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Hall Integration, Stability, DT/BPS Invariants, and Wall Crossing

1 · Prerequisites

2 · Summary

This page proves the finite-field counting branch of Hall wall crossing for every finite acyclic quiver, including wild quivers. Fix k=Fq, 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

  1. Finite-field stability data for an acyclic quiver fixes the representation, Euler, phase, semistability, and quotient-stack conventions.
  2. 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-Ext1 Euler formula without identifying Yoneda and derived Ext1.
  3. 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.
  4. 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.
  5. Quiver Harder–Narasimhan filtrations exist, are unique, and descend proves the choice-free HN result and finite-field descent.
  6. 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.
  7. 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.
  8. 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 CY3 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

DefinitionDefinition: AI-adaptedProof: Not applicableOpen item page →

Finite-field stability data for an acyclic quiver

Definition

Let Q=(Q0,Q1,s,t) be a finite quiver: Q0 and Q1 are finite sets, and s,t:Q1→Q0 give the source and target of each arrow. Assume Q has no directed cycles. For a field K, a finite-dimensional representation M assigns a finite-dimensional K-vector space Mi to each i∈Q0 and a linear map Ma:Ms(a)→Mt(a) to each a∈Q1. A morphism is a family of linear maps at the vertices commuting with all arrow maps. Write AQ(K) for this category and d(M)=(dim⁡KMi)i∈Q0∈NQ0 for its dimension vector. For the finite-field Hall branch, fix k=Fq and write AQ=AQ(k). The next lemma proves the abelian and Euler properties over any field; over k it constructs a small finitary abelian skeleton of AQ, so AQ is essentially small.

For d,e∈ZQ0 define the bilinear form χQ(d,e)=∑i∈Q0diei−∑a:i→jdiej, and its skew-symmetrization ⟨d,e⟩=χQ(d,e)−χQ(e,d). The next lemma proves that χQ(d(M),d(N)) is the Hom-minus-Yoneda-Ext1 dimension for this arrow convention.

Fix zi∈H:={z∈C:Im⁡z>0} for each vertex and extend Z(d)=∑idizi additively. If d∈NQ0 is nonzero, then Im⁡Z(d)=∑idiIm⁡zi>0; thus its principal argument lies in (0,π). For a nonzero representation M, put ϕZ(M)=arg⁡Z(d(M))/π∈(0,1). Call M Z-semistable if every nonzero subrepresentation U⊆M satisfies ϕZ(U)≤ϕZ(M), and Z-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 d, let Rep⁡d(Q)=∏a:i→jHom⁡k(kdi,kdj),Gd=∏i∈Q0GL⁡di,k. The group Gd acts by change of bases. Define Rep⁡dss(Q,Z) geometrically: its points over an algebraic closure kˉ are representations for which every nonzero kˉ-subrepresentation satisfies the semistability inequality. The associated quotient stack is Mdss(Q,Z)=[Rep⁡dss(Q,Z)/Gd]. For d=0, set Rep⁡0ss=Rep⁡0=Spec⁡k. The group G0 is trivial, so its rational-point groupoid has one zero object, trivial automorphism group, and cardinality 1. Here [X/G] denotes the groupoid-valued quotient: over a scheme S its objects are G-torsors on S with equivariant maps to X, and its arrows are equivariant isomorphisms over S. The openness lemma below proves that Rep⁡dss is open.

For a finite groupoid G, define its groupoid cardinality by ∣G∣=∑[x]∈Iso⁡(G)1∣Aut⁡G(x)∣. The rational-point groupoid of Mdss 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.

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

Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity

Statement

Let Q be a finite acyclic quiver and K any field. The category AQ(K) of finite-dimensional representations is abelian. For all X,Y∈AQ(K), the spaces Hom⁡(X,Y) and Yoneda Ext⁡1(X,Y) are finite-dimensional K-vector spaces, and dim⁡KHom⁡(X,Y)−dim⁡KYExt⁡1(X,Y)=χQ(d(X),d(Y)). The explicit projective resolution below shows that the projective-resolution groups Ext⁡AQ(K)r(X,Y) vanish for r≥2; these groups are the cohomology of applying Hom⁡AQ(K)(−,Y) to a projective resolution. If K=Fq, the displayed vector spaces have finite underlying sets and AQ(K) has a small skeleton (a small full subcategory with one representative of each isomorphism class). Thus AQ(K) is essentially small, and this skeleton is a small finitary abelian category. Yoneda Ext⁡1 is classified directly below; it is not identified with derived Ext⁡1 by an unstated theorem.

Facts & Assumptions

Given: A finite acyclic quiver Q, a field K, and X,Y∈AQ(K).

[F1]

For every field K, AQ(K) is the category of vertexwise vector spaces and arrow maps, and χQ is the displayed Euler form (Finite-field stability data for an acyclic quiver).

[F2]

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).

[F3]

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.

1.1F1constructalgebra

For a morphism f:X→Y, its vertexwise kernels form a subrepresentation: if x∈ker⁡fi, then fjXa(x)=Yafi(x)=0 for every arrow a:i→j. The vertexwise cokernels form a quotient representation because Ya(im⁡fi)⊆im⁡fj. 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 AQ(K) abelian.

1.2F1constructalgebra

For i∈Q0, let Pi(v) have basis the directed paths from i to v, with arrow maps given by path concatenation. Acyclicity and finiteness of Q make each path set finite. A morphism Pi→N is uniquely determined by the image of the length-zero path at i, so Hom⁡(Pi,N)≅Ni; evaluation at i preserves epimorphisms, and therefore Pi is projective.

1.3F1constructalgebra

Put C0(X,Y)=⨁iHom⁡K(Xi,Yi),C1(X,Y)=⨁a:i→jHom⁡K(Xi,Yj), and define ∂:C0→C1 by (∂h)a=Yahi−hjXa. Its kernel is exactly Hom⁡AQ(K)(X,Y) by the commuting-square definition of a representation morphism.

2.1F1constructalgebra

For a representation X, define ϵ:⨁iPi⊗KXi→X by p⊗x↦Xp(x), where Xp is the composite arrow map along the path p. Define d:⨁a:i→jPj⊗KXi⟶⨁iPi⊗KXi at a path p:j→v by d(p⊗x)=(p⊗Xa(x))j−((p∘a)⊗x)i. Both terms are finite direct sums of the projectives from step 1.2. Then ϵd=0 because Xp∘a=XpXa.

2.2F1step 1.1choose

Now assume K=Fq. For each dimension vector d, there are finitely many arrow matrix tuples on the fixed spaces Kdi, and the finite group Gd(K) has finitely many orbits on this set. Fix an enumeration of the finite set K; the lexicographically least tuple in each orbit gives a representative without making a choice from an arbitrary family. The union over the set NQ0 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.

3.1step 2.1algebra

At vertex v, ϵ is onto because x∈Xv is the image of id⁡v⊗x. Modulo im⁡d, the relation in step 2.1 replaces (p∘a)⊗x by p⊗Xa(x). Every positive-length path has a unique first arrow, so repeated replacement sends each path tensor to id⁡v⊗Xp(x). Consequently the quotient of the middle term by im⁡d is isomorphic to Xv through ϵ, and ker⁡ϵ=im⁡d.

4.1step 1.2step 2.1step 3.1algebra

The map d is injective. In a nonzero element of its domain, choose the largest length ℓ of a suffix path p with nonzero coefficient. The second term of d(p⊗x) has length ℓ+1. 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 d has length at most ℓ, since no source suffix has length ℓ+1. Thus the length-(ℓ+1) part of d is nonzero, proving injectivity. The displayed sequence is a projective resolution of length one; applying Hom⁡(−,Y) therefore gives Ext⁡AQ(K)r(X,Y)=0 for r≥2.

5.1F1F3step 1.3constructalgebra

A short exact sequence 0→Y→E→X→0 splits as a sequence of vector spaces at each of the finitely many vertices. In the resulting coordinates every arrow of E has block matrix Ea=(Yaξa0Xa),ξa∈Hom⁡K(Xi,Yj). Every tuple ξ∈C1(X,Y) defines such an extension. Changing the vertexwise splittings by h∈C0(X,Y) changes ξ by ∂h. Conversely, an isomorphism of extensions that is the identity on endpoints has block matrix (1hi01) at each vertex and hence changes ξ by exactly ∂h. By [F3], the generated endpoint-fixed Yoneda relation consists of these isomorphisms. The Baer sum of the extensions represented by ξ and η is represented by ξ+η: the pullback of their direct sum along X→X⊕X followed by pushout along Y⊕Y→Y adds the off-diagonal arrow blocks. Pushout along λid⁡Y sends ξ to λξ. Therefore the Yoneda vector-space structure is the quotient structure YExt⁡1(X,Y)≅C1(X,Y)/im⁡∂, a finite-dimensional K-vector space; it is not being identified here with the projective-resolution group of step 4.1.

6.1F1F2step 1.1step 2.2step 1.3step 5.1algebra∎

Both cochain spaces in step 1.3 are finite-dimensional. Rank-nullity for ∂ gives dim⁡ker⁡∂−dim⁡coker⁡∂=dim⁡C0−dim⁡C1=∑idi(X)di(Y)−∑a:i→jdi(X)dj(Y)=χQ(d(X),d(Y)). The kernel and cokernel identifications already proved give the Hom–Yoneda-Ext1 formula and finite-dimensionality over any K. When K=Fq, 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 AQ(K). Thus this small abelian skeleton satisfies the finitary hypotheses of [F2], while AQ(K) is essentially small.

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

The phase of a sum lies between upper-half-plane phases

Statement

Let H={z∈C:Im⁡z>0} and define ϕ(z)=arg⁡(z)/π∈(0,1). For z,w∈H, the phase of z+w lies between ϕ(z) and ϕ(w), strictly between them when they are unequal and equal to their common value when they coincide.

Facts & Assumptions

Given: z,w∈H.

[F1]

The stability convention is H={z:Im⁡z>0} and ϕ(z)=arg⁡(z)/π∈(0,1) (Finite-field stability data for an acyclic quiver).

Proof

Given: The objects and hypotheses in the statement.

1.1F1algebra

Suppose arg⁡z>arg⁡w. Then Im⁡(w‾z)=∣w∣∣z∣sin⁡(arg⁡z−arg⁡w)>0. Consequently Im⁡(w‾(z+w))>0, which, by [F1], gives arg⁡(z+w)>arg⁡w. Also Im⁡((z+w)‾z)=Im⁡(w‾z)>0, so [F1] gives arg⁡z>arg⁡(z+w).

2.1F1step 1.1algebra∎

If arg⁡w>arg⁡z, interchange z,w in step 1.1. If the arguments are equal, z,w are positive real multiples of the same ray, so their sum has that same argument. These cases prove the stated between-phase rule.

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

Semistable loci of finite-quiver representations are open

Statement

Assume the Axiom of Choice. Let Q, k, d, and Z be as in Finite-field stability data for an acyclic quiver. The subset Rep⁡dss(Q,Z) of representations over kˉ that are semistable for every nonzero geometric subrepresentation is Zariski open in Rep⁡d(Q)kˉ.

Facts & Assumptions

Given: A finite acyclic quiver Q, a finite field k, a dimension vector d, and central charges zi∈H.

[F1]

Rep⁡d(Q) 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).

[F2]

Each Grassmannian has a closed Plücker embedding into a projective space (The Plucker image is a closed projective algebraic set).

[F3]

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).

[F4]

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).

[F5]

A projective morphism is proper; this supplier explicitly assumes AC (Projective morphisms are proper).

[F6]

Proper morphisms of schemes are closed, including after base change (Proper morphisms are closed).

[F7]

Under AC, a homogeneous ideal in A[x0,…,xn] defines a closed subscheme of PAn; on D+(xi) its ring is the degree-zero localized polynomial ring modulo the localized ideal (Closed subschemes of projective space and saturated ideals).

[A1]

The Axiom of Choice is assumed only for the projective-morphism properness result [F5] (The Axiom of Choice).

[A2]

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 kˉ, as fixed by Closed projective embedding from a radical homogeneous ideal and its projective-space prerequisite. Thus the finite field k is not substituted for the classical base field (The Axiom of Choice).

Proof

Given: The objects and hypotheses in the statement.

1.1A2F2F3F7constructalgebra

Work over kˉ. By [F2] and [F7], the Plucker equations define a closed projective subscheme whose kˉ-points are the r-planes. On a chart pI≠0, normalize pI=1 and use the signed one-outside coordinates as the entries of a matrix A. The Plucker relation with tuples J∖{j} and I∪{j} expresses each pJ, for j∈J∖I, using coordinates with fewer indices outside I and one-outside coordinates. Induction identifies every pJ in the quotient chart ring with the corresponding maximal minor of (Ir∣A); conversely those minors satisfy every Plucker relation. Hence the chart ring is kˉ[A]. The row spans of (Ir∣A) give a rank-r 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 r=0,n are points. For the Segre equations in [F3], on zi0j0≠0 normalize zi0j0=1 and put ui=zij0 and vj=zi0j, with ui0=vj0=1. The minor relations give zij=uivj in the quotient ring, and substitution and coordinate extraction are inverse maps with kˉ[ui (i≠i0),vj (j≠j0)]. These charts construct the closed Segre embedding. Iterating it embeds the finite product Pe=∏iGr⁡(ei,kdi)kˉ as a closed subscheme of one projective space; if Q0 is empty, Pe is a point. The chart ring surjections remain surjective after adjoining the arrow-matrix coordinates, so Rep⁡d(Q)kˉ×Pe is closed in a relative projective space over Rep⁡d(Q)kˉ. 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 kˉ.

2.1F1F4step 1.1constructalgebra

For each subvector e with 0<e≤d and ϕZ(e)>ϕZ(d), impose in Rep⁡d(Q)kˉ×Pe, for each arrow a:i→j, that the composition Si⟶kdi→Aakdj⟶Qj vanish. Here Si and Qj are the tautological subbundle and quotient bundle constructed in step 1.1; their fibers at Ui,Uj are Ui and kdj/Uj. On the charts from step 1.1 these are polynomial equations, so their common zero locus Ie is closed. Its geometric points are exactly pairs consisting of an arrow-matrix tuple and a subrepresentation of dimension e. The closed inclusion Ie↪Rep⁡d(Q)kˉ×Pe composes with the relative Plucker–Segre closed immersion of step 1.1, so the projection to Rep⁡d(Q)kˉ is projective by [F4].

3.1A1F5F6step 2.1

By [A1] and [F5], the projection in step 2.1 is proper; [F6] then makes its image closed in Rep⁡d(Q)kˉ. Its kˉ-points are exactly the representations with a destabilizing subrepresentation of dimension e.

4.1F1step 3.1algebra

There are finitely many subvectors e with 0<e≤d. 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 Rep⁡dss(Q,Z). If d=0 the union is empty and the whole one-point representation space is open.

5.1A1A2F5F7step 1.1step 3.1∎

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.

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

Quiver Harder–Narasimhan filtrations exist, are unique, and descend

Statement

Let Q be finite and acyclic, let k=Fq, and give every vertex an arbitrary charge zi∈H. Over any field extension K/k, every finite-dimensional representation has a unique filtration 0=M0⊊M1⊊⋯⊊Mr=M whose nonzero factors Mj/Mj−1 are Z-semistable and have strictly decreasing phases. If M is defined over k, the unique filtration of its scalar extension Mkˉ=M⊗kkˉ is Frobenius invariant and descends to k. Consequently geometric semistability of an Fq-representation is equivalent to semistability tested only on its Fq-subrepresentations. Write ∣d∣=∑idi for total dimension.

Facts & Assumptions

Given: A finite acyclic quiver, k=Fq, charges zi∈H, and a finite-dimensional representation over an extension field K/k; for the descent claims, the representation is the scalar extension of an object defined over k.

[F1]

The central charge is additive on short exact sequences, phases lie in (0,1), and semistability is tested on nonzero subrepresentations (Finite-field stability data for an acyclic quiver).

[F2]

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).

[F3]

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.

1.1F1choosealgebra

Let M≠0 have dimension vector d. The nonzero dimension vectors of its subrepresentations form a nonempty subset of the finite set {e:0≤ei≤di}. 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 S⊆M attain both maxima. Every nonzero subobject of S is a subobject of M, so its phase is at most ϕZ(S); hence S is semistable.

1.2F1F2F3

If A,B are semistable and ϕZ(A)>ϕZ(B), then Hom⁡(A,B)=0. Indeed, a nonzero map has a nonzero image I. From 0→ker⁡f→A→I→0, semistability of A and [F3] force ϕZ(I)≥ϕZ(A): if the kernel is zero the phases are equal; if the kernel is nonzero and ϕZ(I)<ϕZ(A), the phase of the sum lies strictly below ϕZ(A), contradicting Z(A)=Z(ker⁡f)+Z(I). But I⊆B and semistability of B give ϕZ(I)≤ϕZ(B), a contradiction.

2.1F1F2F3step 1.1

If T⊆M/S is nonzero, let P⊆M be its inverse image. Then 0→S→P→T→0 is exact. If ϕZ(T)>ϕZ(S), [F3] gives ϕZ(P)>ϕZ(S), contrary to maximality of the phase of S. If ϕZ(T)=ϕZ(S), additivity and [F3] give ϕZ(P)=ϕZ(S), while ∣d(P)∣>∣d(S)∣, contrary to the second maximum. Thus every nonzero subobject of M/S has phase strictly less than ϕZ(S).

2.2F1F2step 1.2construct

Consider two filtrations with first subobjects S,S′ of phases p,p′. If p>p′, every factor in the quotient filtration of M/S′ has phase below p′. Step 1.2 therefore makes every map from S to each such factor zero. Induction along the finite quotient filtration shows Hom⁡(S,M/S′)=0: a map whose projection to the last factor is zero factors through the preceding subobject. Thus the inclusion of S in M factors through S′, giving a nonzero map S→S′, contrary to Hom⁡(S,S′)=0 from step 1.2. Interchanging S,S′ similarly rules out p′>p; hence p=p′. Applying step 1.2 to all factors of both quotients now gives S⊆S′ and S′⊆S, hence S=S′. Induction on the quotient proves equality of the full filtrations.

3.1F2step 1.1step 2.1construct

Induct on ∣d(M)∣. The zero representation has the empty filtration. For M≠0, the quotient M/S 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 ϕZ(S). Pulling that filtration back along M→M/S and placing S first gives the required filtration of M.

4.1F1F2step 3.1step 2.2algebra

Let M be defined over k, set Mkˉ=M⊗kkˉ, and let σ(x)=xq be Frobenius. Applying σ to a filtration preserves the arrow maps of Mkˉ, 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 σ gives another such matrix for the same subspace, so uniqueness makes the matrix fixed entrywise. Its entries lie in Fq, and the arrow maps of M preserve these descended subspaces. Thus the filtration descends to k.

5.1F1step 1.1step 4.1∎

If an Fq-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 Fq, contradicting Fq-semistability. Conversely, an Fq-subrepresentation extends to kˉ with the same dimension vector and phase. This proves the stated equivalence and the result.

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

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 Q be finite and acyclic over k=Fq, and let d∈NQ0. In this statement, include the zero representation as Z-semistable, without assigning it a phase. The rational-point groupoid of Mdss(Q,Z) is finite and is equivalent to the groupoid whose objects are Z-semistable Fq-representations of dimension d and whose arrows are their representation isomorphisms. Its groupoid cardinality is therefore ∑[M]: d(M)=d, M  Z-semistable1∣Aut⁡AQ(M)∣.

Facts & Assumptions

Given: A finite acyclic quiver, a finite field k, a dimension vector d, and vertex charges in H.

[F1]

The quotient stack [X/G] has objects given by G-torsors with equivariant maps to X; its semistable representation locus is open (Finite-field stability data for an acyclic quiver, Semistable loci of finite-quiver representations are open).

[F2]

Geometric HN filtrations of representations over Fq are Frobenius invariant and descend to Fq; hence geometric and finite-field semistability agree (Quiver Harder–Narasimhan filtrations exist, are unique, and descend).

[A1]

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.

1.1A1F1constructchoose

Under the inherited assumption [A1], the semistable locus is the open subscheme from [F1]. An object of its quotient groupoid over Fq is a tuple of GL⁡di-torsors together with an equivariant semistable representation. A GL⁡n-torsor is the frame torsor of its associated n-dimensional vector space. Every finite-dimensional vector space over Fq has a basis, so that associated space is isomorphic to Fqn and its frame torsor is trivial. Applying this at the finitely many vertices trivializes the product Gd-torsor. Thus every quotient-stack object is isomorphic to a representation on the standard spaces kdi.

2.1givenF1F2step 1.1algebra

Under a chosen trivialization, an equivariant map to Rep⁡dss is an arrow-matrix tuple. Two trivialized objects are isomorphic exactly when their tuples differ by change of bases in Gd(Fq). If d≠0, [F2] identifies the rational tuples in the geometric semistable locus with the finite-field semistable representations. If d=0, the geometric condition is vacuous, the representation space is a point, and G0 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.

3.1F1step 2.1algebra∎

There are finitely many arrow-matrix tuples on the fixed finite vector spaces, and each automorphism group is a subgroup of the finite group Gd(Fq). Hence the groupoid is finite. Under the equivalence of step 2.1, the stabilizer of a tuple is exactly Aut⁡AQ(M). Substituting these stabilizers into the groupoid-cardinality definition in Finite-field stability data for an acyclic quiver gives the displayed sum.

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Subobject-first Hall completion and quantum tori for finite quivers

Definition

Fix Q, k=Fq, and Z as in Finite-field stability data for an acyclic quiver. For a representation M, write aM=∣Aut⁡AQ(M)∣ and let δM be the basis function of its isomorphism class. Let SQ be the small finitary abelian skeleton constructed in Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity. Define HQ:=HSQ,Q, identifying its basis with the isomorphism classes of AQ. Fullness and transport of subobjects and cokernels along isomorphisms preserve the Hall coefficients. Thus HQ 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 [A]∗qf[B] counts sequences 0→B→L→A→0, and identify the basis symbol [M] with the characteristic function δM. Define the subobject-first product by f⋆g:=g∗qff. Then (f⋆g)(L)=∑U⊆Lf(U)g(L/U), where the sum is over subobject classes of L: monomorphisms into L modulo isomorphisms of their domains commuting with the monomorphism. Distinct embedded subobjects are counted separately even when their domains are isomorphic. Put κM=aMδM.

For d∈NQ0, let HQ,d be the span of classes of dimension vector d. It is finite-dimensional: the representation set on the standard spaces kdi is finite. Define the dimension completion H^Q=∏d∈NQ0HQ,d. The product is extended degreewise; each coefficient uses finitely many decompositions d=a+b. There is no analytic convergence assertion. The all-object and phase factors are Aall=∑[M]δM,SZ(ϕ)=δ0+∑[M]M≠0, ϕZ(M)=ϕ, M Z-semistableδM. Each is an element of H^Q because each homogeneous component has finite support.

Let t=q>0 and Kq=Q(q). Take the completed Euler torus and skew torus over Kq, with bases Xd and xd, respectively, and products XdXe=q−χQ(e,d)Xd+e,xd∗xe=t−⟨e,d⟩xd+e. Their completions use the same dimension product. The next theorem proves associativity and gives the continuous Euler and skew integration maps.

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Finite-quiver Hall multiplication counts extensions by automorphism orbits

Statement

Let U,V be finite-dimensional representations over Fq. For κM=∣Aut⁡(M)∣δM and the subobject-first product from Subobject-first Hall completion and quantum tori for finite quivers, κU⋆κV=∑[M]∣YExt⁡1(V,U)M∣∣Hom⁡(V,U)∣ κM, where YExt⁡1(V,U)M is the set of endpoint-fixed Yoneda classes of 0→U→E→V→0 whose middle term is isomorphic to M.

Facts & Assumptions

Given: Finite-dimensional U,V, an isomorphism class [M], and the subobject-first Hall product.

[F1]

In the generic untwisted Hall convention, [A]∗qf[B] counts short exact sequences 0→B→L→A→0 (The untwisted Hall algebra of a finitary abelian category).

[F2]

The local convention is f⋆g=g∗qff, and κU=∣Aut⁡(U)∣δU (Subobject-first Hall completion and quantum tori for finite quivers).

[F3]

The sets Hom⁡(V,U) and YExt⁡1(V,U) are finite; the latter is the endpoint-fixed Yoneda class set (Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity).

[F4]

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.

1.1F1F2construct

Fix the middle object to be M. The coefficient of δM in δU⋆δV counts subobjects S⊆M with S≅U and M/S≅V, by [F1] and [F2]. For each such S, the monomorphisms U→M with image S form a set of size ∣Aut⁡(U)∣; the epimorphisms M→V with kernel S form a set of size ∣Aut⁡(V)∣. These choices are independent. Hence the number of endpoint-fixed short exact sequences with middle object literally M is gV,UM∣Aut⁡(U)∣∣Aut⁡(V)∣, where gV,UM is the Hall coefficient of [F1].

1.2F3constructalgebra

The finite group Aut⁡(M) acts on those sequences by (i,p)↦(gi,pg−1). Its orbits are exactly the endpoint-fixed Yoneda classes with middle term isomorphic to M: an isomorphism from any middle object E≅M transports its sequence to one on M, and changing that isomorphism changes the result by this action. The stabilizer of a sequence (i,p) consists of g with gi=i and pg=p. Put h=g−1. Since hi=0 and p is an epimorphism, h factors uniquely as h=ifp for a unique f:V→U. Conversely, 1+ifp is invertible because (ifp)2=0, with inverse 1−ifp. Thus every stabilizer has exactly ∣Hom⁡(V,U)∣ elements.

2.1F1F2F3F4step 1.1step 1.2algebra∎

For a fixed sequence, the map from Aut⁡(M) to its orbit has fibers exactly the cosets of its stabilizer, so that orbit has size ∣Aut⁡(M)∣/∣Hom⁡(V,U)∣. Summing over the ∣YExt⁡1(V,U)M∣ orbits gives gV,UM∣Aut⁡(U)∣∣Aut⁡(V)∣=∣Aut⁡(M)∣ ∣YExt⁡1(V,U)M∣∣Hom⁡(V,U)∣. Multiplying the coefficient of δM in κU⋆κV by the definition of κM yields precisely the claimed coefficient. Summing over the finitely many possible middle terms is valid by [F3] and [F4].

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Euler and skew integration are multiplicative for finite acyclic quivers

Statement

Let Q be a finite acyclic quiver over k=Fq, let t=q>0, 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 I(f)=∑[M]f(M)∣Aut⁡(M)∣Xd(M),J(f)=∑[M]tχQ(d(M),d(M))f(M)∣Aut⁡(M)∣xd(M) are unital algebra homomorphisms to the completed tori with products XdXe=q−χQ(e,d)Xd+e,xd∗xe=t−⟨e,d⟩xd+e. These are separate normalizations: the first is the Euler form target, while the second uses the skew-symmetrized form and the diagonal factor tχQ(d,d).

Facts & Assumptions

Given: A finite acyclic quiver over Fq, the subobject-first Hall convention, and t=q>0.

[F1]

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.

[F2]

The normalized basis satisfies κU⋆κV=∑[M]∣YExt⁡1(V,U)M∣∣Hom⁡(V,U)∣κM (Finite-quiver Hall multiplication counts extensions by automorphism orbits).

[F3]

The representation category has a small finitary abelian full skeleton. The finite vector spaces of Hom and Yoneda Ext1 satisfy dim⁡Hom⁡(V,U)−dim⁡YExt⁡1(V,U)=χQ(d(V),d(U)) (Finite acyclic quiver representations: heredity, Euler form, and finite-field finitarity).

[F4]

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).

[F5]

The homogeneous Hall products have finite support (Untwisted Hall structure constants and products are finite).

Proof

Given: The objects and hypotheses in the statement.

1.1F1F3F4algebra

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 ∗q for this quotient-first product. By [F1], f⋆g=g∗qf, so (f⋆g)⋆h=h∗q(g∗qf)=(h∗qg)∗qf=f⋆(g⋆h) by [F4]. The zero-object class is the unit for ∗q, hence also for ⋆.

1.2F1F5algebra

The degree of an extension is the sum of the endpoint dimension vectors. For a fixed output degree n, a product coefficient uses only the finitely many pairs d+e=n; each HQ,d is finite-dimensional by the representation-matrix definition. Thus [F5] extends the product degree by degree to H^Q, and truncating above total dimension D changes no coefficient of dimension at most D. This is continuity for the total-dimension filtration.

1.3F1F2F3algebra

On a normalized basis vector, I(κM)=Xd(M) because κM=∣Aut⁡(M)∣δM. For d=d(U) and e=d(V), [F2] gives I(κU⋆κV)=∣YExt⁡1(V,U)∣∣Hom⁡(V,U)∣Xd+e. By [F3], both sets are finite vector spaces and the ratio of their cardinalities is qdim⁡YExt⁡1(V,U)−dim⁡Hom⁡(V,U)=q−χQ(e,d). This is exactly I(κU)I(κV) in the Euler target.

1.4F1F2F3algebra

On the same basis, J(κM)=tχQ(d,d)xd. Applying [F2] and [F3] to κU⋆κV gives its J-image coefficient t−2χQ(e,d)+χQ(d+e,d+e). By bilinearity, χQ(d+e,d+e)=χQ(d,d)+χQ(e,e)+χQ(d,e)+χQ(e,d). Since ⟨e,d⟩=χQ(e,d)−χQ(d,e) and q=t2, the coefficient becomes tχQ(d,d)+χQ(e,e)−⟨e,d⟩, which is exactly the coefficient of J(κU)∗J(κV) in the skew target.

2.1F1step 1.1step 1.2step 1.3step 1.4algebra∎

Bilinearity of χQ makes the Euler twist associative: both parenthesizations of XdXeXf have exponent −χQ(e,d)−χQ(f,d)−χQ(f,e). 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 I and J 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 I and J to unital algebra homomorphisms on the completions.

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Completed Hall wall crossing for finite acyclic quivers

Statement

Let Q be any finite acyclic quiver over Fq, including wild quivers, and let Z− and Z+ be any two assignments of upper-half-plane charges zi∈H. In the dimension completion of the subobject-first Hall algebra, Aall=∏ϕ∈ΦZ decreasingSZ(ϕ),ΦZ={ϕZ(e):0≠e∈NQ0}. The product is degreewise finite and includes all semistable objects, whether stable or strictly semistable. Applying either Euler integration I or skew integration J gives equal completed ordered products for Z− and Z+. Each integrated ordered product has constant term 1 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 Fq and two collections of charges Z−,Z+ with each vertex charge in H.

[F1]

Aall and SZ(ϕ) are the degree-completed sums of all objects and of semistable objects at phase ϕ; the product is subobject-first (Subobject-first Hall completion and quantum tori for finite quivers).

[F2]

Every representation has a unique HN filtration with nonzero semistable factors of strictly decreasing phase (Quiver Harder–Narasimhan filtrations exist, are unique, and descend).

[F3]

Both I and J 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.

1.1F1constructalgebra

Fix distinct phases ϕ1>⋯>ϕr. Iterating the defining formula (f⋆g)(M)=∑U⊆Mf(U)g(M/U) from [F1], with left-associated products, shows that the coefficient of δM in SZ(ϕ1)⋆⋯⋆SZ(ϕr) is the number of weak flags 0=M0⊆M1⊆⋯⊆Mr=M for which every nonzero factor Mj/Mj−1 is semistable of phase ϕj. The induction step chooses Mr−1⊆M in the last binary product and then uses the previous flag inside Mr−1; zero quotients exactly represent skipped phases.

1.2F1algebra

For a fixed dimension vector d, any contributing nonzero factor has dimension vector e with 0<e≤d. There are finitely many such vectors and therefore finitely many possible phases. A contributing flag has at most ∣d∣ nonzero factors. Thus the ordered product over all phases is a finite computation in each degree and defines an element of H^Q.

2.1F1F2step 1.1step 1.2

By [F2], for every M exactly one flag counted by the preceding flag-count argument has strictly decreasing semistable factors: its unique HN filtration. Therefore the coefficient of each δM in the ordered product is 1, which is the coefficient of δM in Aall. The zero object contributes the common degree-zero unit. This proves the Hall identity.

3.1F3step 2.1algebra

Apply I and J 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 Z− and Z+.

4.1F1F3step 1.2step 3.1algebra∎

Write each integrated phase factor as 1+gϕ, where every term of gϕ has positive total dimension. Then (1+gϕ)−1=1−gϕ+gϕ2−⋯, 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 PZ and the reverse-ordered product of these inverses both converge degreewise. Their finite truncations are mutual inverses, and continuity of multiplication gives PZPZ−1=PZ−1PZ=1. Thus a↦PZaPZ−1 is a continuous automorphism with inverse a↦PZ−1aPZ. Step 3.1 gives the same PZ for Z− and Z+, so these conjugations agree. All limits are formal in the degree completion.

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Finite-quiver Hall counts and the limits of DT/BPS interpretation

Remarks

The coefficients of J(SZ(ϕ)) are finite-field, Euler-normalized semistable groupoid masses: the weight of [M] is tχQ(d(M),d(M))/∣Aut⁡(M)∣. 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

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