschemes and Morphisms Locally of Finite Type
- Separation Axioms: the Hierarchy
- Sequences and Limits
- Sequences and Series of Functions; Uniform Convergence
- Series: Convergence and the Nonnegative Tests
- Sheaf Cohomology Cech Cohomology and Comparison
- Sheaf Operations Exactness Ringed Spaces and Module Pullback
- Simple Field Extensions and the Construction of the Complex Numbers
- Simple Homotopy, Whitehead Groups, and Torsion
- Simplicial Complexes and Simplicial Homology
- Simplicial Subdivision and Simplicial Approximation
- Sine, Cosine, and the Definition of Pi
- Singular Chains and Singular Homology
- Singular Cohomology and Coefficient Theorems
- Smooth Manifolds and Smooth Maps
- Smooth Partitions of Unity and Exhaustions
- Smooth Vector Bundles and Sections
- Spectral Sequences
- Splitting Fields
- Stiefel Whitney and Euler Classes by Universal Constructions
- Subobject Lattices Generators and the Grothendieck Axioms
- Subspaces, Products, and Quotients
- Suprema and Infima
- Symmetric Groups, Cycle Decomposition and the Sign Homomorphism
- Tangent Cotangent and the Differential
- Tensor Products of Modules
- The Argument Principle and Rouché's Theorem
- 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 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 Logarithm and General Powers
- The Residue Theorem and the Evaluation of Real Integrals
- The Riemann Integral in Rᵐ and Jordan Content
- The Riemann Integral: Definition and Integrability
- The Serre Spectral Sequence and Applications
- The Topology of Euclidean Space
- The Total Derivative in ℝᵐ → ℝⁿ
- The Winding Number and the Global Cauchy Theorem
- The ZFC Axioms and the Basic Set Constructions
- Topological Spaces and Continuity
- Topological Vector Bundles and Grassmannian Classification
- Topology of ℝ
- Tor Flatness and Global Dimension
- Triangularisation, Generalised Eigenspaces and Jordan Canonical Form
- Triangulated Categories
- 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
- Urysohn's Lemma and the Tietze Extension Theorem
- Valuation Rings and Discrete Valuation Rings
- Vector Spaces, Linear Subspaces, Span and Direct Sums
- Whitney Embedding Tubular Neighbourhoods and Approximation
- Yoneda Extensions and Homological Dimension
- Zariski Tangent Spaces, Regular Points, Smoothness, and Bertini
- Zariski Topology on Prime Spectra
2 · Summary
This page proves the finite-field counting branch of Hall wall crossing for every finite acyclic quiver, including wild quivers. Fix , finite-dimensional representations, and arbitrary vertex charges in the open upper half-plane. The local HN proof gives existence, uniqueness, and descent from the algebraic closure. The Hall convention is subobject first; its Euler and skew integrations are both proved with their exact twists.
Construction order
- Finite-field stability data for an acyclic quiver fixes the representation, Euler, phase, semistability, and quotient-stack conventions.
- Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity supplies the small finitary abelian category, a length-one projective resolution, and the Hom-minus-Yoneda-Ext Euler formula without identifying Yoneda and derived Ext.
- The phase of a sum lies between upper-half-plane phases proves the phase comparison for sums of central charges used in the HN argument.
- Semistable loci of finite-quiver representations are open proves openness by an explicit subrepresentation incidence construction. Its projective-closedness argument records the closed-embedding and projective-properness AC branches separately.
- Quiver Harder–Narasimhan filtrations exist, are unique, and descend proves the choice-free HN result and finite-field descent.
- Finite-field points of the semistable quiver stack give the Hall groupoid trivializes the finite-field general-linear torsors and identifies the semistable stack mass with the finite Hall groupoid.
- Subobject-first Hall completion and quantum tori for finite quivers, Finite-quiver Hall multiplication counts extensions by automorphism orbits, and Euler and skew integration are multiplicative for finite acyclic quivers fix the product order, prove the extension orbit formula, and establish both continuous integration maps.
- Completed Hall wall crossing for finite acyclic quivers proves the completed HN product and its Euler and skew integrated wall identities, including strict semistables.
The finite-field series are Euler-normalized groupoid masses. This proof does not establish Behrend-weighted CY DT invariants, motivic vanishing-cycle integration, cohomological BPS spaces, or physical state-counting identifications. Their hypotheses and the current CoHA interface status are recorded in Finite-quiver Hall counts and the limits of DT/BPS interpretation. The four required preceding pages remain separate constructions and are reading context; no integration theorem from them supplies this proof.
Companion calculations: hall-stability-dt-bps-and-wall-crossing-examples.
3 · Logical flowchart
4 · Definitions, theorems and proofs
Finite-field stability data for an acyclic quiver
Definition
Let be a finite quiver: and are finite sets, and give the source and target of each arrow. Assume has no directed cycles. For a field , a finite-dimensional representation assigns a finite-dimensional -vector space to each and a linear map to each . A morphism is a family of linear maps at the vertices commuting with all arrow maps. Write for this category and for its dimension vector. For the finite-field Hall branch, fix and write . The next lemma proves the abelian and Euler properties over any field; over it constructs a small finitary abelian skeleton of , so is essentially small.
For define the bilinear form and its skew-symmetrization . The next lemma proves that is the Hom-minus-Yoneda-Ext dimension for this arrow convention.
Fix for each vertex and extend additively. If is nonzero, then ; thus its principal argument lies in . For a nonzero representation , put . Call -semistable if every nonzero subrepresentation satisfies , and -stable if the inequality is strict for every proper nonzero subrepresentation.
For the semistable groupoids and stacks below, include the zero representation as semistable without assigning it a phase. Stable objects and HN factors remain nonzero.
For a dimension vector , let The group acts by change of bases. Define geometrically: its points over an algebraic closure are representations for which every nonzero -subrepresentation satisfies the semistability inequality. The associated quotient stack is . For , set . The group is trivial, so its rational-point groupoid has one zero object, trivial automorphism group, and cardinality . Here denotes the groupoid-valued quotient: over a scheme its objects are -torsors on with equivariant maps to , and its arrows are equivariant isomorphisms over . The openness lemma below proves that is open.
For a finite groupoid , define its groupoid cardinality by The rational-point groupoid of is finite, and the finite-field descent lemma identifies it with the groupoid of finite-field semistable representations and their isomorphisms. No Calabi–Yau structure, potential, orientation data, vanishing cycles, or physical state-counting identification is part of this definition.
Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity
Statement
Let be a finite acyclic quiver and any field. The category of finite-dimensional representations is abelian. For all , the spaces and Yoneda are finite-dimensional -vector spaces, and The explicit projective resolution below shows that the projective-resolution groups vanish for ; these groups are the cohomology of applying to a projective resolution. If , the displayed vector spaces have finite underlying sets and has a small skeleton (a small full subcategory with one representative of each isomorphism class). Thus is essentially small, and this skeleton is a small finitary abelian category. Yoneda is classified directly below; it is not identified with derived by an unstated theorem.
Facts & Assumptions
Given: A finite acyclic quiver , a field , and .
For every field , is the category of vertexwise vector spaces and arrow maps, and is the displayed Euler form (Finite-field stability data for an acyclic quiver).
A small finitary abelian category has finite Hom sets and finite Yoneda extension-class sets, with endpoint-fixed short-exact-sequence equivalence (Small finitary abelian categories for Hall multiplication).
A morphism between short exact sequences that is the identity on both endpoints is an isomorphism on the middle object (Short five lemma in an abelian category).
Proof
Given: The objects and hypotheses in the statement.
For a morphism , its vertexwise kernels form a subrepresentation: if , then for every arrow . The vertexwise cokernels form a quotient representation because . The kernel and cokernel universal properties hold vertex by vertex. The canonical coimage-to-image map is an isomorphism at every vertex, hence an isomorphism of representations. With vertexwise finite direct sums and a zero object, these facts make abelian.
For , let have basis the directed paths from to , with arrow maps given by path concatenation. Acyclicity and finiteness of make each path set finite. A morphism is uniquely determined by the image of the length-zero path at , so ; evaluation at preserves epimorphisms, and therefore is projective.
Put and define by . Its kernel is exactly by the commuting-square definition of a representation morphism.
For a representation , define by , where is the composite arrow map along the path . Define at a path by Both terms are finite direct sums of the projectives from step 1.2. Then because .
Now assume . For each dimension vector , there are finitely many arrow matrix tuples on the fixed spaces , and the finite group has finitely many orbits on this set. Fix an enumeration of the finite set ; the lexicographically least tuple in each orbit gives a representative without making a choice from an arbitrary family. The union over the set is a set, so the full subcategory on these representatives is small. It is a skeleton: every finite-dimensional representation becomes one of the matrix tuples after choosing bases at its finitely many vertices. The full skeleton is abelian because each vertexwise kernel and cokernel from step 1.1 is isomorphic to its selected representative, and transporting its kernel or cokernel map across that isomorphism preserves the universal property.
At vertex , is onto because is the image of . Modulo , the relation in step 2.1 replaces by . Every positive-length path has a unique first arrow, so repeated replacement sends each path tensor to . Consequently the quotient of the middle term by is isomorphic to through , and .
The map is injective. In a nonzero element of its domain, choose the largest length of a suffix path with nonzero coefficient. The second term of has length . Each such path has a unique first arrow and suffix, so its coefficient cannot cancel with the second term of a different source basis summand. A first term of has length at most , since no source suffix has length . Thus the length- part of is nonzero, proving injectivity. The displayed sequence is a projective resolution of length one; applying therefore gives for .
A short exact sequence splits as a sequence of vector spaces at each of the finitely many vertices. In the resulting coordinates every arrow of has block matrix Every tuple defines such an extension. Changing the vertexwise splittings by changes by . Conversely, an isomorphism of extensions that is the identity on endpoints has block matrix at each vertex and hence changes by exactly . By [F3], the generated endpoint-fixed Yoneda relation consists of these isomorphisms. The Baer sum of the extensions represented by and is represented by : the pullback of their direct sum along followed by pushout along adds the off-diagonal arrow blocks. Pushout along sends to . Therefore the Yoneda vector-space structure is the quotient structure a finite-dimensional -vector space; it is not being identified here with the projective-resolution group of step 4.1.
Both cochain spaces in step 1.3 are finite-dimensional. Rank-nullity for gives The kernel and cokernel identifications already proved give the Hom–Yoneda-Ext formula and finite-dimensionality over any . When , the underlying sets are finite. The full skeleton constructed in step 2.2 has the same Hom sets on its objects; transporting extension middle terms to their representatives identifies its Yoneda classes with those in . Thus this small abelian skeleton satisfies the finitary hypotheses of [F2], while is essentially small.
The phase of a sum lies between upper-half-plane phases
Statement
Let and define . For , the phase of lies between and , strictly between them when they are unequal and equal to their common value when they coincide.
Facts & Assumptions
Given: .
The stability convention is and (Finite-field stability data for an acyclic quiver).
Proof
Given: The objects and hypotheses in the statement.
Suppose . Then . Consequently , which, by [F1], gives . Also , so [F1] gives .
If , interchange in step 1.1. If the arguments are equal, are positive real multiples of the same ray, so their sum has that same argument. These cases prove the stated between-phase rule.
Semistable loci of finite-quiver representations are open
Statement
Assume the Axiom of Choice. Let , , , and be as in Finite-field stability data for an acyclic quiver. The subset of representations over that are semistable for every nonzero geometric subrepresentation is Zariski open in .
Facts & Assumptions
Given: A finite acyclic quiver , a finite field , a dimension vector , and central charges .
is the affine parameter scheme of arrow matrices, and geometric semistability tests all nonzero subspaces preserved by those matrices (Finite-field stability data for an acyclic quiver).
Each Grassmannian has a closed Plücker embedding into a projective space (The Plucker image is a closed projective algebraic set).
The Segre image of a product of two projective spaces is a closed projective algebraic set (The Segre image is the projective rank-one locus cut out by 2 by 2 minors).
A morphism is projective on the repository's stated convention if it factors as a closed immersion into relative projective space followed by projection (Projective morphisms before Proj).
A projective morphism is proper; this supplier explicitly assumes AC (Projective morphisms are proper).
Proper morphisms of schemes are closed, including after base change (Proper morphisms are closed).
Under AC, a homogeneous ideal in defines a closed subscheme of ; on its ring is the degree-zero localized polynomial ring modulo the localized ideal (Closed subschemes of projective space and saturated ideals).
The Axiom of Choice is assumed only for the projective-morphism properness result [F5] (The Axiom of Choice).
The Axiom of Choice is also inherited through [F7] for the scheme-theoretic realizations of the Plucker and Segre equations in [F2] and [F3]. Their classical projective coordinate interpretation uses the algebraically closed field , as fixed by Closed projective embedding from a radical homogeneous ideal and its projective-space prerequisite. Thus the finite field is not substituted for the classical base field (The Axiom of Choice).
Proof
Given: The objects and hypotheses in the statement.
Work over . By [F2] and [F7], the Plucker equations define a closed projective subscheme whose -points are the -planes. On a chart , normalize and use the signed one-outside coordinates as the entries of a matrix . The Plucker relation with tuples and expresses each , for , using coordinates with fewer indices outside and one-outside coordinates. Induction identifies every in the quotient chart ring with the corresponding maximal minor of ; conversely those minors satisfy every Plucker relation. Hence the chart ring is . The row spans of give a rank- subbundle of the trivial bundle, and its quotient is locally free; the pivot changes on overlaps are invertible and glue these bundles and charts. Thus the equations construct the Grassmannian scheme with its closed Plucker embedding. The endpoint cases are points. For the Segre equations in [F3], on normalize and put and , with . The minor relations give in the quotient ring, and substitution and coordinate extraction are inverse maps with . These charts construct the closed Segre embedding. Iterating it embeds the finite product as a closed subscheme of one projective space; if is empty, is a point. The chart ring surjections remain surjective after adjoining the arrow-matrix coordinates, so is closed in a relative projective space over . The chart calculations show these projective subschemes are reduced with the point loci in [F2] and [F3]; [A2] records their classical projective coordinate interpretation over .
For each subvector with and , impose in , for each arrow , that the composition vanish. Here and are the tautological subbundle and quotient bundle constructed in step 1.1; their fibers at are and . On the charts from step 1.1 these are polynomial equations, so their common zero locus is closed. Its geometric points are exactly pairs consisting of an arrow-matrix tuple and a subrepresentation of dimension . The closed inclusion composes with the relative Plucker–Segre closed immersion of step 1.1, so the projection to is projective by [F4].
By [A1] and [F5], the projection in step 2.1 is proper; [F6] then makes its image closed in . Its -points are exactly the representations with a destabilizing subrepresentation of dimension .
There are finitely many subvectors with . The unstable locus is the finite union of the closed images from step 3.1 over the subvectors satisfying the strict phase inequality. Its complement is therefore open and, by [F1], is precisely . If the union is empty and the whole one-point representation space is open.
The two declared axiom branches are [A2], used in step 1.1 through [F7] for the scheme-theoretic projective constructions, and [A1], used in step 3.1 through [F5] for properness. The semistability and HN counting arguments do not otherwise use AC.
Quiver Harder–Narasimhan filtrations exist, are unique, and descend
Statement
Let be finite and acyclic, let , and give every vertex an arbitrary charge . Over any field extension , every finite-dimensional representation has a unique filtration whose nonzero factors are -semistable and have strictly decreasing phases. If is defined over , the unique filtration of its scalar extension is Frobenius invariant and descends to . Consequently geometric semistability of an -representation is equivalent to semistability tested only on its -subrepresentations. Write for total dimension.
Facts & Assumptions
Given: A finite acyclic quiver, , charges , and a finite-dimensional representation over an extension field ; for the descent claims, the representation is the scalar extension of an object defined over .
The central charge is additive on short exact sequences, phases lie in , and semistability is tested on nonzero subrepresentations (Finite-field stability data for an acyclic quiver).
Kernels, images, quotients and inverse images of subrepresentations are computed vertexwise in the abelian category of quiver representations (Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity).
The phase of a sum of two nonzero upper-half-plane central charges lies between their phases (The phase of a sum lies between upper-half-plane phases).
Proof
Given: The objects and hypotheses in the statement.
Let have dimension vector . The nonzero dimension vectors of its subrepresentations form a nonempty subset of the finite set . Choose the largest attained phase and, among subobjects attaining it, the largest attained total dimension. Such a phase and dimension are maxima of finite sets of attained values, so they are attained without an infinite choice. Let attain both maxima. Every nonzero subobject of is a subobject of , so its phase is at most ; hence is semistable.
If are semistable and , then . Indeed, a nonzero map has a nonzero image . From , semistability of and [F3] force : if the kernel is zero the phases are equal; if the kernel is nonzero and , the phase of the sum lies strictly below , contradicting . But and semistability of give , a contradiction.
If is nonzero, let be its inverse image. Then is exact. If , [F3] gives , contrary to maximality of the phase of . If , additivity and [F3] give , while , contrary to the second maximum. Thus every nonzero subobject of has phase strictly less than .
Consider two filtrations with first subobjects of phases . If , every factor in the quotient filtration of has phase below . Step 1.2 therefore makes every map from to each such factor zero. Induction along the finite quotient filtration shows : a map whose projection to the last factor is zero factors through the preceding subobject. Thus the inclusion of in factors through , giving a nonzero map , contrary to from step 1.2. Interchanging similarly rules out ; hence . Applying step 1.2 to all factors of both quotients now gives and , hence . Induction on the quotient proves equality of the full filtrations.
Induct on . The zero representation has the empty filtration. For , the quotient has smaller total dimension, so by induction it has a filtration with semistable factors in strictly decreasing phase order. Step 2.1 places every one of those phases below . Pulling that filtration back along and placing first gives the required filtration of .
Let be defined over , set , and let be Frobenius. Applying to a filtration preserves the arrow maps of , every dimension vector, and every phase. It therefore gives another HN filtration; uniqueness proved above fixes each term. At each vertex, a Frobenius-invariant subspace has a unique reduced row-echelon basis matrix. Applying gives another such matrix for the same subspace, so uniqueness makes the matrix fixed entrywise. Its entries lie in , and the arrow maps of preserve these descended subspaces. Thus the filtration descends to .
If an -object is geometrically unstable, it has a geometric subrepresentation of phase greater than its total phase. Step 1.1 chooses a subobject of maximal phase, so the first HN term has phase greater than the total phase. Step 4.1 descends that term and its phase inequality to , contradicting -semistability. Conversely, an -subrepresentation extends to with the same dimension vector and phase. This proves the stated equivalence and the result.
Finite-field points of the semistable quiver stack give the Hall groupoid
Statement
Assume the Axiom of Choice inherited from the semistable-openness prerequisite. Let be finite and acyclic over , and let . In this statement, include the zero representation as -semistable, without assigning it a phase. The rational-point groupoid of is finite and is equivalent to the groupoid whose objects are -semistable -representations of dimension and whose arrows are their representation isomorphisms. Its groupoid cardinality is therefore
Facts & Assumptions
Given: A finite acyclic quiver, a finite field , a dimension vector , and vertex charges in .
The quotient stack has objects given by -torsors with equivariant maps to ; its semistable representation locus is open (Finite-field stability data for an acyclic quiver, Semistable loci of finite-quiver representations are open).
Geometric HN filtrations of representations over are Frobenius invariant and descend to ; hence geometric and finite-field semistability agree (Quiver Harder–Narasimhan filtrations exist, are unique, and descend).
AC is inherited only for the algebraic-open-substack premise from Semistable loci of finite-quiver representations are open (The Axiom of Choice).
Proof
Given: The objects and hypotheses in the statement.
Under the inherited assumption [A1], the semistable locus is the open subscheme from [F1]. An object of its quotient groupoid over is a tuple of -torsors together with an equivariant semistable representation. A -torsor is the frame torsor of its associated -dimensional vector space. Every finite-dimensional vector space over has a basis, so that associated space is isomorphic to and its frame torsor is trivial. Applying this at the finitely many vertices trivializes the product -torsor. Thus every quotient-stack object is isomorphic to a representation on the standard spaces .
Under a chosen trivialization, an equivariant map to is an arrow-matrix tuple. Two trivialized objects are isomorphic exactly when their tuples differ by change of bases in . If , [F2] identifies the rational tuples in the geometric semistable locus with the finite-field semistable representations. If , the geometric condition is vacuous, the representation space is a point, and is trivial. Its quotient groupoid therefore has one object with trivial automorphism group, matching the zero representation included by the statement's convention. This proves the claimed equivalence in every dimension.
There are finitely many arrow-matrix tuples on the fixed finite vector spaces, and each automorphism group is a subgroup of the finite group . Hence the groupoid is finite. Under the equivalence of step 2.1, the stabilizer of a tuple is exactly . Substituting these stabilizers into the groupoid-cardinality definition in Finite-field stability data for an acyclic quiver gives the displayed sum.
Subobject-first Hall completion and quantum tori for finite quivers
Definition
Fix , , and as in Finite-field stability data for an acyclic quiver. For a representation , write and let be the basis function of its isomorphism class. Let be the small finitary abelian skeleton constructed in Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity. Define , identifying its basis with the isomorphism classes of . Fullness and transport of subobjects and cokernels along isomorphisms preserve the Hall coefficients. Thus is the direct sum over those classes, with rational coefficients and the quotient-first untwisted Hall product of The untwisted Hall algebra of a finitary abelian category. In that convention counts sequences , and identify the basis symbol with the characteristic function . Define the subobject-first product by . Then where the sum is over subobject classes of : monomorphisms into modulo isomorphisms of their domains commuting with the monomorphism. Distinct embedded subobjects are counted separately even when their domains are isomorphic. Put .
For , let be the span of classes of dimension vector . It is finite-dimensional: the representation set on the standard spaces is finite. Define the dimension completion The product is extended degreewise; each coefficient uses finitely many decompositions . There is no analytic convergence assertion. The all-object and phase factors are Each is an element of because each homogeneous component has finite support.
Let and . Take the completed Euler torus and skew torus over , with bases and , respectively, and products Their completions use the same dimension product. The next theorem proves associativity and gives the continuous Euler and skew integration maps.
Finite-quiver Hall multiplication counts extensions by automorphism orbits
Statement
Let be finite-dimensional representations over . For and the subobject-first product from Subobject-first Hall completion and quantum tori for finite quivers, where is the set of endpoint-fixed Yoneda classes of whose middle term is isomorphic to .
Facts & Assumptions
Given: Finite-dimensional , an isomorphism class , and the subobject-first Hall product.
In the generic untwisted Hall convention, counts short exact sequences (The untwisted Hall algebra of a finitary abelian category).
The local convention is , and (Subobject-first Hall completion and quantum tori for finite quivers).
The sets and are finite; the latter is the endpoint-fixed Yoneda class set (Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity).
For fixed endpoints, the untwisted Hall product has finite support (Untwisted Hall structure constants and products are finite).
Proof
Given: The objects and hypotheses in the statement.
Fix the middle object to be . The coefficient of in counts subobjects with and , by [F1] and [F2]. For each such , the monomorphisms with image form a set of size ; the epimorphisms with kernel form a set of size . These choices are independent. Hence the number of endpoint-fixed short exact sequences with middle object literally is where is the Hall coefficient of [F1].
The finite group acts on those sequences by . Its orbits are exactly the endpoint-fixed Yoneda classes with middle term isomorphic to : an isomorphism from any middle object transports its sequence to one on , and changing that isomorphism changes the result by this action. The stabilizer of a sequence consists of with and . Put . Since and is an epimorphism, factors uniquely as for a unique . Conversely, is invertible because , with inverse . Thus every stabilizer has exactly elements.
For a fixed sequence, the map from to its orbit has fibers exactly the cosets of its stabilizer, so that orbit has size . Summing over the orbits gives Multiplying the coefficient of in by the definition of yields precisely the claimed coefficient. Summing over the finitely many possible middle terms is valid by [F3] and [F4].
Euler and skew integration are multiplicative for finite acyclic quivers
Statement
Let be a finite acyclic quiver over , let , and use the subobject-first completion and tori from Subobject-first Hall completion and quantum tori for finite quivers. The degree-completed Hall product is associative and unital. The continuous maps are unital algebra homomorphisms to the completed tori with products These are separate normalizations: the first is the Euler form target, while the second uses the skew-symmetrized form and the diagonal factor .
Facts & Assumptions
Given: A finite acyclic quiver over , the subobject-first Hall convention, and .
The subobject-first Hall product is the opposite of the quotient-first product, and the dimension completions and both target products are defined in Subobject-first Hall completion and quantum tori for finite quivers.
The normalized basis satisfies (Finite-quiver Hall multiplication counts extensions by automorphism orbits).
The representation category has a small finitary abelian full skeleton. The finite vector spaces of Hom and Yoneda Ext satisfy (Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity).
The generic quotient-first untwisted Hall product is associative and unital on every small finitary abelian category (The untwisted Hall product is associative and unital).
The homogeneous Hall products have finite support (Untwisted Hall structure constants and products are finite).
Proof
Given: The objects and hypotheses in the statement.
Apply [F4] to the small finitary abelian full skeleton supplied by [F3]. Its inclusion preserves isomorphism classes and subobject classes: transporting a monomorphism's domain to its skeleton representative gives a bijection on monomorphisms modulo domain isomorphism, and transports the quotient to the same quotient class. Thus its Hall coefficients are exactly those in [F1]. Write for this quotient-first product. By [F1], , so by [F4]. The zero-object class is the unit for , hence also for .
The degree of an extension is the sum of the endpoint dimension vectors. For a fixed output degree , a product coefficient uses only the finitely many pairs ; each is finite-dimensional by the representation-matrix definition. Thus [F5] extends the product degree by degree to , and truncating above total dimension changes no coefficient of dimension at most . This is continuity for the total-dimension filtration.
On a normalized basis vector, because . For and , [F2] gives By [F3], both sets are finite vector spaces and the ratio of their cardinalities is This is exactly in the Euler target.
On the same basis, . Applying [F2] and [F3] to gives its -image coefficient By bilinearity, Since and , the coefficient becomes which is exactly the coefficient of in the skew target.
Bilinearity of makes the Euler twist associative: both parenthesizations of have exponent . Bilinearity of gives the same cocycle identity for the skew product. Both products have the degree-zero basis vector as unit. Step 1.2 gives finite-dimensional homogeneous components, so the formulas for and define degree-preserving linear maps and are continuous on the completion. Step 1.1 establishes the source unit and associativity, and steps 1.3–1.4 establish multiplicativity on normalized basis vectors. The cocycle calculation above establishes the target unit and associativity, so linearity and continuity extend and to unital algebra homomorphisms on the completions.
Completed Hall wall crossing for finite acyclic quivers
Statement
Let be any finite acyclic quiver over , including wild quivers, and let and be any two assignments of upper-half-plane charges . In the dimension completion of the subobject-first Hall algebra, The product is degreewise finite and includes all semistable objects, whether stable or strictly semistable. Applying either Euler integration or skew integration gives equal completed ordered products for and . Each integrated ordered product has constant term and is a unit in its completed quantum torus; conjugation by the two equal products therefore gives the same continuous automorphism. No generic-stability, finite-type, 3-Calabi–Yau, orientation-data, or analytic convergence assumption is used.
Facts & Assumptions
Given: A finite acyclic quiver over and two collections of charges with each vertex charge in .
and are the degree-completed sums of all objects and of semistable objects at phase ; the product is subobject-first (Subobject-first Hall completion and quantum tori for finite quivers).
Every representation has a unique HN filtration with nonzero semistable factors of strictly decreasing phase (Quiver Harder–Narasimhan filtrations exist, are unique, and descend).
Both and are continuous unital homomorphisms on the completed Hall algebra (Euler and skew integration are multiplicative for finite acyclic quivers).
Proof
Given: The objects and hypotheses in the statement.
Fix distinct phases . Iterating the defining formula from [F1], with left-associated products, shows that the coefficient of in is the number of weak flags for which every nonzero factor is semistable of phase . The induction step chooses in the last binary product and then uses the previous flag inside ; zero quotients exactly represent skipped phases.
For a fixed dimension vector , any contributing nonzero factor has dimension vector with . There are finitely many such vectors and therefore finitely many possible phases. A contributing flag has at most nonzero factors. Thus the ordered product over all phases is a finite computation in each degree and defines an element of .
By [F2], for every exactly one flag counted by the preceding flag-count argument has strictly decreasing semistable factors: its unique HN filtration. Therefore the coefficient of each in the ordered product is , which is the coefficient of in . The zero object contributes the common degree-zero unit. This proves the Hall identity.
Apply and from [F3] to the degreewise truncations of the identity in step 2.1. Their continuity shows that the limits preserve the identity, giving both equalities of completed Euler and skew ordered products for and .
Write each integrated phase factor as , where every term of has positive total dimension. Then , since for any fixed degree only finitely many powers contribute. By step 1.2 only finitely many phases affect a fixed degree, so the ordered product and the reverse-ordered product of these inverses both converge degreewise. Their finite truncations are mutual inverses, and continuity of multiplication gives . Thus is a continuous automorphism with inverse . Step 3.1 gives the same for and , so these conjugations agree. All limits are formal in the degree completion.
Finite-quiver Hall counts and the limits of DT/BPS interpretation
Remarks
The coefficients of are finite-field, Euler-normalized semistable groupoid masses: the weight of is . The wall crossing proved on this page is an arithmetic finite-field Hall identity and its stated Euler/skew integrations. It does not identify these coefficients with Behrend-weighted numerical Donaldson–Thomas invariants of a Calabi–Yau-threefold, motivic vanishing-cycle invariants, cohomological BPS spaces, or dimensions of physical Hilbert spaces.
The four required preceding pages provide distinct reading contexts. The derived definition uses dg enhancements and higher homotopy weights; the motivic definition uses stack-function coefficients; the cohomological definition uses rational intrinsic quotient-stack Borel–Moore homology and the exact-sequence correspondence operations; a Hall-module definition is an algebra action on a separate module. These coefficient theories remain distinct from the arithmetic groupoid masses. Their operation and integration theorems are not used in this finite-field proof.
Any physical BPS identification is conditional on a specified supersymmetric quiver model, charge assignment, central charge, superpotential, relevant Calabi–Yau-threefold enhancement and orientation data, together with a proved state-counting comparison. The finite-field argument establishes none of those additional identifications.
5 · Examples, counterexamples and false statements
None yet.
Sources
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- Markus Reineke, The Harder–Narasimhan system in quantum groups and cohomology of quiver moduli, §§2–3
- Olivier Schiffmann, Lectures on Hall Algebras, §§1.1, 1.3 and 3.3
- Tom Bridgeland, Hall algebras and Donaldson–Thomas invariants, §§2.1 and 3.2–3.4
- Tom Bridgeland, Hall algebras and Donaldson–Thomas invariants, §4.4
- Markus Reineke, The Harder–Narasimhan system in quantum groups and cohomology of quiver moduli, Lemma 2.2
- Markus Reineke, The Harder–Narasimhan system in quantum groups and cohomology of quiver moduli, §3
- Markus Reineke, The Harder–Narasimhan system in quantum groups and cohomology of quiver moduli, §2
- Tom Bridgeland, Hall algebras and Donaldson–Thomas invariants, §§2.1 and 4.4
- Tom Bridgeland, An Introduction to Motivic Hall Algebras, §§3.1–3.2
- Tom Bridgeland, Hall algebras and Donaldson–Thomas invariants, §§2.1, 3.3–3.4
- Tom Bridgeland, Hall algebras and Donaldson–Thomas invariants, Lemma 2.2
- Olivier Schiffmann, Lectures on Hall Algebras, §§1.1 and 1.3
- Tom Bridgeland, Hall algebras and Donaldson–Thomas invariants, §§3.3–3.4
- Markus Reineke, The Harder–Narasimhan system in quantum groups and cohomology of quiver moduli, §6
- Markus Reineke, The Harder–Narasimhan system in quantum groups and cohomology of quiver moduli, §§2 and 4
- Tom Bridgeland, Hall algebras and Donaldson–Thomas invariants, §§4.3–4.6
- Bertrand Toën, Derived Hall algebras, §§3–4
- Tom Bridgeland, An Introduction to Motivic Hall Algebras, §§3–5
- Maxim Kontsevich and Yan Soibelman, Cohomological Hall algebra, exponential Hodge structures and motivic Donaldson-Thomas invariants, §§1–2
- Maxim Kontsevich and Yan Soibelman, Stability structures, motivic Donaldson–Thomas invariants and cluster transformations, §§1–2 and 7