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✓ 15 results · all verified · 0 also independently AI-judged
Every result on this page is machine-checked by a proof checker and read in full and owner-audited; the judge is an additional, independent cross-model AI review of the proofs. The 15 not AI-judged were verified by owner audit (typically over a confirmed judge false positive), not failures.

Euler-Twisted Hall Products, Green Coproducts, and Quantum Groups

1 · Prerequisites

2 · Summary

The Euler-twisted Hall product uses a supplied small finite-field hereditary category and the subobject convention 0→N→R→M→0. The Green coproduct lands in a coefficientwise completed tensor space; its image products converge and its compatibility is proved by the full cross-square fiber count. The extended algebra uses left-torus normal order and the DJ-compatible coproduct. The ordinary tensor target is asserted when every basis coproduct has finite support.

For every finite loopless quiver, using finite-dimensional nilpotent representations when oriented cycles occur, the fixed-parameter Ringel map is an injective extended-positive-Borel map with composition image. The numerical Serre-only presentation is proved equal to the actual integral specialization at the prime-power parameter; generic nondegeneracy alone is not used as specialization. Reflection, finite-field Schur descent and explicit affine flag families prove that composition equals full Hall exactly when every connected graph component is finite ADE. Disconnected and empty quivers are included.

Companion: green-hall-bialgebras-and-quantum-group-realizations-examples.

3 · Logical flowchart

4 · Definitions, theorems and proofs

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The Hall-normalized extended positive Borel of a loopless quiver

Definition

Let Q be a finite loopless quiver over Fq. Write cij for the number of arrows i→j, set ν=q>1, and define the symmetric Cartan matrix aij=2δij−cij−cji. Let Q(ν) be the coefficient field. Define the extended positive Borel algebra BQ+ to be the Q(ν)-algebra generated by Ei and invertible commuting Ki±1, with KiKi−1=1,KiEjKi−1=νaijEj, and, for i≠j and m=1−aij, ∑r=0m(−1)r(mr)νEim−rEjEir=0. The Gaussian coefficients use the symmetric convention of Quantum integers, factorials, Gaussian binomials and divided powers at qi. The formulas Δ(Ei)=Ei⊗Ki−1+1⊗Ei,Δ(Ki)=Ki⊗Ki, are the coproduct convention intended for this presentation; their well-definedness on the defining relations is checked using The coproduct preserves the positive and negative quantum Serre ideals. The positive half is the subalgebra generated by the Ei alone; adjoining the Ki±1 gives the extended positive Borel.

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

A symmetric Gaussian alternating sum vanishes in the Serre range

Statement

Let m≥1, and let d∈Z satisfy 1−m≤d≤m−1 and d≡m−1(mod2). With the symmetric Gaussian binomial Cm,n=(mn)ν from Quantum integers, factorials, Gaussian binomials and divided powers at qi, ∑n=0m(−1)nν−dnCm,n=0 for every real ν>1.

Facts & Assumptions

Given: The integer range and parity above, and the symmetric Gaussian coefficient convention.

[F1]

The Gauss product formula is a Laurent-polynomial identity and remains valid after substituting ν−1 for its parameter (The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality).

Proof

technique · direct
1.1givenF1algebra

Substituting ν−1 for the parameter in [F1] gives ∏j=0m−1(1+ν−2jz)=∑n=0mν−n(m−1)Cm,nzn. This identity is valid at the real number ν>1 because both sides are Laurent polynomials. Set z=−νm−1−d; the right side becomes exactly ∑n=0m(−1)nν−dnCm,n.

2.1givenstep 1.1algebra∎

The parity assumption makes j=(m−1−d)/2 an integer, and the bounds on d give 0≤j≤m−1. The factor indexed by this j on the left side of step 1.1 is 1−ν−2jνm−1−d=0. Therefore the right side, which is the sum in the Statement, is zero.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

A zero Yoneda splice factors through the middle object

Statement

Let E be 0→A→B→pC→0 and let F be 0→C→D→X→0 in an abelian category. If their splice is zero in YExt⁡2(X,A), then there is an extension G of X by B whose pushout along p:B→C is equivalent to F. Conversely every such pushout has zero splice with E.

Facts & Assumptions

Given: The two displayed short exact sequences in an arbitrary abelian category. Write their maps as i:A→B, p:B→C, j:C→D, and q:D→X.

[F1]

Two-fold equivalence is generated by finite zigzags of endpoint-fixed chain maps (An n-fold Yoneda extension, Equivalence of n-fold extensions). Its zero representative is Z:0→A→1A→0X→1X→0.

[F2]

Pullback and pushout short extensions are exact (Pullback and pushout of an extension). An endpoint-fixed map between short exact sequences is an isomorphism: its kernel is zero by first factoring through the left kernel, and its cokernel is zero by first factoring through the right cokernel; the coimage-image axiom then makes it invertible (Abelian category).

Proof

technique · direct
1.1F2construct

Call a filling of the displayed two-extension an object T with an exact sequence 0→B→bT→tX→0 and a map r:T→D such that rb=jp and qr=t, for which 0→A→biT→rD→0 is exact. A lift G in the statement is exactly such a filling: its pushout along p is T/A, and an endpoint-fixed equivalence to F is an isomorphism by [F2]. Conversely the quotient map r identifies that pushout with F. Thus it suffices to prove that existence of a filling is invariant under each direction of an endpoint-fixed chain map of two-extensions.

1.2F1F2construct

Consider any such chain map with middle maps u:B→B′ and v:D→D′. Factoring the differentials through their images gives c:C→C′ satisfying ui=i′, p′u=cp, vj=j′c, and q′v=q. The natural maps B→B′×C′C and C′⨿CD→D′ induce identities on the endpoints of the respective short exact sequences. They are isomorphisms by [F2]. In particular B=B′×C′C and F′=c∗F, up to these specified isomorphisms.

2.1F2step 1.1step 1.2construct

If the unprimed two-extension has a filling T, push 0→B→T→X→0 out along u to obtain 0→B′→T′→X→0. The maps T→rD→vD′ and B′→p′C′→j′D′ agree on B, so induce r′:T′→D′. Quotienting the pushout by the common copy of A gives T′/A≅C′⨿C(T/A)≅C′⨿CD≅D′. These isomorphisms follow directly from the universal property of a cokernel and a pushout: a map out of either side is precisely a compatible pair of maps annihilating A. Consequently ker⁡r′=A and r′ is epic. This is a filling of the primed extension.

2.2F2step 1.1step 1.2construct

If instead the primed extension has a filling T′, form T=T′×D′D using its quotient r′:T′↠D′ and v. The projection r:T→D is epic with kernel A by pullback exactness. Set t=qr, which is epic. Its kernel is T′×D′C, where C→D′ is j′c. Since the inverse image of C′⊂D′ in T′ is B′, this kernel is B′×C′C≅B by step 1.2. The induced B→T satisfies rb=jp and identifies its copy of A with ker⁡r. Thus T is a filling of the unprimed extension. Every object and morphism used here is a finite pullback or pushout; the argument uses neither resolutions nor a choice principle.

3.1F1step 1.1step 2.1step 2.2construct

The zero representative Z has filling A⊕X, with its two evident split short exact sequences. If the given splice is zero, [F1] supplies an actual finite zigzag from it to Z. Traverse this zigzag backwards starting with that filling, applying step 2.1 when the traversal follows a chain map and step 2.2 when it opposes one. Finite induction produces a filling of the given splice, hence the required G. This explicitly supplies the factorization data through every switch, including switches whose intermediate kernels change.

4.1F1F2step 1.1construct∎

Conversely let a filling T be given. Form H=B×CB, with first projection h:H→B and second projection s:H→B. The sequence 0→A→(i,0)H→sB→0 is split by the diagonal and has a retraction ρ:H→A specified by iρ=h−s. Splice this split extension with 0→B→bT→X→0 to obtain L:0→A→H→bsT→X→0. There is an endpoint-fixed chain map L→EF, with middle maps h and r, since jph=jps=rbs. There is also an endpoint-fixed chain map L→Z, with middle maps ρ and t; the differential square commutes because tbs=0. Hence EF←L→Z is a concrete finite zigzag, proving the splice is zero.

Source notes

The proof supplies directly, for degree two, the finite-switch data underlying Mitchell VII, Lemma 4.1. It uses the endpoint-fixed chain-map formulation of equivalence rather than assuming an isomorphism of the middle terms. It does not invoke the general higher-degree switch lemma.

LemmaStatement: Literature-sourcedProof: AI-adaptedjudge pass (gpt-6-luna)Open item page →

Low-degree exact sequences for Yoneda Ext in both variables

Statement

For a short exact sequence 0→A→iB→pC→0 and an object X in an abelian category, the sequence 0→Hom⁡(X,A)→Hom⁡(X,B)→Hom⁡(X,C)→δYExt⁡1(X,A)→YExt⁡1(X,B)→YExt⁡1(X,C)→∂YExt⁡2(X,A) is exact at every term before the final YExt⁡2 term. The boundary δ pulls back the given extension along a map X→C; ∂ splices it with a short extension of X by C. The dual sequence in the first Ext variable is exact at the corresponding terms: 0→Hom⁡(C,X)→Hom⁡(B,X)→Hom⁡(A,X)→YExt⁡1(C,X)→YExt⁡1(B,X)→YExt⁡1(A,X)→YExt⁡2(C,X).

Here exactness means that the image at each asserted term equals the preimage of the zero class. This interpretation is valid even when a Yoneda class collection is a proper class. When the displayed class collections are sets, equip them with the Baer operations; the displayed sequences are then exact sequences of abelian groups.

Facts & Assumptions

Given: The displayed short exact sequence E and object X, with no projective, injective, or choice assumption.

[F1]

Pullback and pushout are the exact constructions of Pullback and pushout of an extension. An endpoint-fixed map of short exact sequences is invertible by its zero kernel and cokernel in Abelian category.

[F3]

A splice EF is zero exactly when F lifts to an extension by B (A zero Yoneda splice factors through the middle object).

Proof

technique · direct
1.1F1F2construct

Every displayed map has the asserted direction: Hom uses composition; the two maps between short extension classes are i∗ and p∗; δ(f)=f∗E; and ∂[F]=[EF]. Universal properties send endpoint-fixed maps to endpoint-fixed maps, so pullback, pushout, and splicing respect the generated equivalence relation. These constructions commute with finite direct sums. Pullbacks and pushouts in independent endpoints commute, as is seen by their common universal property. Consequently the maps between short extension classes preserve Baer addition.

1.2F1F2construct

Exactness at the first three Hom terms follows from the kernel property of i and the cokernel property of p: a morphism X→B is killed by p exactly when it factors uniquely through i. At Hom⁡(X,C), a map f belongs to ker⁡δ exactly when f∗E splits. A section of that pullback is exactly a map s:X→B satisfying ps=f. Thus ker⁡δ=im⁡(p∘−).

2.1F1F2step 1.1constructalgebra

The connecting maps are additive as well. For f,g:X→C, form the pullback of E⊕E along (f,g):X→C⊕C and then push out along A⊕A→∇A. Addition B⊕B→B induces an endpoint-fixed map from this short extension to (f+g)∗E, proving δ(f+g)=δ(f)+δ(g). For the other connecting map, use the two-fold Baer construction: direct sum, diagonal pullback at X, codiagonal pushout at A. Write F0=ΔX∗(F⊕F′), whose kernel is C⊕C. Then F+F′=∇C∗F0. Put H=B×C(C⊕C), with pullback along ∇C. The map B⊕B→H induced by ∇B and p⊕p induces an isomorphism ∇A∗(E⊕E)≅∇C∗E of extensions of C⊕C by A. Finally the defining pushout map F0→∇C∗F0 and pullback map ∇C∗E→E give an endpoint-fixed chain map between their splices. These explicit maps identify the two-fold Baer representative of [EF]+[EF′] with [E(F+F′)]. Thus ∂ preserves addition wherever the extension-class collections are sets; the same formulas hold on classes.

2.2F1F2step 1.1construct

Let H:0→A→aT→tX→0. If i∗H splits, its middle pushout P=B⨿AT admits a retraction to its subobject B. Composing T→P with this retraction gives h:T→B with ha=i. Hence ph factors uniquely through t as f:X→C. The pair (h,t) gives an endpoint-fixed map H→f∗E, so [H]=δ(f). Conversely i∗E splits: on its pushout B⨿AB, the two identity maps to B induce a retraction onto the first copy of B. Pulling back along f shows i∗δ(f)=0. This proves exactness at YExt⁡1(X,A).

2.3F1F2step 1.1construct

Let H:0→B→bT→tX→0 and suppose p∗H splits. A retraction from its middle pushout to C, composed with T's pushout map, yields h:T→C satisfying hb=p. Let K=ker⁡h. The kernel of t∣K is A, and t∣K:K→X is epic. For the last assertion without elements, if z:X→Y satisfies zt∣K=0, then zt factors through h, since h is epic and K=ker⁡h. Write zt=wh; restricting to B gives wp=0, so w=0 and then z=0. Thus the cokernel of t∣K is zero. The resulting extension 0→A→K→X→0 pushes out along i to H: the map B⨿AK→T induced by b and the inclusion of K is an endpoint-fixed short-extension isomorphism. Conversely p∗i∗H′=0 for every H′ by pi=0, since pushout along the zero map is split. Therefore exactness holds at YExt⁡1(X,B).

3.1F3step 1.2step 2.2step 2.3

At YExt⁡1(X,C), [F3] states precisely that ∂[F]=0 if and only if [F] lies in the image of p∗. This proves every asserted exactness in the covariant sequence, with no assertion of surjectivity onto the final term.

4.1F1F2step 1.1step 2.1step 1.2step 2.2step 2.3step 3.1∎

The opposite of an abelian category is abelian: kernels and cokernels interchange, biproducts remain biproducts, and the coimage-image isomorphism dualizes. Reversing all arrows therefore identifies its short and two-fold extensions, endpoint-fixed zigzags, pullbacks, pushouts, and Baer operations with the corresponding dual constructions in the original category. Apply steps 1.1–3.1 in that opposite category to 0→C→B→A→0 and X. The resulting covariant sequence is exactly the second displayed sequence; its first connecting map pushes E out along A→X, and its last connecting map splices an extension of A by X on the left of E. This proves all its asserted exactness.

Remarks

The assertion is a representative-level image-equals-kernel statement in every abelian category. Where Yoneda extension classes form sets, these are the usual exact sequences of abelian groups. No implicit set-smallness theorem for arbitrary abelian categories, and no identification with derived Ext, is needed for the proof.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

Finite-field hereditary Hall categories

Definition

A finite-field hereditary Hall category is a supplied small Fq-linear abelian category A with the following properties:

  1. For every pair M,N, Hom⁡A(M,N) is a finite-dimensional Fq-vector space and the Yoneda extension group YExt⁡1(M,N) is finite-dimensional over Fq. Its addition is Baer sum; scalar multiplication by λ∈Fq is pushout along λid⁡N.
  2. For every M,N, YExt⁡2(M,N)=0, where a two-fold extension is an exact sequence 0→N→E1→E0→M→0 modulo endpoint-fixed chain-map equivalence (An n-fold Yoneda extension, Equivalence of n-fold extensions).
  3. Smallness and the finiteness conditions of the Hall definition hold (Small finitary abelian categories for Hall multiplication).

Here Fq-linear means that every Hom set is a vector space and composition is bilinear. “Hereditary” in this page means exactly the stated vanishing of Yoneda Ext⁡2; no projective or injective resolutions, derived-Ext identification, or choice principle is built into the definition. Under these conditions the Euler form used below is ⟨[M],[N]⟩=dim⁡FqHom⁡(M,N)−dim⁡FqYExt⁡1(M,N).

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

Finite-dimensional representations of an acyclic quiver form a hereditary finitary Hall category

Statement

Let Q be a finite acyclic quiver and k=Fq. A representation is finite-dimensional at every vertex, with one linear map for each arrow. The category Rep⁡k(Q) is essentially small. Use a small skeleton RQ, for example the one obtained by fixing the spaces kdi and retaining one arrow-matrix tuple from each orbit under vertexwise change of basis. This skeleton is a hereditary finitary abelian category in the sense of Finite-field hereditary Hall categories. Its simple objects are the vertex representations Si, its Grothendieck group is freely generated by [Si] and is isomorphic to ZQ0, and dim⁡kYExt⁡1(Si,Sj)=cij, where cij is the number of arrows i→j. For any two representations V,W, its Euler form is explicitly ⟨[V],[W]⟩=∑i∈Q0dim⁡Vidim⁡Wi−∑a:i→jdim⁡Vidim⁡Wj.

Facts & Assumptions

Given: A finite acyclic directed graph Q and the finite field k.

[F1]

A finite-dimensional representation consists of finite-dimensional vertex spaces and arrow maps; kernels and cokernels are computed vertexwise, and a finite-dimensional representation has finite length because total vector-space dimension strictly decreases along every proper subobject chain.

[F2]

For a finite-field hereditary Hall category, Hom and Yoneda Ext⁡1 are finite-dimensional k-spaces and Yoneda Ext⁡2 vanishes (Finite-field hereditary Hall categories).

[F3]

K0 is generated by object classes with the relation [B]=[A]+[C] for each short exact sequence (Grothendieck group of an essentially small abelian category).

[F4]

Baer sum is pullback along the diagonal followed by pushout along the codiagonal (The Baer sum of extension classes), and it makes extension classes an abelian group (Baer sum makes extension classes an abelian group).

Proof

technique · direct
1.1F1construct

Fix orderings of the finite sets Q0, Q1, and k. Kernels, images and cokernels of a morphism of representations are formed at each vertex, with the induced arrow maps; the vector-space kernel and cokernel identities imply the abelian-category axioms vertexwise. For each dimension vector, enumerate the finitely many arrow-matrix tuples on the fixed spaces kdi and retain the lexicographically least tuple in each orbit under ∏iGL⁡di(k). Their union RQ is an explicit small skeleton; no representatives from a proper class are selected.

1.2F1construct

For a vertex i, let Pi have at vertex j the vector space with basis the directed paths i→j, with arrows acting by path extension. Acyclicity and finiteness of Q imply there are finitely many paths, so Pi is finite-dimensional. Evaluation gives a natural isomorphism Hom⁡(Pi,W)≅Wi; since evaluation is exact, Pi is projective in Rep⁡k(Q). Its chosen representative in RQ is projective as well, since the skeleton is equivalent to the full representation category.

1.3F1F3algebra

The simple Si is k at vertex i and zero elsewhere. If a representation is simple, choose a sink i in its nonzero support; a one-dimensional subspace at that vertex is a nonzero subrepresentation, so simplicity forces the representation to equal Si. A composition series then shows [V]=∑i(dim⁡Vi)[Si] in K0 by [F3]. The dimension-vector map K0→ZQ0 sends [Si] to the standard basis vector; it is inverse to the map sending that vector to [Si].

2.1F1step 1.1given

Every Hom set is a subset of the finite product ∏iHom⁡k(Vi,Wi) and is therefore finite. For fixed endpoints V,W, an extension has vertex dimensions dim⁡Vi+dim⁡Wi; there are only finitely many arrow-matrix collections and endpoint maps in those dimensions. Yoneda classes are a quotient of this finite set, so YExt⁡1(V,W) is finite.

2.2F1step 1.2construct

For a representation V, define P0(V)=⨁iPi⊗kVi,P1(V)=⨁a:i→jPj⊗kVi. The augmentation P0(V)→V sends a path p:i→r tensored with v to the image of v under the composite map Vp. For a:i→j and a path p:j→r, the differential sends p⊗v to (pa)⊗v−p⊗Va(v). These maps commute with every arrow.

2.3F1F4step 1.3construct

In an extension 0→Sj→E→Si→0, the vertex dimensions are fixed. If i≠j, all arrow maps vanish except the maps on arrows i→j, each of which is a scalar in k. Endpoint-fixed equivalence leaves these scalars unchanged, and every scalar tuple defines an extension. Under Baer sum, the direct sum is pulled back along the diagonal and pushed out along the codiagonal; on each arrow coordinate these two operations add the two scalars. Pushing out along multiplication by λ∈k multiplies each coordinate by λ. If i=j, looplessness leaves every arrow map zero and the extension splits. Thus YExt⁡1(Si,Sj)≅kcij as k-spaces.

2.4F1F4step 1.3constructalgebra

More generally, in an extension 0→W→E→V→0, choose a vector-space splitting at each vertex. Each arrow map on Ei=Wi⊕Vi then has block form (Waξa0Va) with ξa:Vi→Wj. Changing the vertex splittings by maps θi:Vi→Wi changes the family (ξa) by the image of ∂(θ)a=Waθi−θjVa. Conversely every family (ξa) defines such an extension, and an endpoint-fixed isomorphism changes it by exactly such a splitting change. Hence YExt⁡1(V,W)≅coker⁡∂, while Hom⁡(V,W)=ker⁡∂ because a morphism is precisely a family of vertex maps commuting with every arrow. Rank–nullity gives dim⁡Hom⁡(V,W)−dim⁡YExt⁡1(V,W)=∑idim⁡Vidim⁡Wi−∑a:i→jdim⁡Vidim⁡Wj. The right side is bilinear in the two dimension vectors.

3.1step 1.2step 2.2algebra

At vertex r, every positive-length path ending at r has a unique first arrow a:i→j followed by a path p:j→r. The relation in step 2.2 reduces (pa)⊗v to p⊗Va(v); induction on path length shows the augmentation is surjective and its kernel is generated by those relations. A linear combination of relations has a unique maximal path length; its terms of that length have distinct first-arrow/path/vector indices, so they cannot cancel unless their coefficients vanish. Descending on path length proves the differential is injective. Hence 0⟶P1(V)⟶P0(V)⟶V⟶0 is a projective resolution of length one.

4.1step 1.2step 3.1F1construct

To see directly that every Yoneda two-extension of V by W is zero, write it as 0→W→E1→E0→V→0. Projectivity of P0(V) gives a lift s:P0(V)→E0 of its augmentation. The composite of P1(V)→P0(V)→sE0 lands in J=ker⁡(E0→V)=im⁡(E1→E0). Projectivity of P1(V) lifts it through E1↠J to t:P1(V)→E1. The resulting map from the split two-extension 0→W→W⊕P1(V)→P0(V)→V→0 to the given extension is the identity on W,V and commutes with all arrows. The split two-extension is zero in Yoneda Ext⁡2, so the given extension is zero.

5.1F2step 1.1step 2.1step 4.1step 1.3step 2.3step 2.4∎

Step 1.1 constructs the small abelian model, step 2.1 verifies Hom and extension finiteness, and step 4.1 proves Yoneda Ext⁡2=0. Steps 1.3, 2.3 and 2.4 give the asserted K0, simple extension dimensions and Euler-form formula. Thus all clauses of [F2] hold for RQ, and Rep⁡k(Q) is essentially small with this finite-field hereditary Hall skeleton.

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

Finite loopless quiver nilpotent representation categories are hereditary and finitary

Statement

Let Q be a finite loopless quiver over Fq. If Q has oriented cycles, take the abelian category of finite-dimensional nilpotent representations; if Q is acyclic, take all finite-dimensional representations. In either case the indicated representation category is essentially small; let AQ be the explicit small skeleton constructed in the proof. This skeleton is a finite-field hereditary Hall category. Its simple objects are Si, K0≅ZQ0 by dimension vector, and dim⁡FqYExt⁡1(Si,Sj)=cij for arrows i→j.

Facts & Assumptions

Given: A finite loopless quiver Q, the finite field k=Fq, and the category of its finite-dimensional nilpotent representations. Nilpotent means that some integer n≥1 kills the composite along every path of length n.

[F1]

The target Hall-category conditions are those of Finite-field hereditary Hall categories and Small finitary abelian categories for Hall multiplication. In particular, heredity here means vanishing of endpoint-fixed Yoneda two-extension classes, rather than a resolution assertion.

[F2]

A two-fold splice is zero if its second short extension is the pushout of an extension by the first middle object (A zero Yoneda splice factors through the middle object).

[F3]

The Grothendieck-group relation is [B]=[A]+[C] for each short exact sequence (Grothendieck group of an essentially small abelian category). Baer addition is the diagonal-pullback/codiagonal-pushout operation of The Baer sum of extension classes and Baer sum makes extension classes an abelian group.

Proof

technique · direct
1.1givenconstruct

Kernels and cokernels of representation maps are formed at each vertex; the induced arrow maps satisfy the abelian identities vertexwise. Subrepresentations and quotients of a representation killed by all paths of length n have the same property. If 0→U→V→W→0 is vertexwise exact and all length-r paths kill U while all length-s paths kill W, then any length-s path sends V into U, and the next r arrows kill it. Thus all length-(r+s) paths kill V. Consequently nilpotent finite-dimensional representations are closed under kernels, cokernels, and extensions, and form an abelian k-linear category. This quantitative bound applies to every extension constructed below.

2.1F1step 1.1construct

Fix an ordering of the finite field and of the finite vertex and arrow sets. For each dimension vector d, use the fixed spaces kdi and list the finitely many arrow-matrix tuples. Keep the nilpotent tuples and the lexicographically least member of each orbit under the finite group ∏iGL⁡di(k). Their union over d∈NQ0, with all commuting families of matrices as morphisms, is the supplied small skeleton AQ. Isomorphisms to representatives may also be chosen as the least in the corresponding finite matrix sets, so transporting kernels, cokernels, and biproducts to it needs no infinite choice. We use this small abelian model when applying [F1]. Hom spaces are subspaces of the finite-dimensional vector space ⨁iHom⁡k(Vi,Wi).

2.2F3step 1.1constructalgebra

For fixed nilpotent V,W, split a short extension vertexwise, using bases in finitely many finite-dimensional vector spaces. Each arrow a:i→j then acts on Wi⊕Vi by the block matrix (Waξa0Va) with ξa:Vi→Wj. Conversely every tuple (ξa) defines a representation extension because a quiver representation has no relations beyond the specified compositions of arrows. It is nilpotent by step 1.1, independently of the tuple. Changing the vertex sections by maps θi:Vi→Wi changes the tuple by d(θ)a=Waθi−θjVa. Every endpoint-fixed isomorphism is exactly such a change of sections. Hence YExt⁡1(V,W) is identified with coker⁡(d:⨁iHom⁡k(Vi,Wi)→⨁a:i→jHom⁡k(Vi,Wj)). Under [F3], Baer sum adds arrow tuples and pushout along λid⁡W multiplies them by λ. This proves that the prescribed extension operations give a finite-dimensional k-space.

2.3F3step 1.1constructalgebra

The vertex representations Si are simple. Every nonzero nilpotent representation has a subobject isomorphic to some Si: among all nonzero images of nonzero vectors under paths choose one of greatest path length, which exists because sufficiently long paths vanish. Its terminal vector is killed by every outgoing arrow, so its one-dimensional span at that vertex and zero at the other vertices is the required subrepresentation. In a simple representation this is the whole object. Total vector-space dimension strictly decreases on a proper quotient, giving a finite composition series with factors among the Si. Counting vertex dimensions along it and using [F3] gives [V]=∑idim⁡k(Vi)[Si]. The dimension-vector map is additive on short exact sequences and sends these classes to the standard basis, so it is inverse to the map ZQ0→K0 taking that basis to [Si].

3.1step 1.1step 2.2construct

Consider an arbitrary two-extension 0→A→B→D→X→0 in the nilpotent category. Its image C⊂D gives short extensions E:0→A→B→pC→0 and F:0→C→D→X→0. Choose a vector-space section of Di→Xi and of pi:Bi→Ci at every vertex. There are finitely many choices, so this does not use the Axiom of Choice. In the resulting coordinates Di=Ci⊕Xi, its arrow maps have form (Caξa0Xa). If sj:Cj→Bj is the chosen section of pj, put ξ~a=sjξa. Define Ti=Bi⊕Xi and Ta=(Baξ~a0Xa). These maps define a finite-dimensional quiver representation and an exact sequence 0→B→T→X→0.

4.1F2step 1.1step 3.1construct

If length-r paths kill B and length-s paths kill X, then length-(r+s) paths kill T by step 1.1. Thus the constructed intermediate object belongs to the nilpotent category, including when Q has oriented cycles. The maps Ti→Di given by (b,x)↦(pib,x) commute with arrows because pjξ~a=ξa and pjBa=Capi. They give a surjection T→D with kernel A, and the pushout of 0→B→T→X→0 along p is precisely F. By [F2] the given two-extension is zero within the nilpotent category itself: the finite zigzag in that lemma involves only finite sums, subquotients, and extensions of these objects, which remain finite-dimensional and nilpotent by step 1.1. Since the original two-extension was arbitrary, all its Yoneda two-extension classes vanish.

5.1F1step 1.1step 2.1step 2.2step 3.1step 4.1step 2.3algebra∎

Apply step 2.2 to V=Si,W=Sj. If i≠j, the source of d is zero, and its target has one scalar coordinate for each arrow i→j. If i=j, that target is zero because Q has no loops. Thus dim⁡kYExt⁡1(Si,Sj)=cij in all cases. Steps 1.1–4.1 verify every condition in [F1], while step 2.3 and this computation prove the remaining assertions for the chosen skeleton. If Q is acyclic then every path has length less than ∣Q0∣, so all finite-dimensional representations are nilpotent; hence the same argument covers the chosen small skeleton of the acyclic category in the statement, consistently with Finite-dimensional representations of an acyclic quiver form a hereditary finitary Hall category.

Source notes

Schiffmann §3.1 explicitly allows cycles, defines nilpotence by uniformly vanishing path composites, proves the simple-object and Grothendieck-group assertions, and states that this nilpotent category is hereditary. The proof above supplies the missing local hereditary argument by lifting arrow coordinates. It neither places infinite-dimensional path projectives in the category nor assumes an ambient-to-Serre-subcategory comparison for Yoneda Ext².

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

The hereditary Euler form is additive on the Grothendieck group

Statement

Let A be a finite-field hereditary Hall category. For objects M,N, define ⟨[M],[N]⟩=dim⁡FqHom⁡(M,N)−dim⁡FqYExt⁡1(M,N). This form is additive in short exact sequences in either variable, so it descends to a well-defined bilinear form on K0(A).

Facts & Assumptions

Given: A finite-field hereditary Hall category and a short exact sequence 0→A→B→C→0.

[F1]

For every pair of objects, Hom and Yoneda Ext⁡1 are finite-dimensional Fq-vector spaces and Yoneda Ext⁡2 vanishes (Finite-field hereditary Hall categories).

[F2]

The covariant and contravariant low-degree Yoneda exact sequences are exact through the Ext⁡2 boundary (Low-degree exact sequences for Yoneda Ext in both variables).

[F3]

K0 imposes [B]=[A]+[C] for every short exact sequence (Grothendieck group of an essentially small abelian category).

Proof

technique · direct
1.1F1F2given

Fix X. The covariant sequence from [F2] ends Hom⁡(X,A)→Hom⁡(X,B)→Hom⁡(X,C)→YExt⁡1(X,A)→YExt⁡1(X,B)→YExt⁡1(X,C)→0, because its next term is YExt⁡2(X,A)=0 by [F1]. It is a finite exact sequence of finite-dimensional vector spaces.

1.2F1F2algebra

Apply the contravariant sequence in [F2]. Its finite exact segment is Hom⁡(C,X)→Hom⁡(B,X)→Hom⁡(A,X)→YExt⁡1(C,X)→YExt⁡1(B,X)→YExt⁡1(A,X)→0. Alternating dimensions give ⟨[B],[X]⟩=⟨[A],[X]⟩+⟨[C],[X]⟩.

2.1step 1.1algebra

The alternating-dimension identity for the finite exact sequence of the previous step gives dim⁡Hom⁡(X,B)−dim⁡YExt⁡1(X,B)=(dim⁡Hom⁡(X,A)−dim⁡YExt⁡1(X,A))+(dim⁡Hom⁡(X,C)−dim⁡YExt⁡1(X,C)). Thus ⟨[X],[B]⟩=⟨[X],[A]⟩+⟨[X],[C]⟩.

3.1F3step 2.1step 1.2algebra∎

The two additivity identities in steps 2.1 and 1.2 respect every defining relation of K0 in [F3]. The universal property of the quotient therefore extends the formula uniquely and additively in both variables to K0(A)×K0(A). All entries are integers, proving the statement.

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

Exact-sequence counts equal endpoint automorphism counts times subobject counts

Statement

Let A be a small finitary abelian category and let M,N,R∈A. Let PM,NR be the number of endpoint-labelled short exact sequences 0→N→R→M→0, and let aX=∣Aut⁡(X)∣. Then PM,NR=aMaNgM,NR, where gM,NR counts subobjects N↪R with quotient isomorphic to M as in The untwisted Hall algebra of a finitary abelian category.

Facts & Assumptions

Given: A finitary abelian category and objects M,N,R.

[F1]

gM,NR counts subobject classes represented by monomorphisms N↪R whose cokernel is isomorphic to M (The untwisted Hall algebra of a finitary abelian category).

[F2]

Hom sets are finite, and a short exact sequence has a monomorphism and epimorphism with the indicated kernel and cokernel (Small finitary abelian categories for Hall multiplication, Exact sequence and short exact sequence in an abelian category).

Proof

technique · direct
1.1F1F2construct

Fix a subobject class counted by [F1], represented by i:N→R. Its quotient is a quotient object isomorphic to M. The number of isomorphisms N→im⁡(i) is aN, and the number of isomorphisms R/im⁡(i)→M is aM. Each pair of isomorphisms determines exactly one endpoint-labelled short exact sequence with this subobject; every such sequence arises from that pair.

2.1step 1.1F1algebra

Distinct subobject classes give disjoint sets of labelled sequences, because the image of the first map recovers the subobject class. Therefore each counted subobject contributes exactly aNaM sequences, and summing over the gM,NR classes proves the formula.

3.1F2step 2.1∎

The total set of labelled sequences is a subset of Hom⁡(N,R)×Hom⁡(R,M) and hence finite by [F2]. The count PM,NR is therefore a well-defined natural number.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The Euler-twisted Hall algebra

Definition

Let A be a finite-field hereditary Hall category over Fq, and choose the positive square root ν=q. For objects M,N, put χ0(M,N)=dim⁡FqHom⁡(M,N)−dim⁡FqYExt⁡1(M,N). This integer depends only on the isomorphism classes of M,N. At this point χ0 is only an object-level exponent; additivity on K0 and the resulting bicharacter are separate proof obligations. The coefficient field is Q(ν). The Euler-twisted Hall algebra is the graded vector space HA,ν=⨁[M]Q(ν)[M],deg⁡[M]=[M]∈K0(A), with bilinear operation [M]⋆[N]=νχ0(M,N)∑[L]gM,NL[L], where The untwisted Hall algebra of a finitary abelian category fixes 0→N→L→M→0. This operation is distinct from the untwisted product: its field, Euler exponent and square-root parameter are additional data. Finite support and associativity are verified in the following items.

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

The Euler-twisted Hall product is well-defined

Statement

For a finite-field hereditary Hall category, the basis formula in The Euler-twisted Hall algebra has finite support and defines a Q(ν)-bilinear operation on the direct-sum Hall space.

Facts & Assumptions

Given: The category, ν=q, and the Euler-twisted basis formula.

[F1]

The untwisted coefficient gM,NL is finite and has finite support in [L] for fixed M,N (Untwisted Hall structure constants and products are finite).

[F2]

The twist scalar νχ0(M,N) is a well-defined element of Q(ν) because χ0(M,N) is an integer (The Euler-twisted Hall algebra).

Proof

1.1F1F2given

For fixed M,N, [F1] gives a finite set of isomorphism classes [L] with nonzero Hall coefficient. Multiplication by the single scalar in [F2] does not enlarge that support, so the displayed basis product is a finite linear combination in the direct sum.

2.1step 1.1algebra∎

Every Hall vector has finite support. Bilinearity therefore expands any product of two vectors into a finite sum of the finite basis products in step 1.1, producing an element of the same direct sum.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The Green Hall completion and coproduct

Definition

Let A be a finite-field hereditary Hall category and use HA,ν and the object-level integer χ0(M,N) from The Euler-twisted Hall algebra. For a basis object R, let PM,NR count endpoint-labelled exact sequences 0→N→R→M→0, and put aR=∣Aut⁡(R)∣. Define the coefficientwise completed tensor space HA,ν⊗^HA,ν=∏([M],[N])Q(ν) ([M]⊗[N]), the space of all coefficient functions on ordered pairs of isomorphism classes. Define the Green coproduct and counit by Δ′([R])=∑[M],[N]νχ0(M,N)PM,NRaR[M]⊗[N],ϵ([R])={1,R≅0,0,R≇0. Each coefficient is finite; the sum need not have finite support. On finite pure tensors define the Euler-twisted tensor multiplication by ([X]⊗[Y])⋅([Z]⊗[W])=νχ0(Y,Z)+χ0(Z,Y)([X]⋆[Z])⊗([Y]⋆[W]). It is extended to completed tensors only when every output coefficient is a finite sum. No algebra structure on the whole completion is asserted; this finite-convergence condition is proved for products of Green images below.

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

The Euler-twisted Hall product is associative and unital

Statement

The operation of The Euler-twisted Hall algebra is a well-defined associative Q(ν)-bilinear product with unit [0].

Facts & Assumptions

Given: A finite-field hereditary Hall category and the twisted product [M]⋆[N]=ν⟨M,N⟩∑LgM,NL[L].

[F1]

The untwisted Hall product is associative with unit [0] (The untwisted Hall product is associative and unital).

[F2]
[F3]

The twisted basis products have finite support (The Euler-twisted Hall product is well-defined).

Proof

technique · direct
1.1givenF2algebra

Fix basis objects M,N,P. Every middle object L in [M]⋆[N] has class [L]=[M]+[N], and every middle object U in [N]⋆[P] has class [U]=[N]+[P], by short exact sequence additivity in K0. Thus the scalar exponent in ([M]⋆[N])⋆[P] is ⟨M,N⟩+⟨M+N,P⟩, while in [M]⋆([N]⋆[P]) it is ⟨N,P⟩+⟨M,N+P⟩.

1.2F1F2algebra

The zero object has class 0 and ⟨0,α⟩=⟨α,0⟩=0. Its twisted products therefore have the same coefficients as the untwisted products in [F1], so [0] is a two-sided unit.

2.1F1F2step 1.1algebra

Bilinearity [F2] makes those exponents equal. After factoring out their common scalar, the remaining coefficient sums are the corresponding untwisted Hall coefficients, which agree by [F1]. Therefore the two parenthesizations agree on basis triples.

3.1F3step 2.1step 1.2algebra∎

Finite support [F3] and bilinearity extend the basis calculation to all vectors in the direct-sum Hall space. Step 1.2 supplies the unit.

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

Green coproduct coefficients are finite

Statement

For fixed objects R,M,N in a finite-field hereditary Hall category, the endpoint-labelled count PM,NR and hence the coefficient of [M]⊗[N] in The Green Hall completion and coproduct are finite. This assertion does not claim finite support in [M],[N] for a fixed R.

Facts & Assumptions

Given: Fixed objects R,M,N in the category.

[F1]

Hom sets are finite in the stated category (Finite-field hereditary Hall categories).

[F2]

The coefficient is the scalar νχ0(M,N)PM,NR/aR (The Green Hall completion and coproduct).

Proof

technique · direct
1.1F1given

An endpoint-labelled sequence 0→N→iR→pM→0 is a pair (i,p) in Hom⁡(N,R)×Hom⁡(R,M) satisfying exactness. This product is finite by [F1], so its exact-sequence subset and the count PM,NR are finite.

2.1F2step 1.1algebra∎

The automorphism number aR is a positive finite integer, and νχ0(M,N) is a defined scalar in Q(ν). Thus the coefficient in [F2] is well-defined. Since the argument fixed M,N, it proves no finite-support claim as those objects vary.

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

The Green cross–square counting identity

Statement

Let A be a finite-field hereditary Hall category. Write aX=∣Aut⁡(X)∣, and let PM,NR count exact sequences 0→N→R→M→0. For fixed objects M,N,K,L, the following cross–square identity holds: ∑[J]PM,NJPK,LJaJ=∑[K1],[K2],[L1],[L2]∣YExt⁡1(K2,L1)∣∣Hom⁡(K2,L1)∣PK2,K1KPL2,L1LPK2,L2MPK1,L1NaK1aK2aL1aL2. Both sums are finite. The left side counts pairs of exact sequences with a common middle object J; the right side counts the compatible four-edge square data, weighted by the displayed Yoneda Ext/Hom ratio.

The diagrams below display the data being counted. A cross is a pair of short exact sequences with the same middle object; it is not an assertion of vertical maps between the endpoint objects.

0NJM00LJK0nb`b0

A square datum is the isomorphism class of these four exact edges: 0→L1→N→K1→0,0→L1→L→L2→0,0→K1→K→K2→0,0→L2→M→K2→0.

0L1NK100L1LL200K1KK200L2MK20

The equal labels indicate shared endpoint isomorphism classes only; no additional morphisms between the two rows are part of the square datum.

Facts & Assumptions

Given: A finite-field hereditary Hall category and four fixed objects M,N,K,L.

[F1]

Hom and Yoneda Ext groups are finite-dimensional Fq-vector spaces, and the short-exact-sequence low-degree Yoneda Ext sequences continue through an Ext⁡2 term that vanishes (Finite-field hereditary Hall categories, Low-degree exact sequences for Yoneda Ext in both variables).

[F2]

The short-exact-sequence and pullback/pushout constructions in an abelian category provide kernels, images, quotients, pullbacks of epimorphisms and pushouts of monomorphisms (Abelian category, Pullback and pushout of an extension).

Proof

technique · direct
1.1F2givenconstruct

For each cross, let L1=N∩L, let L2 be the image of L in J/N=M, let K1 be the image of N in J/L=K, and put K2=J/(N+L). The kernel–image–quotient identities give the four exact sequences in the square datum. Thus an isomorphism of crosses induces an isomorphism of square data and defines a map from cross isomorphism classes to square isomorphism classes.

1.2F2construct

Fix a square datum S. Its four short exact sequences determine X=K×K2M and Y=L⨿L1N. Pullback and pushout exactness give 0→W→X→K2→0, 0→L1→Y→vW→0, and W=K1⊕L2, where W→X is the pair of kernel inclusions and v is induced by the quotient maps N→K1 and L→L2. The order of the two summands is fixed as K1,L2.

2.1step 1.1F2algebra

For a fixed cross, an automorphism ϕ of J stabilizes its two endpoint-labelled sequences exactly when it is the identity on both subobjects N,L and on both quotients J/N,J/L. Then ϕ−1 vanishes on N+L and has image in N∩L=L1, so it factors uniquely as J↠K2→fL1↪J for f∈Hom⁡(K2,L1). Conversely every such f gives a stabilizing automorphism 1+ifπ: since πi=0, its inverse is 1−ifπ. Therefore the stabilizer has cardinality ∣Hom⁡(K2,L1)∣.

2.2step 1.2F2construct

A cross over S is equivalent to an extension 0→Y→J→K2→0 together with a map of this extension to 0→W→X→K2→0 that is v on kernels and the identity on K2. Given this diagram, take the two canonical subobjects N,L→Y→J from the pushout defining Y. Their intersection is L1 and their sum is Y. The composite J→X→M has kernel N: on Y its kernel is v−1(K1⊕0)=N, and on J/Y≅K2 it induces the quotient M↠K2, so there are no additional kernel elements. It is epic because its image contains L2 and surjects onto M/L2≅K2. The same argument with J→X→K shows kernel L and epimorphic quotient. Conversely, from a cross, the quotient maps J→J/L=K and J→J/N=M induce the unique map J→X with the stated restrictions. This identifies the fiber over S.

3.1F2step 2.2construct

Let η∈YExt⁡1(K2,W) be the class of X, and let v∗:YExt⁡1(K2,Y)→YExt⁡1(K2,W) be pushout along v. An extension class ξ has a map to X of the type in step 2.2 exactly when v∗(ξ)=η: pushing out its left endpoint along v produces an extension with endpoints W,K2, and a fixed-end map to X exists precisely when that pushout is equivalent to X. For any one such class and any fixed representative sequence, the set of maps to X is a torsor for Hom⁡(K2,W), because the difference of two maps vanishes on Y and therefore factors uniquely through the quotient J→K2.

3.2step 2.1givenconstruct

The left side of the claimed identity is ∑[J]∣CJ∣/aJ, where CJ is the finite set of pairs of endpoint-labelled exact sequences with middle J. By the orbit–stabilizer formula for Aut⁡(J), it equals the sum over cross isomorphism classes of the reciprocal of their stabilizer size. By step 2.1, each class over a fixed square contributes 1/∣Hom⁡(K2,L1)∣.

4.1F1step 3.1givenalgebra

The exact Yoneda sequence of [F1] for 0→L1→Y→vW→0 is 0→Hom⁡(K2,L1)→Hom⁡(K2,Y)→Hom⁡(K2,W)→YExt⁡1(K2,L1)→YExt⁡1(K2,Y)→v∗YExt⁡1(K2,W)→0. The final zero follows from YExt⁡2(K2,L1)=0. Hence v∗ is surjective, so v∗−1(η) is nonempty and has cardinality ∣v∗−1(η)∣=∣YExt⁡1(K2,L1)∣ ∣Hom⁡(K2,Y)∣∣Hom⁡(K2,W)∣ ∣Hom⁡(K2,L1)∣. This follows by taking cardinalities successively in the finite exact sequence: the kernel of v∗ is the image of YExt⁡1(K2,L1), whose kernel is the image of Hom⁡(K2,W); the first three Hom terms have the displayed orders by exactness.

4.2step 2.1step 3.1givenconstruct

For a fixed Yoneda class ξ with middle object J, all labelled short exact sequences representing ξ form one Aut⁡(J)-orbit. The stabilizer consists of automorphisms 1+ifp with f:K2→Y; its cardinality is ∣Hom⁡(K2,Y)∣, since (ifp)2=0. Hence the orbit has size aJ/∣Hom⁡(K2,Y)∣. By step 3.1 each representative has ∣Hom⁡(K2,W)∣ compatible maps to X. By step 2.1 each cross has stabilizer ∣Hom⁡(K2,L1)∣. Dividing the number of representatives and maps by the cross orbit size, the class ξ contributes ∣Hom⁡(K2,W)∣ ∣Hom⁡(K2,L1)∣∣Hom⁡(K2,Y)∣ cross isomorphism classes over S.

5.1step 4.1step 4.2algebra

Summing the contribution in step 4.2 over all classes in v∗−1(η) and substituting the fiber cardinality in step 4.1 shows that exactly ∣YExt⁡1(K2,L1)∣ cross isomorphism classes lie over S.

6.1step 5.1step 3.2construct

The product PK2,K1KPL2,L1LPK2,L2MPK1,L1N counts labelled square data. The action of Aut⁡(K1)×Aut⁡(K2)×Aut⁡(L1)×Aut⁡(L2) is free: an automorphism fixing the adjacent monomorphism is the identity by monicity, and one fixing the adjacent epimorphism is the identity by epicity. Thus division by the four automorphism numbers gives the number of square isomorphism classes. Each square has ∣YExt⁡1(K2,L1)∣ cross classes by step 5.1, each weighted by 1/∣Hom⁡(K2,L1)∣ by step 3.2. This is exactly the right side of the identity.

7.1F1step 6.1given∎

Both sums are finite. The left sum has finite support in J because YExt⁡1(M,N) is finite. For the right sum, a square datum determines the composites L→L2↪M and N→K1↪K. Their images, kernels and cokernels determine the four corner classes (L1,L2,K1,K2). The finite sets Hom⁡(L,M) and Hom⁡(N,K) therefore allow only finitely many such quadruples. The counted orbit sums are finite, and their equality in step 6.1 is the stated identity.

DefinitionDefinition: Literature-sourcedProof: Not applicableOpen item page →

The extended Hall algebra and composition subalgebra

Definition

Let A be a finite-field hereditary Hall category and let K0=K0(A). Put ([α],[β])=⟨α,β⟩+⟨β,α⟩. The extended Hall algebra is the vector space H~=Q(ν)[K0]⊗HA,ν with basis kα[M] and multiplication (kα[M])(kβ[N])=ν−(β,[M])kα+β([M]⋆[N]). The notation is left-torus normal order: kα[M] is the actual product of the torus and Hall elements. Thus moving kβ past [M] contributes ν−(β,[M]). Equivalently, kαkβ=kα+β and kα[M]kα−1=ν(α,[M])[M]. Associativity follows from the bilinearity of the symmetric Euler form and the associative Hall product; the toral action is checked in The extended Hall torus action is well-defined ↗.

If A has a specified set of simple objects {Si}, the composition subalgebra is the subalgebra of HA,ν generated by [Si]. Its extension by all kα is the extended composition subalgebra.

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

The extended Hall torus action is well-defined

Statement

For each α∈K0, the map on homogeneous Hall elements x↦ν(α,deg⁡x)x is an algebra automorphism. Hence the cross-relations in The extended Hall algebra and composition subalgebra define an associative crossed-product algebra.

Facts & Assumptions

Given: The associative graded Hall algebra and its symmetric Euler form.

[F1]

Every Hall product is homogeneous: deg⁡([M]⋆[N])=[M]+[N], since each middle term is in a short exact sequence with endpoints M,N (The Euler-twisted Hall algebra).

[F2]

The form (α,β) is symmetric and bilinear on K0 (The hereditary Euler form is additive on the Grothendieck group).

[F3]

The Hall product is associative and unital (The Euler-twisted Hall product is associative and unital).

Proof

technique · direct
1.1F1F2algebra

Let x,y be homogeneous of degrees β,γ. By [F1], deg⁡(x⋆y)=β+γ. Thus ν(α,β+γ)(x⋆y)=ν(α,β)+(α,γ)(x⋆y) by [F2], which is the product of the two scaled factors. Therefore the scaling preserves multiplication.

2.1F2F3step 1.1algebra∎

Scaling by ν−(α,deg⁡x) is the inverse map, so the scaling in step 1.1 is an automorphism. Associativity of the crossed product follows from [F3], the action law in step 1.1, and addition in K0: in the declared left-torus normal order, for homogeneous x,y,z of degrees m,n,p, the product is (kαx)(kβy)=ν−(β,m)kα+β(x⋆y). A triple kαx,kβy,kγz contributes exponent −(β,m)−(γ,m+n) in the first parenthesization and −(γ,n)−(β+γ,m) in the second. Bilinearity makes these equal, and [F3] identifies the Hall products. The unit is k0[0], and the conjugation relation follows by the same product formula.

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

The Green Hall coproduct is coassociative

Statement

The Green coproduct Δ′ of The Green Hall completion and coproduct is coassociative in the coefficientwise completion, with counit ϵ as defined there.

Facts & Assumptions

Given: A finite-field hereditary Hall category and an object R.

[F1]

Every coefficient of Δ′([R]) is finite (Green coproduct coefficients are finite).

[F2]

Endpoint-labelled sequence counts satisfy PA,BL=aAaBgA,BL (Exact-sequence counts equal endpoint automorphism counts times subobject counts).

[F3]
[F4]

The Green coproduct and counit coefficients are the formulas in The Green Hall completion and coproduct.

Proof

technique · direct
1.1F1F4given

Fix basis objects A,B,C,R. The coefficient of [A]⊗[B]⊗[C] in (Δ′⊗id)Δ′([R]) is ν⟨A+B,C⟩+⟨A,B⟩aR∑[L]PL,CRPA,BLaL. Only finitely many L occur: each is a middle term of an extension of A by B, and YExt⁡1(A,B) is finite.

2.1F2step 1.1construct

Using [F2], each summand in the flag count becomes aAaBaCgL,CRgA,BL. It counts a flag C⊆U⊆R with U/C≅B and R/U≅A, weighted by the same endpoint automorphism factor aAaBaC.

3.1F1F2step 2.1construct

The coefficient of [A]⊗[B]⊗[C] in (id⊗Δ′)Δ′([R]) is ν⟨A,B+C⟩+⟨B,C⟩aR∑[T]PA,TRPB,CTaT. Again the sum is finite by finiteness of YExt⁡1(B,C). Using [F2], it counts flags C⊆T⊆R with T/C≅B and R/T≅A, with the same weight aAaBaC. The two flag sets described in step 2.1 and in this calculation are identical under U=T.

4.1F3step 1.1step 3.1algebra

By bilinearity [F3], ⟨A+B,C⟩+⟨A,B⟩=⟨A,B+C⟩+⟨B,C⟩. Hence the two coefficients are equal. Every triple coefficient is therefore equal, proving coassociativity in the coefficientwise completion.

5.1F4F1algebra∎

In Δ′([R]), the coefficient of [R]⊗[0] and that of [0]⊗[R] are both one: the exact sequences with zero endpoint are uniquely determined up to the aR endpoint labellings, which cancel the denominator aR. Applying ϵ to either factor therefore returns [R], and all other terms are killed. Linearity proves the two counit identities.

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

Products of Green coproducts converge coefficientwise

Statement

For any M,N, the product Δ′([M])⋅Δ′([N]) in the twisted tensor multiplication of The Green Hall completion and coproduct has a finite coefficient sum at every fixed basis pair [R]⊗[S]. Thus the product is defined in the coefficientwise completion. The claim does not extend to arbitrary pairs of completed tensors.

Facts & Assumptions

Given: Objects M,N,R,S in a finitary abelian category.

[F1]

Every nonzero Hall coefficient is witnessed by a short exact sequence with the stated quotient and subobject, and Hom sets are finite (Small finitary abelian categories for Hall multiplication).

[F2]

A product coefficient can be nonzero only for exact sequences 0→L1→M→K1→0, 0→L2→N→K2→0, 0→K2→R→K1→0, and 0→L2→S→L1→0 (The Green Hall completion and coproduct).

Proof

technique · direct
1.1F1F2construct

Fix S,R. A nonzero contribution to their coefficient determines the four exact sequences in [F2]. Compose S↠L1 with the monomorphism L1↪M; its image is L1 because the first map is epic and the second is monic. Thus the isomorphism class [L1] occurs as the image of a morphism S→M. There are finitely many such morphisms by [F1], hence finitely many possible [L1].

2.1F1F2step 1.1construct

Compose N↠K2 with K2↪R. Its image is K2, and its kernel is L2, so finite Hom⁡(N,R) gives only finitely many possible pairs (K2,L2). The finite set Hom⁡(S,M) similarly gives only finitely many pairs (L1,K1) from the image and cokernel of S↠L1↪M. Hence only finitely many quadruples (K1,L1,K2,L2) contribute.

3.1step 2.1algebra∎

Each quadruple contributes one scalar, finite Hall coefficients and a finite sum by step 2.1. Therefore the coefficient of [R]⊗[S] is a finite sum, for every output pair.

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

Green’s coproduct is an algebra map into the twisted tensor completion

Statement

For a finite-field hereditary Hall category, products of Green images converge coefficientwise and Δ′([M]⋆[N])=Δ′([M])⋅Δ′([N]) in the completion of The Green Hall completion and coproduct, where the target multiplication is the stated Euler-twisted tensor multiplication. The coproduct is coassociative and counital by The Green Hall coproduct is coassociative. It is not asserted that the whole completion is an algebra.

Facts & Assumptions

Given: A finite-field hereditary Hall category and basis objects M,N.

[F1]

The basis formulas for Δ′, the twisted Hall product and twisted tensor multiplication are those of The Green Hall completion and coproduct.

[F2]

Products Δ′([M])⋅Δ′([N]) have finite coefficient sums (Products of Green coproducts converge coefficientwise).

[F3]

The cross–square identity holds for the four external objects (The Green cross–square counting identity).

[F4]
[F5]

Endpoint-labelled exact-sequence counts and Hall numbers satisfy PA,BR=aAaBgA,BR (Exact-sequence counts equal endpoint automorphism counts times subobject counts).

Proof

technique · direct coefficient comparison
1.1F1given

Fix output objects K,L. From [F1], the coefficient of [K]⊗[L] in Δ′([M]⋆[N]) is ν⟨M,N⟩+⟨K,L⟩aMaN∑[J]PM,NJPK,LJaJ. The sum is finite because only middle terms of extensions of M by N occur.

1.2F1F2F5algebra

In Δ′([M])⋅Δ′([N]), denote the decompositions of M by (K2,L2) and those of N by (K1,L1). The Hall products in the two tensor factors contribute PK2,K1K and PL2,L1L. Consequently the coefficient of [K]⊗[L] is 1aMaN∑K1,K2,L1,L2νEPK2,L2MPK1,L1NPK2,K1KPL2,L1LaK1aK2aL1aL2, where E=⟨K2,L2⟩+⟨K1,L1⟩+(L2,K1)+⟨K2,K1⟩+⟨L2,L1⟩. The summation is finite by [F2]. Converting each Hall coefficient to the endpoint-labelled sequence normalization uses [F5].

2.1F4step 1.2algebra

Each nonzero summand in step 1.2 has [M]=[K2]+[L2], [N]=[K1]+[L1], [K]=[K2]+[K1] and [L]=[L2]+[L1]. Expanding the two desired Euler exponents by [F4] gives ⟨M,N⟩+⟨K,L⟩=E+2⟨K2,L1⟩. All terms in the expansion occur once in E except the two displayed copies of ⟨K2,L1⟩.

3.1F3F4step 1.1step 1.2step 2.1algebra

By [F3], the weighted square count in step 1.2 with factor ∣YExt⁡1(K2,L1)∣/∣Hom⁡(K2,L1)∣ equals the cross count in step 1.1. By [F4] and finite-dimensionality, ∣YExt⁡1(K2,L1)∣∣Hom⁡(K2,L1)∣=q−⟨K2,L1⟩=ν−2⟨K2,L1⟩. Thus the exponent E in step 1.2 contributes exactly ν⟨M,N⟩+⟨K,L⟩ times the required Ext/Hom ratio. Substitution of the identity [F3] makes the coefficients in steps 1.1 and 1.2 equal.

4.1F2step 3.1algebra∎

Equality holds at every output basis pair, proving multiplicativity on basis elements. Bilinearity and finite support of Hall products extend it to all finite Hall vectors. Coefficientwise convergence is [F2], and coassociativity and the counit are supplied by the flag proof in The Green Hall coproduct is coassociative.

PropositionStatement: Literature-sourcedProof: AI-adaptedprecheck pendingOpen item page →

The Green Hall pairing is nondegenerate and adjoint to product and coproduct

Statement

On the direct-sum Hall space define ([M],[N])G=δ[M],[N]aM. This bilinear form is nondegenerate over Q(ν) and satisfies ([M]⋆[N],[R])G=([M]⊗[N],Δ′([R]))G⊗G, where the tensor pairing is the product of the two Green pairings.

Facts & Assumptions

Given: A finite-field hereditary Hall category and the Hall basis.

[F1]

aM is a finite positive integer and the Green coproduct has coefficient νχ0(M,N)PM,NR/aR (The Green Hall completion and coproduct).

Proof

technique · evaluate on basis vectors
1.1F1algebra

In the Hall basis, the pairing matrix is diagonal with entries 1/aM. Each is nonzero in Q(ν) by [F1], so the pairing is nondegenerate: if x=∑McM[M] pairs to zero with every [M], then cM/aM=0 for every coefficient, hence every cM=0.

2.1F1F2algebra∎

The left side of the adjointness identity is νχ0(M,N)gM,NR/aR. The right side is νχ0(M,N)PM,NR/(aRaMaN), which is the same scalar by [F2]. Thus the identity holds on basis vectors and extends bilinearly.

CorollaryStatement: Literature-sourcedProof: AI-adaptedprecheck pendingOpen item page →

The extended Green coproduct is an algebra map

Statement

For the extended Hall algebra of The extended Hall algebra and composition subalgebra, define Δ−(kα)=kα⊗kα and, for homogeneous [R], Δ−([R])=∑[M],[N]ν⟨M,N⟩PM,NRaR [M]⊗k−[M][N]. Then Δ− is an algebra map into the coefficientwise completed tensor space of the extended Hall algebra, with ordinary (untwisted) tensor multiplication on the coproduct images, whose coefficient sums converge. The counit is an algebra map to the coefficient field. If every basis coproduct has finite support, these maps define an ordinary tensor-product bialgebra; otherwise their target is the stated completion. This is the DJ-compatible extended Green convention used on this page. The alternative formula Δ+([R])=∑cM,NR[M]k[N]⊗[N] has Δ+([Si])=[Si]⊗1+ki⊗[Si] and is kept separate.

Facts & Assumptions

Given: The twisted Hall coproduct and torus action above.

[F1]

Δ′ is coassociative and counital, and is multiplicative for the Euler-twisted tensor product on convergent products (The Green Hall coproduct is coassociative, Green’s coproduct is an algebra map into the twisted tensor completion).

[F2]

The torus action is kαxkα−1=ν(α,deg⁡x)x (The extended Hall torus action is well-defined).

[F3]

Products of Green images have finite coefficient sums (Products of Green coproducts converge coefficientwise).

Proof

technique · direct bosonization calculation
1.1F1F2construct

For homogeneous x,y,z,w of degrees α,β,γ,δ, define Φ−(x⊗y)=x⊗k−αy. Then Φ−(x⊗y)Φ−(z⊗w)=xz⊗k−αyk−γw=ν(β,γ)xz⊗k−(α+γ)yw. The second equality follows from yk−γ=ν(β,γ)k−γy, obtained by rearranging the torus relation [F2]. The final expression is Φ−((x⊗y)⋅(z⊗w)) for the twisted product in [F1]. Thus Φ− is an algebra map on finite tensors.

1.2F1algebra

On a basis element kα[R], the formula is Δ−(kα[R])=∑M,NcM,NR kα[M]⊗kα−[M][N],cM,NR=ν⟨M,N⟩PM,NR/aR. For a three-step flag with successive quotients A,B,C, both iterates (Δ−⊗id)Δ− and (id⊗Δ−)Δ− have torus factors kα[A]⊗kα−[A][B]⊗kα−[A]−[B][C]. The flag coefficient and Euler exponent agree by coassociativity of Δ′ in [F1]. Hence Δ− is coassociative.

2.1F1F2step 1.1algebra

Define Δ−∣H=Φ−∘Δ′. By [F1] and step 1.1 it is multiplicative on the Hall subalgebra. Put Δ−(kα)=kα⊗kα and extend multiplicatively. For a Green summand [M]⊗k−[M][N], conjugation by kα⊗kα multiplies it by ν(α,[M])+(α,[N])=ν(α,[R]), since [M]+[N]=[R]. Thus the cross-relation defining the extended algebra is preserved, and Δ− is a well-defined algebra map on the extension.

2.2F1step 1.2algebra

Define ϵ(kα[R])=1 if R≅0 and 0 otherwise. In the displayed coproduct, the only terms surviving application of ϵ to the first factor or the second factor are respectively the zero quotient and the zero subobject; each has coefficient one by the endpoint count. Therefore both counit identities hold. The same formula shows ϵ is multiplicative, since a Hall product can have a nonzero coefficient of the zero object only when both endpoint objects are zero: an exact sequence with zero middle object has zero subobject and quotient. This argument does not require the Grothendieck-group grading to detect zero objects.

3.1F3step 2.1step 1.2step 2.2given∎

By [F3], the product of any two Green coproduct images has finite coefficient sums, and the same holds for finite linear combinations of these images. Adjoining torus factors only fixes their group-algebra labels and adds no Hall decompositions. Thus the products needed in steps 2.1–2.2 are defined coefficientwise and those identities hold for coproduct images. No multiplication on arbitrary elements of the coefficientwise completion, or topology on that completion, is asserted. If every basis coproduct has finite support, as for finite-dimensional quiver representations over a finite field, the coproducts lie in the ordinary tensor product and these maps define an ordinary extended bialgebra.

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

The extended Green and repository Drinfeld–Jimbo coproduct conventions agree on simple generators

Statement

For a vertex simple Si, the DJ-compatible extended Green coproduct has Δ−([Si])=[Si]⊗ki−1+1⊗[Si], which is exactly the repository Drinfeld–Jimbo coproduct formula on Ei. The alternative Hall convention Δ+([Si])=[Si]⊗1+ki⊗[Si] is distinct and is not silently identified with Δ−. The positive Borel coproduct formulas are well-defined at ν=q>1.

Facts & Assumptions

Given: A finite loopless quiver, its positive Borel presentation, and the extended Green coproduct of The extended Green coproduct is an algebra map.

[F1]

The repository Drinfeld–Jimbo coproduct is Δ(Ei)=Ei⊗Ki−1+1⊗Ei and Δ(Ki)=Ki⊗Ki (The Drinfeld–Jimbo formulas define a Hopf algebra).

[F2]

The positive Borel coproduct assignments are the same formulas in the presentation of The Hall-normalized extended positive Borel of a loopless quiver.

[F3]

The positive Serre ideal is a coideal for these coproducts in the toral action quotient (The coproduct preserves the positive and negative quantum Serre ideals). Its identities are Laurent-polynomial identities in qi; at qi=ν>1 all quantum factorial denominators are nonzero, so those identities specialize.

[F4]

For a simple Si, the extended coproduct is Δ−([R])=∑ν⟨M,N⟩PM,NRaR−1[M]⊗k−[M][N] (The extended Green coproduct is an algebra map).

Proof

technique · direct comparison of generator formulas
1.1F4givenalgebra

In the sum [F4] for R=Si, the only endpoint pairs are (Si,0) and (0,Si). Each endpoint-labelled exact-sequence count is aSi, and the Euler exponents involving zero are zero. Their terms are respectively [Si]⊗ki−1 and 1⊗[Si].

2.1F1F2F3step 1.1algebra∎

The formula in step 1.1 agrees term by term with [F1] under Ei↦[Si] and Ki↦ki. The group-like torus formulas agree as well. Formula [F2] is well-defined on the positive Serre quotient by [F3] and specialization at ν>1. Schiffmann’s Δ+ has different simple terms, so no equality between those two coproduct conventions is asserted.

PropositionStatement: Literature-sourcedProof: AI-adaptedprecheck pendingOpen item page →

The Ringel assignment is a bialgebra homomorphism onto the extended composition subalgebra

Statement

For a finite loopless quiver Q over Fq, using nilpotent finite-dimensional representations when Q has oriented cycles, the assignment Ei⟼[Si],Ki±1⟼k±ei defines a surjective bialgebra homomorphism from the extended positive Borel of The Hall-normalized extended positive Borel of a loopless quiver onto the extended composition subalgebra of The extended Hall algebra and composition subalgebra. The claim does not include injectivity.

Facts & Assumptions

Given: A finite loopless quiver Q, k=Fq, and ν=q>1.

[F1]

For the selected representation category, the simple objects are Si, K0≅ZQ0, and dim⁡YExt⁡1(Si,Sj)=cij; the Euler values are ⟨Si,Sj⟩=δij−cij and (Si,Sj)=aij. For acyclic Q this is proved in Finite-dimensional representations of an acyclic quiver form a hereditary finitary Hall category. For oriented cycles, the full nilpotent-category hereditary assertion is proved in Finite loopless quiver nilpotent representation categories are hereditary and finitary.

[F2]

Hall products count subobjects in exact sequences 0→N→L→M→0 and the Euler-twisted scalar is ν⟨M,N⟩ (The Euler-twisted Hall algebra).

[F3]

The extended torus acts by kα[M]kα−1=ν(α,[M])[M] (The extended Hall torus action is well-defined).

[F4]

The DJ-compatible extended Green coproduct agrees on simple and torus generators with the Borel coproduct formulas (The extended Green and repository Drinfeld–Jimbo coproduct conventions agree on simple generators, The extended Green coproduct is an algebra map). The extended Hall counit is an algebra map by the latter supplier.

[F5]

The symmetric Gaussian alternating sum vanishes under the stated parity and range conditions (A symmetric Gaussian alternating sum vanishes in the Serre range).

[F7]

The fixed-parameter positive Borel is presented by the torus, Cartan action and quantum Serre relations in The Hall-normalized extended positive Borel of a loopless quiver.

[F6]

Quantum divided powers use x(n)=xn/[n]ν! with nonzero factorials at ν>1 (Quantum integers, factorials, Gaussian binomials and divided powers at qi).

Proof

technique · verify the generator relations by a local flag count
1.1F1F3givenalgebra

The torus generators map to commuting group-like elements with inverse k−ei. By [F3], kei[Sj]k−ei=ν(ei,ej)[Sj]=νaij[Sj], which is the Cartan action relation in the Borel presentation.

1.2F6F7algebra

Fix i≠j, and put r=cij, s=cji, t=r+s=−aij and m=t+1. The ordinary Serre relation in [F7] is equivalent to the divided-power form ∑ℓ=0m(−1)ℓ[Si](ℓ)⋆[Sj]⋆[Si](m−ℓ)=0: multiply this expression by [m]ν!, reindex r=m−ℓ, use (mℓ)ν=(mr)ν, and note that the two sign conventions differ by the common factor (−1)m.

1.3F1F2F6construct

Since there are no loops, every extension of Si by Si splits. For ℓ≥0, the coefficient of [Si⊕ℓ] in the ℓ-fold Hall product counts complete flags in Fqℓ, namely [ℓ]q!, and the iterated Euler twist is νℓ(ℓ−1)/2. The identity [j]q=νj−1[j]ν gives [Si]ℓ=νℓ(ℓ−1)[ℓ]ν![Si⊕ℓ],[Si](ℓ)=νℓ(ℓ−1)[Si⊕ℓ]. The same formula holds for n=m−ℓ.

1.4F1F2construct

Consider a representation M of dimension mei+ej, so Mj is one-dimensional. Define UM=⋂a:i→jker⁡(xa:Mi→Mj),VM=∑b:j→iim⁡(xb:Mj→Mi), and let u=dim⁡UM, w=dim⁡VM. Every composition Mj→xbMi→xaMj is nilpotent and acts on a one-dimensional space, hence is zero. Therefore VM⊆UM. A flag with successive layers Si⊕n,Sj,Si⊕(m−n) is specified by a subspace W⊆Mi of dimension n with VM⊆W⊆UM: the first inclusion makes the intermediate object a subrepresentation, and the second makes the bottom object a subrepresentation. Thus the number of such flags is zero unless VM⊆UM, and otherwise it is #Gr⁡(n−w,u−w)q.

2.1F1F2step 1.3step 1.4algebra

The flag count for the three Hall factors, together with the twist ⟨ℓei,ej⟩=−ℓr, ⟨ℓei+ej,nei⟩=n(ℓ−s) and the two divided-power scalars from step 1.3, shows that the coefficient of [M] in [Si](ℓ)⋆[Sj]⋆[Si](n) is zero unless VM⊆UM, and otherwise equals ν−ns−ℓr+nℓ+ℓ(ℓ−1)+n(n−1)#Gr⁡(n−w,u−w)q. This is obtained by first choosing the bottom subspace W, then using the exact-sequence Hall coefficients for the middle and top quotients; the displayed pairings are the only cross terms between the three graded layers.

3.1F6step 2.1algebra

For a=u−w and b=n−w, counting ordered linearly independent b-tuples and dividing by ∣GL⁡b(Fq)∣ gives #Gr⁡(b,a)q=∏j=0b−1qa−qjqb−qj=νb(a−b)(ab)ν. The second equality follows from the factorial definitions in [F6] and q=ν2. Hence the coefficient in step 2.1 can be written ν−ns−ℓr+nℓ+ℓ(ℓ−1)+n(n−1)+(u−n)(n−w)(u−wn−w)ν.

4.1step 1.2step 3.1algebra

Put ℓ=m−n and d=2s+1−u−w. Expanding the exponent in step 3.1 and using m=r+s+1 gives −ns−ℓr+nℓ+ℓ(ℓ−1)+n(n−1)+(u−n)(n−w)=ms−uw−dn. Thus the coefficient of [M] in the divided Serre sum of step 1.2 is zero if VM⊈UM, and otherwise equals νms−uw(−1)m−wν−dw∑k=0u−w(−1)kν−dk(u−wk)ν. Here k=n−w; Gaussian coefficients outside 0≤n−w≤u−w vanish.

5.1F1F5step 4.1givenalgebra

There are r maps from the m-dimensional Mi to the one-dimensional Mj, so u≥m−r=s+1. There are s reverse-arrow images, each of dimension at most one, so w≤s. Hence u−w≥1 and d−(1−(u−w))=2(s−w)≥0,(u−w−1)−d=2(u−s−1)≥0, while d−(u−w−1)=2(s+1−u) is even. Therefore d satisfies the range and parity hypotheses of [F5] with m there replaced by u−w. The preceding Gaussian sum vanishes. Every degree-(mei+ej) object has zero coefficient, so the divided Serre relation holds in the Hall algebra.

6.1F4F7step 1.1step 5.1algebra

Step 1.1 verifies the torus action, and step 5.1 proves every quantum Serre relation; the Borel presentation [F7] therefore gives an algebra homomorphism with the stated images. By [F4], it intertwines coproducts on generators; since both coproducts are algebra maps, it intertwines them on every product.

7.1F4F7step 6.1algebra∎

On the Borel presentation define ϵB(Ei)=0 and ϵB(Ki±1)=1. These assignments respect the torus relations, the Cartan relations (both sides have value zero) and the Serre relations (every monomial has value zero), so define an algebra map. Both counit identities follow on generators from the coproduct formulas in [F7], and extend to all products because the coproduct and ϵB are algebra maps. For the Hall counit in [F4], the group-like counit identity gives ϵH(k±ei)=1; applying ϵH⊗id to the simple coproduct then gives ϵH([Si])ki−1+[Si]=[Si], hence ϵH([Si])=0. Thus the assignment preserves counits on generators and hence everywhere. Its image is exactly the subalgebra generated by the simple classes and torus, the extended composition subalgebra. This proves the stated surjective bialgebra homomorphism.

Source notes

The cyclic nilpotent hereditary supplier proves vanishing by direct arrow-coordinate lifts inside the finite-dimensional nilpotent category; no infinite-dimensional path projectives are imported.

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

Prime-power specializations of the integral quantum half have a nondegenerate Green form

Statement

Assume the inherited Axiom of Choice of the global-basis suppliers. Let I be a finite symmetric Cartan datum with symmetrizers di=1; its generalized Cartan matrix need not be of finite type. Write A=Z[t,t−1], and let UA− denote the divided-power integral half inside the generic quantum Serre algebra over Q(t). Let Q=pa>1 be a prime power, let ν=Q>1, and set K=Q(ν) and H±=K⊗A,t↦ν±1UA−.

The normalized Kashiwara form Bt specializes to a nondegenerate symmetric form on every finite homogeneous component of both H+ and H−. Their component dimensions are the classical PBW ranks. On H− the primitive-generator coproduct has tensor multiplication (x⊗y)(x′⊗y′)=ν(deg⁡y,deg⁡x′)xx′⊗yy′. The rescaled homogeneous form G(x,y)=(Q−1)−ht⁡αBν−1(x,y) for x,y∈H−[−α], zero in different degrees, has G(Fi,Fj)=δij/(Q−1) and both braided Hopf adjunctions. Thus it has exactly the generator values and symmetric tensor twist of the Green pairing.

This statement concerns the specialization of the integral half. It does not identify that algebra with the algebra presented at the numerical parameter by the quantum Serre relations alone.

Facts & Assumptions

Given: The finite symmetric Cartan datum, Q,ν,K, and the integral half and normalized generic half form Bt.

[F1]

The integral half has, in each finite root degree, a finite A-basis g1,…,gN of bar-fixed lower global elements, and its rank is the classical PBW rank (Integral triangular decomposition and freeness of the Lusztig form, Bar invariance, congruence and uniqueness of the lower global basis).

[F2]

In that basis the Gram matrix of Bt is regular at t=0 and congruent to the identity modulo t (Crystal lattice polarizations are perfect at q=0). All its entries lie in Z[t,t−1,Dm(t)−1:m≥1], where Dm(t)=∏r=1m(1+t2+⋯+t2(r−1)); this is the exact divided-power denominator bound of The negative-half bilinear form is symmetric, nondegenerate and integral(iv).

[F3]

The form is symmetric and homogeneous and satisfies both primitive braided Hopf adjunctions with tensor twist t−(deg⁡y,deg⁡x′) and generator value 1; on words its value is the sum over matching permutations π of t−∑a<b,π(a)>π(b)(αia,αib) (The negative-half bilinear form is symmetric, nondegenerate and integral, proof steps 1.1–2.1; Generic quantum Serre halves have classical PBW ranks and a nondegenerate Hopf pairing).

[F4]

The integral bar fixes divided powers and sends t to t−1 (The bar involution and the contravariant anti-involution preserve UA). Gaussian-binomial coproduct coefficients are Laurent integral (The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality).

Proof

1.1givenalgebra

The minimal polynomial of ν is X−ν∈Z[X] if Q is a square, and X2−Q otherwise. In either case it is monic with constant term of absolute value greater than 1. If an integer polynomial P with P(0)=1 vanished at ν, division by the monic minimal polynomial would express P as its product with an integer polynomial: perform monic polynomial division in Z[X], and the remainder must be zero because it has smaller degree and vanishes at ν. Comparing constant terms would make an integer of absolute value greater than 1 divide 1, a contradiction. Consequently no such P vanishes at ν.

1.2F1F4algebra

Reversal R(Fi1⋯Fin)=Fin⋯Fi1 preserves the generic Serre ideal: reversing a Serre polynomial interchanges its summand indexed by r with the summand indexed by 1−aij−r, multiplying the whole polynomial by (−1)1−aij. It therefore defines an involutive anti-automorphism of the generic half, and preserves UA− since it reverses products of divided powers. Its matrix T(t) in the global basis has entries in A and inverse itself. In particular T(ν) is invertible.

1.3F3F4algebra

The primitive braided coproduct preserves UA−: on a divided power the quantum binomial formula gives r(Fi(n))=∑r+s=nt−rsFi(r)⊗Fi(s), and the divided powers generate the integral half. Thus its coassociativity and counit specialize from the generic identities, as do both form adjunctions of [F3], because their coefficients lie in the localization at nonzero Gaussian factorials. At t=ν−1 the tensor scalar is ν(deg⁡y,deg⁡x′). The specialized algebra remains connected and root graded, so the usual height recursion S(x)=−x−∑S(x′)x′′ for the reduced coproduct gives its antipode: the two convolution recursions give left and right inverses, and associativity makes them equal.

2.1F1F2step 1.1algebra

Fix a root degree and its global basis in [F1]. By [F2], the determinant Δ(t) of its Gram matrix belongs to the indicated localization, is regular at zero and has Δ(0)=1. Clear its finitely many Gaussian-factorial denominators, obtaining Δ(t)=L(t)/D(t) with L∈Z[t,t−1] and D∈Z[t] with D(0)=1. Since Δ is regular at zero, L=ΔD has no negative Laurent powers, so in fact L∈Z[t] and L(0)=1. Each Dm(ν) is a product of positive geometric sums and is nonzero; step 1.1 gives L(ν)≠0. Hence the specialized Gram determinant is nonzero. The specialized global family is a basis because it was an A-basis. Thus Bν is nondegenerate, and its component dimension is the rank in [F1].

3.1F1F2F3step 2.1step 1.2algebra

For α=∑iniαi put cα=((α,α)−∑ini(αi,αi))/2, the integer sum of the pairings over all unordered pairs of letter positions in any word of degree −α. Reversal of the first word complements the inversion set in the matching-permutation formula of [F3]; the color form is symmetric, so Bt−1(u,v)=tcαBt(Ru,v) for equal-degree words. For arbitrary generic elements, coefficient inversion consequently gives Bt(x,y)‾=tcαBt(Rxˉ,yˉ). The global basis is bar fixed by [F1]. Therefore its Gram matrix M satisfies M(t−1)=tcαT(t)TM(t). Evaluating at t=ν and using steps 1.2 and 2.1 proves that M(ν−1) is invertible. Its entries are evaluable since all Gaussian-factorial denominators are positive at ν−1. This proves nondegeneracy on H−, with the same ranks from [F1].

4.1F3step 2.1step 3.1step 1.3algebra∎

On a homogeneous degree −α multiply the form by (Q−1)−ht⁡α. In a nonzero summand of either adjunction the factor degrees add to α, and heights add; hence the scaling factors multiply and both adjunctions remain true. Its simple-generator values are δij/(Q−1) by [F3], and its nondegeneracy follows from step 3.1 since its scaling factors are nonzero. Together with steps 1.1–3.1 this proves every assertion.

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

Finite Serre word forms descend and have classical PBW rank bounds

Statement

Work in ZF. Let I be finite and nonempty and a=(aij) a symmetric generalized Cartan matrix. Also allow I=∅ by taking each half to be the coefficient field and its integral subalgebra to be A. Set A=Z[t,t−1], k=Q(t) and S=k⟨fi:i∈I⟩/(sij:i≠j), where, for m=1−aij, sij=∑r=0m(−1)r(mr)tfim−rfjfir. Identify S with the actual negative Drinfeld–Jimbo half by the choice-free crossed-double lemma, and let UA− be its actual divided-power subalgebra. There exists a unique homogeneous bilinear form Bt with Bt(1,1)=1 and Bt(fix,y)=Bt(x,Diy),Di(fjy)=δijy+t−aijfjDi(y),Di(1)=0. It is symmetric. For ordinary words u=fi1⋯fih and v=fj1⋯fjh its value is Bt(u,v)=∑π: jπ(b)=ibt−∑b<c, π(b)>π(c)aibic, where the sum is over matching permutations. In particular ordinary-word values lie in A, and values on UA− lie in the localization of A obtained by inverting the symmetric quantum factorials.

For any α∈NI, including α=0, enumerate the finite set Wα of ordinary words of that degree, and let Gα(t) be their Gram matrix in the displayed formula. At every real c>0, rank⁡Q(c)Gα(c)≤rank⁡kGα(t)≤dim⁡kS[α]≤pα, where pα is the classical PBW rank: the dimension of the classical Serre enveloping-algebra component. No nondegeneracy or freeness of the divided-power lattice is asserted or used.

Facts & Assumptions

Given: The finite symmetric Cartan matrix, its generic Serre quotient, its actual divided-power subalgebra and the finite ordinary words in each root degree.

[F1]

Quantum factorials are nonzero rational functions; the symmetric Gaussian coefficients are Laurent polynomials, satisfy (mr)t[m−r]t=(mr+1)t[r+1]t, and obey ∑r=0m(−1)r(mr)tt±(m−1)r=0 for m≥1 (Quantum integers, factorials, Gaussian binomials and divided powers at qi, The quantum Pascal recurrences, the Gauss product formula and Gaussian integrality). The cross identity is direct factorial cancellation. The positive-exponent alternating identity is the Gauss product at z=−1; substituting t−1 and using [n]t−1=[n]t gives the negative-exponent identity.

[F2]

The abstract separate Serre half embeds as the actual negative half, without any choice principle (The generic quantum halves form a Drinfeld–Jimbo crossed double). Its divided-power subalgebra consists exactly of finite A-linear combinations of products of fin/[n]t! (The Lusztig divided-power integral form UA).

[F3]

PBW for a supplied ordered finite or countable Lie basis is proved by terminating adjacent-inversion reduction and Jacobi. In a finite-word graded Lie presentation an ordered homogeneous basis can be obtained by retaining the first independent bracket words, without AC (PBW for countably presented Kac Moody Lie algebras). The proof works over Q verbatim: its reductions use only field arithmetic and Jacobi.

[F4]

For the classical complex Kac–Moody algebra, its negative half is the Lie algebra on the negative simple generators with exactly the separate negative Serre relations (Serre presentation of a kac moody algebra). Thus the classical PBW rank here means the same dim⁡CU(n−)[−α] as in the existing generic-rank theorem.

Proof

1.1givenF1constructalgebra

If I=∅, only degree zero occurs; both forms and Gram matrices are (1) and p0=1, so every assertion holds directly. Otherwise supply an order on the finite set I. On the free algebra T=k⟨fi⟩ define Di by the stated recursion. For homogeneous x,y, direct induction on word length gives Di(xy)=Di(x)y+t−(αi,deg⁡x)xDi(y), where (αi,αj)=aij. The recursion also gives Di(fin)=t−(n−1)[n]tfin−1. These are finite sums, and Di lowers height by one.

2.1F1step 1.1algebra

Every Dℓ kills each Serre polynomial already in T. Put a=aij and m=1−a. If ℓ∉{i,j} this is immediate. For ℓ=j, its value is t−amfim∑r(−1)r(mr)ttar=0, since a=−(m−1) and [F1] applies. For ℓ=i, the coefficient of fim−1−rfjfir, 0≤r<m, is (−1)rt−(m−r−1)(mr)t[m−r]t+(−1)r+1t−2(m−r−1)−a−r(mr+1)t[r+1]t=0: the two exponents agree because a=1−m, and the remaining factors agree by [F1]. This calculation includes a=0,m=1.

3.1step 1.1step 2.1algebra

Let J be the two-sided Serre ideal in T. Applying the twisted product rule to a homogeneous contextual relation usijv shows Dℓ(usijv)∈J: differentiating the middle factor gives zero, and differentiating either outside factor leaves the Serre factor. Homogeneous contextual relations span J, so DℓJ⊆J. Thus each Di descends to S, with augmentation ϵ:S→k killing positive height.

4.1step 1.1step 3.1constructalgebra

For a free word u=fi1⋯fih and y∈S define b(u,y)=ϵ(Dih⋯Di1y), where Di1 acts first. Extend linearly in u. This is well-defined in its second argument by step 3.1. Repeated deletion of letters in a representative word v gives exactly the matching-permutation formula in the Statement: the first deletion at position π(1) crosses the preceding remaining letters, and these are precisely the inversion pairs involving the first matched letter; continue inductively. Unequal root degrees give zero.

4.2givenF1step 3.1constructalgebra

Fix α=∑iniαi. The words Wα are a finite ordered list of length N=(∑ini)!/∏ini!. Construct the finite N-row matrix Rα(t) whose columns are all contextual Serre polynomials usijv of degree α, expanded in Wα. This is a finite list: i,j have finitely many possibilities and both context lengths are bounded by ht⁡α. Include all possible context words of the required complementary degrees. The image of this matrix over k is exactly J[α], since every homogeneous ideal element is a finite sum of such contexts. Consequently dim⁡kS[α]=N−rank⁡kRα(t).

5.1step 4.1F2algebra

The bijection π↦π−1 preserves the exponent after interchanging u,v, since a is symmetric. Consequently b(u,[v])=b(v,[u]) for free words and hence for free polynomials. If P∈J, then b(u,[P])=0 for every u; symmetry implies b(P,[u])=0 for every u. Thus b factors in its first argument too, defining the asserted symmetric bilinear form on S. Its definition gives the adjunction and vacuum value. Conversely these adjunctions and homogeneity evaluate any first word by successive deletion, proving uniqueness. Identification [F2] makes this a form on the actual generic half, rather than a form on an unrelated free word space.

5.2F1step 4.2algebra

All entries of Rα(t) lie in A. At t=1, [n]t evaluates to n and each Gaussian coefficient evaluates to the ordinary binomial coefficient, by its polynomial identity or factorial quotient. Hence Rα(1) is exactly the contextual classical Serre matrix. Every nonzero minor of Rα(1) comes from a Laurent-polynomial minor nonzero at 1, and that minor is therefore nonzero over k. Thus rank⁡kRα(t)≥rank⁡QRα(1) and dim⁡kS[α]≤N−rank⁡QRα(1). This is an upper bound; no equality of generic and classical ranks is needed.

6.1F1F2step 5.1algebra

The finite permutation expression has Laurent-polynomial values. Every divided-power product is an ordinary word divided by a finite product of quantum factorials. Bilinearity and [F2] therefore give the asserted localization bound on Bt(UA−,UA−). This uses the actual integral lattice's defining inclusion in the actual half, not a claim that a torsion-free module over A is free.

6.2F3F4step 5.2algebraconstruct

The final rational classical quotient is U(nQ−): define nQ− as the rational Lie algebra on the finite generators fi modulo (ad⁡fi)1−aijfj=0. A linear map from these generators into the commutator Lie algebra of an associative algebra factors through nQ− exactly when its images satisfy the ordinary associative Serre sums, since expanding the iterated commutator gives ∑r(−1)r(mr)fim−rfjfir. Therefore the enveloping algebra and the associative classical Serre quotient have the same universal property, giving mutually inverse generator maps. Enumerate finite homogeneous bracket words, degree by degree, retaining each first independent image to obtain an ordered homogeneous Lie basis. Each root degree has finitely many bracket words and hence finite dimension. PBW [F3] identifies the degree-α component dimension with the number pα of ordered basis monomials of that degree. Extending the finite rational matrix Rα(1) to C preserves its rank: each nonzero rational minor stays nonzero, and each zero minor stays zero. Thus the rational and complex associative quotient dimensions agree. Over C, [F4] identifies the Lie Serre half with the actual classical Kac–Moody negative half; the enveloping universal property just proved identifies its enveloping algebra with the complex associative Serre quotient. Consequently pα is exactly the classical PBW rank of the original target, rather than the rank of a newly chosen different Lie algebra. At α=0 there is one empty word, no contextual relation, G0=(1) and p0=1.

7.1step 5.1step 5.2step 6.2algebra∎

By step 5.1, Gα(t) is the pullback of a bilinear form on the dim⁡kS[α]-dimensional quotient, so its rank is at most that dimension. At c>0 the Laurent entries evaluate. If a specialized minor of Gα(c) is nonzero over Q(c), its Laurent-polynomial minor is nonzero in k. Thus rank⁡Q(c)Gα(c)≤rank⁡kGα(t). Combine this with steps 5.2 and 6.2 to obtain the full chain. All bases and matrix ranks needed here are furnished by finite pivot scans or the explicit bracket-word enumeration. The recursion defines the form in all degrees at once; there is no family of arbitrary choices.

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Green positivity specializes the integral half into the composition algebra

Statement

Let Q=pa>1, ν=Q, and K=Q(ν)⊂R. Let H be the real twisted Hall algebra of the finite-dimensional nilpotent representations of a finite loopless quiver over FQ; an acyclic quiver needs no nilpotence restriction. Write ui=[Si] for its vertex simples and CK for the K-algebra they generate. Let A=Z[t,t−1], and let UA− be the generic divided-power integral half for the symmetric matrix aij=2δij−(number of arrows joining i,j).

There is a surjective graded algebra map Ψ:K⊗A,t↦ν−1UA−⟶CK,Fi⟼ui. It preserves the homogeneous form (Q−1)−ht⁡αBν−1. In particular dim⁡KCK[α] is at most the classical PBW rank. This conclusion requires only positive Green pairing and the generic word-form identity, and does not require specialized nondegeneracy or any numerical Serre-presentation comparison.

Facts & Assumptions

Given: The indicated quiver Hall algebra, its simple classes and composition algebra, the integral half and the specialization parameter.

[F1]

The selected quiver category is a finite-field hereditary Hall category by Finite loopless quiver nilpotent representation categories are hereditary and finitary. Its simple Euler values symmetrize to the displayed Cartan matrix. The Green coproduct in The Green Hall completion and coproduct makes each vertex simple primitive, since it has only the zero subobject and itself. The Green form is ([M],[N])H=δ[M],[N]/∣Aut⁡M∣, so its extension to finite real sums is positive definite. Its homogeneous adjunction is compatible with the primitive braided coproduct on words in vertex simples, with twist ν(α,β), vacuum norm 1 and simple norms 1/(Q−1) (The Green Hall pairing is nondegenerate and adjoint to product and coproduct, Green’s coproduct is an algebra map into the twisted tensor completion). Here the primitive assertion refers to the root-graded braided Hall coproduct, before adjoining the torus.

[F2]

The actual generic symmetric half has the uniquely normalized homogeneous form Bt defined by the matching-permutation formula on ordinary words. Its adjunction is primitive first-letter deletion with tensor twist t−(α,β) and simple norms 1. Ordinary-word values are Laurent polynomials; divided-power products have only finite products of symmetric quantum factorials as denominators. In each degree, the finite ordinary-word Gram matrix Gα(t) satisfies rank⁡Q(c)Gα(c)≤pα at every positive real c, where pα is the classical PBW rank. These assertions, including actual Serre-quotient descent, are proved in Finite Serre word forms descend and have classical PBW rank bounds.

[F3]

The integral half UA− is the actual A-subalgebra of the generic half generated by Fi(n)=Fin/[n]t!. This is its definition in The Lusztig divided-power integral form UA. Quantum factorials have nonzero evaluations at c=ν−1>0; their symmetric quantum-integer factors are positive sums cn−1+cn−3+⋯+c1−n.

Proof

1.1givenF3algebra

Let T be the free A-algebra on Xi,n, i∈I,n≥1, with degree nαi. The map Xi,n↦Fi(n) has image the actual integral half UA−. Define Φ:T→CK by coefficient evaluation t↦c=ν−1 and Xi,n↦uin/[n]c!. The denominator evaluations are nonzero by [F3]. Its image includes every ui, so its K-linear span is CK.

2.1F1F2F3step 1.1algebra

For ordinary words w,z of degree α and height h, the primitive Hall coproduct and Green adjunction evaluate their Hall pairing by deleting successive letters. Deleting a letter at position r crosses the preceding letters that remain in the second tensor factor and contributes ν∑s<rai,js. Each generator pairing contributes 1/(Q−1). Thus repeated deletion gives exactly (w(u),z(u))H=(Q−1)−hBt(w(F),z(F))∣t=c, since c−a=νa. Equivalently both sides have the same first-letter recursion, vacuum value and generator norms after the height rescaling. By dividing by the evaluated factorials and taking finite linear combinations, for homogeneous P,R∈T one obtains (Φ(P),Φ(R))H=(Q−1)−ht⁡αBt(P(F),R(F))∣t=c. Every evaluation is legitimate by the actual form's localization bound in [F2]. Unequal degrees give zero on both sides.

3.1F1F2F3step 1.1step 2.1algebra

If homogeneous P is in the actual kernel of T→UA−, then P(F)=0 as an element of the actual generic half. Since [F2] has constructed a well-defined bilinear form on that actual half, its norm Bt(P(F),P(F)) is the zero rational function. Step 2.1 and positive definiteness of the real Green form imply Φ(P)=0. The kernel is graded, so applying this to its finitely many homogeneous components kills every kernel element. The map Φ consequently factors through an A-algebra map UA−→CK, and extension of scalars gives an algebra map whose image contains K and every ui, hence the surjection Ψ:K⊗A,t↦cUA−→CK asserted in the Statement. The evaluated form on UA− is A-balanced and induces a K-bilinear form on its scalar extension. Step 2.1 passes through the quotient and scalar extension, proving the stated form-preservation assertion, with the factor (Q−1)−ht⁡α.

4.1F1F2step 2.1step 3.1algebra∎

Fix α. The finite set of ordinary words Wα spans CK[α], since CK is generated by the homogeneous simple classes. Let E:KWα→CK[α] be word evaluation. Its pullback Green Gram matrix is (Q−1)−ht⁡αGα(c) by step 2.1. The kernel of this matrix is exactly ker⁡E: one inclusion is immediate; if v is in the matrix kernel then (E(v),E(v))H=0, and positivity in the real Hall space gives E(v)=0. All coefficients lie in the specified real field K=Q(c)=Q(ν). Finite rank-nullity therefore gives dim⁡KCK[α]=rank⁡KGα(c)≤pα. The final inequality is [F2]. This proves the dimension consequence without asserting freeness of UA−[α], nondegeneracy of the generic or specialized form, or injectivity of any numerical Serre-presentation map.

Remarks

The source of Ψ is the actual integral specialization. The numerical Serre-only algebra maps surjectively to this source; proving that additional map injective is a separate obligation. Neither this proof nor the dimension consequence silently identifies those two algebras.

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Reflection classifies finite-Dynkin quiver indecomposables over a finite field

Statement

Assume the Axiom of Choice inherited from finite-root suppliers. Let Q be a finite acyclic quiver and k=Fq. At a sink i define the reflection functor on a representation M by replacing Mi with ker⁡(⨁j→iMj→Mi) and reversing the incident arrows using its kernel projections. At a source use the dual cokernel functor. These are inverse exact equivalences between the full subcategories with no Si direct summand. They commute with field extension.

If the underlying graph is a finite ADE forest, the dimension map gives a bijection from the indecomposable kQ-modules to the positive roots of the componentwise finite root system. Every indecomposable is absolutely indecomposable, has endomorphism ring k and self-Ext⁡1=0. There is an ordering M1,…,Mm of these indecomposables with Hom⁡(Mj,Mi)=0,Ext⁡1(Mi,Mj)=0(i<j). Here representations are finite-dimensional; there are no oriented cycles, so path nilpotence is automatic.

Facts & Assumptions

Given: A finite acyclic quiver and its finite-dimensional representations over k; the classification and ordering assertions additionally assume its graph is a finite ADE forest.

[F1]

Give every ADE edge Coxeter label 3. The proved classification, clauses (1)–(3), in Classification of finite Coxeter systems, including the H and dihedral families and Finiteness criterion: W is finite exactly when the Coxeter form is positive definite give a finite reflection group and positive definite Coxeter form B; its matrix satisfies A=2B, with diagonal 2 and off-diagonal −1 along edges. The orbit Φ=W{αi} of the coordinate basis is therefore a finite reduced crystallographic root system: its reflections preserve the integer lattice and the form A, every orbit vector has squared length 2, the basis spans, and conjugating a simple reflection gives the reflection in its orbit root. Integral coordinates and the integral matrix A give integral root-coroot pairings; the common length excludes proportional roots other than opposites. Its sign coherence and simple-reflection action are proved in Root sign coherence and the action of simple reflections on positive roots, so the coordinate basis is its simple system. This is the finite-root convention of Finite Weyl root system, lattice and chamber conventions and Finite Weyl positive roots and simple reflections. In particular A is nonsingular and every simple reflection preserves positive roots other than its own simple root, which it negates.

[F2]

The category is hereditary and the vertex simples have the usual arrow Euler form (Finite-dimensional representations of an acyclic quiver form a hereditary finitary Hall category).

[F3]

Finite-dimensional modules have unique finite decompositions into indecomposables: apply Graded Krull–Schmidt for finite-dimensional graded modules with the path algebra and module concentrated in degree zero.

Proof

1.1F2givenalgebra

At a sink i, write fM:⨁j→iMj→Mi for the incoming map. A complement to its image is an Si direct summand, because there are no outgoing arrows. Conversely an Si summand makes fM nonsurjective. Thus absence of this summand is exactly surjectivity. After reflection the outgoing map from the new i-space is the kernel inclusion and is injective, the source analogue of this condition. Taking its cokernel recovers Mi and every incoming arrow. Conversely the kernel of the source cokernel recovers the source module. These constructions on morphisms give mutually inverse full equivalences on the specified subcategories.

2.1F2step 1.1algebra

In a short exact sequence whose terms have surjective incoming maps, apply the snake lemma to their incoming-map diagram. The cokernels vanish, so the kernel sequence is exact. Such representations are extension closed: if the outer incoming maps are onto, the middle one is onto by a lift followed by correction from the subobject. The same statements hold dually for injective outgoing maps. Thus the two equivalences are exact for these inherited exact structures and identify the entire Ext⁡1 groups between their objects, since all extension middle terms stay in the subcategory. Tensoring kernels or cokernels with a field extension is exact, proving field-extension compatibility. At a reflected vertex their dimension vector changes by sid, since the new coordinate is ∑j∼idj−di.

3.1F1step 2.1algebra

For the classification assertions now assume finite ADE type. Choose a sink ordering 1,…,r of a connected component, so arrows initially go from higher to lower labels. Reflect each vertex once in this order and repeat; the orientation returns after every full pass, since each edge has been reversed at both endpoints. Let C=sr⋯s1 be its action on dimension columns. If y=Cx, the successive coordinate updates give yi=−xi+∑j<i,j∼iyj+∑j>i,j∼ixj. Put L=I−B− with B− the strict lower adjacency matrix. These equations say Ly=−Ltx, so C=−L−1Lt and 1−C=L−1(L+Lt)=L−1A. The Cartan matrix A is nonsingular by [F1]. Since C lies in the finite Weyl group, some h>0 has Ch=1; then (1−C)∑j=0h−1Cj=0 and consequently ∑j=0h−1Cj=0.

4.1F1F2step 1.1step 2.1step 3.1algebra

Apply this repeated sink process to an indecomposable. Unless it is the simple at the currently reflected sink, step 1.1 preserves it as a nonzero indecomposable and step 2.1 reflects its dimension. If it never became that simple, every Cjd would be a nonnegative nonzero dimension vector. Their sum over one order of C cannot be zero, contradicting step 3.1. Thus it reaches a sink simple at a finite step. Reflecting the dimension backwards proves d is a positive root. The exact equivalences preserve endomorphism rings and self-Ext⁡1; for a sink simple these are k and 0. Repeating over an algebraic closure and using field-extension compatibility shows absolute indecomposability.

5.1F1step 1.1step 3.1step 4.1algebra

Conversely begin with any positive root d and the same repeated sink order. A positive root remains positive under a step unless it is the simple root being reflected, by [F1]. If it never reached that simple root, all its full-pass transforms would stay positive, again contradicting the zero Coxeter sum in step 3.1. Stop just before its first negative transform and put the corresponding sink simple there. Reverse the preceding reflection functors. At every reverse step its root is not the simple at that source, so step 1.1 applies and constructs a nonzero indecomposable of the required dimension. If two indecomposables had this dimension, their deterministic dimension path reaches the same terminal simple at the same first negative step. The inverse equivalences then make them isomorphic. This proves existence and uniqueness for every positive root, including arbitrary finite base fields.

6.1F2F3step 1.1step 2.1step 5.1algebra∎

Order indecomposables by their first stopping time in the repeated sink process. Distinct ones cannot stop at the same time, since the terminal simple and inverse functors would then coincide. If Mi stops before Mj, transport both to just before the earlier stopping time. The former is a sink simple Ss, the latter has onto incoming map and is not Ss. Any map from that latter module to Ss is a functional vanishing on the image of its incoming map, so is zero; and Ext⁡1(Ss,−)=0 because Ss is projective at a sink. The Hom and Ext identifications in steps 1.1 and 2.1 transport these two vanishings back. Distinct connected components have both Hom and Ext zero, so concatenate their orders. The finite enumeration and root constructions use only the inherited Choice; [F3] supplies the direct-sum interpretation.

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Finite-Dynkin Hall algebras are generated by vertex simples

Statement

Let Q be any orientation of a finite ADE forest over k=Fq, with ν=q>1 and coefficient field Q(ν). Its Euler-twisted Hall algebra is generated by the vertex-simple classes. Consequently its composition algebra equals the full positive Hall algebra, and adjoining the declared Cartan torus gives the full extended Hall algebra. No fixed-parameter quantum-group injectivity theorem or Hall polynomial existence theorem is a premise.

Facts & Assumptions

Given: The finite ADE forest, its finite-field representation category, and the subobject-count Hall normalization.

[F1]

Indecomposables M1,…,Mm are indexed by positive roots, with End⁡Mi=k, self-Ext zero and Ext⁡1(Mi,Mj)=0 for i<j (Reflection classifies finite-Dynkin quiver indecomposables over a finite field).

[F2]

Objects decompose uniquely into indecomposables by Graded Krull–Schmidt for finite-dimensional graded modules, applied to the path algebra and modules in degree zero.

[F3]

The Hall coefficient counts subobjects in 0→N→R→M→0, multiplied by νχ0(M,N). By The hereditary Euler form is additive on the Grothendieck group, χ0(M,N)=⟨[M],[N]⟩ is bilinear on K0; for quiver representations the vertex-simple basis identifies these classes with dimension vectors. The composition algebra is the simple-generated subalgebra (The Euler-twisted Hall algebra, The extended Hall algebra and composition subalgebra).

Proof

1.1F1F2F3algebra

By [F1], every extension of Mi⊕a by Mj⊕b for i≤j splits. Hence an ordered Hall product of such blocks is a nonzero scalar multiple of their direct sum: the only possible middle object is the direct sum, and at least its canonical summand inclusion contributes to the positive integer Hall count. Its Euler factor is a nonzero power of ν. This proves that whenever the individual indecomposable classes in a sum have been generated, the class of that sum is generated. In particular [Si⊕a] is a nonzero scalar multiple of [Si]a, since there are no self-extensions at a loopless vertex.

2.1F3step 1.1algebra

Number the vertices topologically, with arrows from earlier to later vertices. For a dimension vector d, the product [d1S1]⋆⋯⋆[drSr] has the same nonzero coefficient on every object of dimension d. Indeed it counts the unique descending filtration whose successive quotients are supported at these vertices: the subobject after each step is the entire representation on the remaining terminal vertex set and zero on the preceding vertices. This is a subrepresentation because arrows never go from a terminal vertex to an earlier one. There are no choices of subspaces within a vertex block. All Euler factors depend only on d, so their product is a common nonzero scalar. There are finitely many objects in the degree, since there are finitely many arrow matrices over k.

3.1F1F2F3step 1.1step 2.1algebra∎

Induct on the total dimension of an indecomposable M. The one-dimensional case is a vertex simple. For larger dimension d, [F1] gives exactly one indecomposable of dimension d. Every other object of that degree is a direct sum of smaller-dimensional indecomposables by [F2]; its class is generated by induction and step 1.1. The simple word in step 2.1 is generated by step 1.1. Subtract all its other degree-d classes and divide by its nonzero coefficient to isolate [M]. This proves generation of every indecomposable, and step 1.1 then proves generation of every object. The composition and extended conclusions are exactly their definitions in [F3]. Across distinct components the cross Euler form, Hom and Ext are zero, so the same argument covers every finite ADE forest, including the empty one.

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Finite-field descent and restriction of Schur quiver representations

Statement

Let Q be a finite quiver, k=Fq, and k‾ an algebraic closure. A finite-dimensional representation M over k‾ is called Schur here when End⁡k‾QM=k‾. Let S be a Frobenius-stable set of Schur geometric isomorphism classes of a fixed dimension vector δ, consisting of representations defined over some finite extensions. Every class fixed by the mth Frobenius power has a model over km=Fqm, unique up to km-isomorphism. If constants c,C>0 satisfy cqm≤∣Fix⁡(Fr⁡m;S)∣≤Cqm for all sufficiently large m, then for all sufficiently large m there are at least c′qm/m pairwise nonisomorphic indecomposable kQ-representations of dimension mδ, for a constant c′>0. This conclusion also holds within the nilpotent representation category when the classes in S are nilpotent.

Facts & Assumptions

Given: The finite fields, Frobenius action, Schur classes and counting bounds in the statement. Assume the inherited Axiom of Choice to choose an algebraic closure and the standard finite-dimensional bases.

[F2]

Distinct field automorphisms are linearly independent as functions (Dedekind's linear independence theorem for distinct characters).

[F3]

Finite-dimensional quiver modules have unique finite indecomposable decompositions by Graded Krull–Schmidt for finite-dimensional graded modules, with path algebra and vector spaces concentrated in degree zero.

Proof

1.1F1F2givenalgebra

Let L/K be a finite cyclic extension with generator σ of order r, and let T be a σ-semilinear automorphism of a finite L-space with Tr=1. Fixed vectors span it over L. Otherwise quotient by their L-span and choose vˉ≠0 there. Every average ∑j=0r−1Tj(av) is fixed, so in the quotient ∑jσj(a)Tjvˉ=0 for all a∈L. A coordinate functional nonzero on vˉ contradicts [F2]. Choose an L-basis among the fixed vectors. A linear combination is fixed exactly when all its coefficients are fixed by σ, so these same vectors are a K-basis of the fixed space. This proves semilinear vector-space descent, and invariant arrow maps descend in these bases.

2.1F1F2step 1.1algebra

Suppose a geometric Schur class is fixed by Fr⁡m. Choose a model and an intertwiner to its transform, all over a finite extension L of K=km; enlarge L if necessary so it is cyclic over K. The intertwiner defines a semilinear operator T on the sum of the vertex spaces, preserving the vertex decomposition and commuting with all arrows. Its rth power is an endomorphism of the Schur representation, so is a common scalar λ. Commuting T with Tr gives σ(λ)=λ, hence λ∈K×. The norm L×→K× is onto: by [F1] it sends a cyclic generator to an element of order ∣K×∣. Choose a with norm λ−1; then (aT)r=1. Step 1.1 supplies fixed bases and a model over K. If two models over K are geometrically isomorphic, their intertwiner space is the kernel of a matrix of linear equations over K, whose dimension stays 1 after scalar extension. A nonzero rational intertwiner is therefore a scalar multiple over k‾ of an isomorphism and is invertible. This proves uniqueness of the rational model.

3.1F1givenstep 2.1algebra

A class fixed by Fr⁡m with orbit length less than m is fixed by Fr⁡d for some proper divisor d of m. For each d, step 2.1 places these fixed classes in bijection with a subset of the isomorphism classes of dimension-δ representations over kd. There are finitely many such representations up to isomorphism: after fixing the finite bases, there are finitely many arrow-matrix tuples over the finite field kd. Thus each fixed set for a small d is finite, and we may increase C to cover the finitely many small extension degrees. The number of classes with orbit length less than m is at most ∑d∣m,d<mCqd≤Cmqm/2. Thus at least cqm−Cmqm/2≥(c/2)qm classes have exact orbit length m for large m, yielding at least (c/2)qm/m distinct Frobenius orbits.

4.1F1F3step 2.1step 3.1algebra∎

For a Schur representative over km with exact orbit length m, restrict every vertex space and arrow to k. Such a representative exists by step 2.1. After scalar extension to k‾, the resulting representation is the direct sum of its m Frobenius conjugates: the algebra km⊗kk‾ is the product of m copies of k‾ under its distinct embeddings, since the finite extension is separable. Each conjugate is indecomposable, because its endomorphism ring is a field, and they are pairwise nonisomorphic by exact orbit length. If the restricted representation split over k, its two nonzero summands would, by [F3], partition this multiset into two nonempty Frobenius-stable subsets. Frobenius acts transitively, so no such partition exists. Hence restriction is indecomposable. Two restrictions from distinct orbits cannot be isomorphic, again by their scalar-extended decompositions and [F3]. Nilpotence of all sufficiently long paths is preserved by restriction. Combining with step 3.1 gives the stated bound.

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Explicit affine D and E flag families give exponentially many indecomposables

Statement

Let Q have underlying graph an affine tree of type D~n (n≥4), E~6, E~7 or E~8, with any orientation, over k=Fq. Let δ be its primitive positive null vector. There are constants c>0,m0 such that for every m≥m0 the category has at least cqm/m pairwise nonisomorphic indecomposable representations of dimension mδ. All its representations are nilpotent, since the underlying graph is a tree. The construction uses only partial flags, finite-field descent and source/sink reflection, not a classification of arbitrary quiver indecomposables.

For D~, δ has value 2 along the central chain and 1 on its four outer leaves. For E~, use the star with arm types (p,q,r)=(3,3,3),(2,4,4),(2,3,6), respectively. The central value is N=3,4,6, and the arm values, from the outside inward, are N/s,2N/s,…,(s−1)N/s for an arm of type s.

Facts & Assumptions

Given: A finite field and an oriented affine D or E tree, with the stated dimension vectors. Assume the inherited Axiom of Choice.

[F1]

A Frobenius-stable family of geometric Schur classes of dimension δ whose mth fixed set has cardinality comparable to qm yields at least cqm/m indecomposables of dimension mδ (Finite-field descent and restriction of Schur quiver representations).

[F2]

The kernel/cokernel reflection construction and inverse exact subcategories clause of Reflection classifies finite-Dynkin quiver indecomposables over a finite field applies to every finite acyclic quiver, not only finite Dynkin type. They preserve endomorphism rings and commute with field extension whenever the object is not the reflected simple.

[F3]

Every two orientations of a finite tree are connected by source/sink firings; clause (1) of Coxeter elements of tree type are conjugate by source and sink firings has this scope without a finite-type hypothesis.

[F4]

Grassmannians have standard affine graph charts and dimension r(n−r); iterating these gives partial-flag charts (Standard affine charts on the Grassmannian, The Grassmannian is smooth, irreducible, and has dimension r(n-r)). The finite general linear group has order ∏j=0N−1(QN−Qj) over FQ: choose its ordered basis columns successively outside the span of the preceding columns.

Proof

1.1F4givenalgebra

For affine D, choose all arrows at the outer leaves pointing toward the central chain and choose any orientation of its edges. Take the chain spaces to have dimension 2 and their maps to be isomorphisms; identify them along the chain. The four nonzero leaf maps then specify four lines in a common 2-space. Isomorphisms of such representations are exactly common GL⁡2 transports of the four lines, and their endomorphisms are exactly linear maps preserving all four lines. Three distinct lines force that endomorphism to be scalar: preserving two lines diagonalizes it and preserving a third with both coordinates nonzero equates the diagonal entries. Such configurations exist over an algebraic closure in every characteristic. Their variety F=(P1)4 is irreducible of dimension 4=22. The stated vector is a null vector: each leaf equation is 2⋅1−2=0, each interior chain equation is 2⋅2−2−2=0, and each end branch has 2⋅2−2−1−1=0; the one-vertex chain has four leaves and the same equality. It is primitive because it has entries 1.

1.2F4algebra

For affine E, orient all arms toward the center and take every arm map injective. Such representations modulo changes of bases on the arms are triples of flags in the central N-space, with steps N/s,…,(s−1)N/s. Endomorphisms are exactly central endomorphisms preserving these flags, since an arm endomorphism is their unique restriction. The product flag variety F is irreducible. The dimension of the flag for s equal blocks of size N/s is ∑i<j(N/s)2=N2(s−1)/(2s) by its successive graph charts. Thus dim⁡F=N2, because 1/p+1/q+1/r=1. Each internal null-vector equation is a second difference of this arithmetic progression; at the center it is 2N−N∑s(s−1)/s=0. The vectors have entries with greatest common divisor 1, proving that they are the primitive positive null vectors.

2.1F4step 1.2algebra

For E6 choose two opposite full flags in dimension 3. Their common endomorphisms are diagonal. Choose the first line of the third full flag to be spanned by (1,1,1) and extend it to any full flag. A diagonal endomorphism preserving this line has equal entries, so the common endomorphism algebra is scalar. For E7 choose two opposite full flags in dimension 4. Choose the third, two-dimensional subspace to be spanned by u=(1,1,1,1) and v=(λ1,λ2,λ3,λ4) with four distinct λi over the algebraic closure. If a diagonal matrix preserves this plane, its diagonal entries are a+bλi, while preservation of v says bλi2+(a−d)λi−c=0 for all four distinct λi. A quadratic polynomial cannot have four distinct roots unless zero, so b=c=0 and d=a. The matrix is scalar. These arguments hold in every characteristic.

3.1F4step 2.1algebra

For E8, choose a full flag in a 6-space grouped into three consecutive pairs, and the opposite partial flag consisting of the last pair and last two pairs. An endomorphism preserving both is block diagonal with three upper triangular 2-by-2 blocks: the full flag makes it upper triangular and the opposite partial flag eliminates the off-block entries. Choose three full flags ℓi⊂Pi in a 3-space whose common endomorphisms are scalar, as in step 2.1. Map this space into ⨁i=13(k3/ℓi) by its three quotient maps; it is injective because the three lines have zero intersection. Identify the first coordinate line in each two-dimensional quotient with Pi/ℓi. Use the image as the remaining three-dimensional subspace in the 6-space. If the three upper triangular blocks preserve this image, they induce a common endomorphism C of k3; the quotient identities force C to preserve every ℓi and Pi. Hence C is scalar by step 2.1, and surjectivity of the quotient maps forces each block to be that same scalar. Thus E8 also has a configuration with scalar endomorphism algebra in every characteristic.

4.1F1F4step 1.1step 1.2step 2.1step 3.1algebra

For each of these product flag varieties F, let Fs be the locus of scalar endomorphism algebra. It is nonempty by steps 1.1, 2.1 and 3.1 and open: preservation of the flags is a finite linear system in the N2 matrix entries; its kernel always contains the scalars, and has dimension 1 exactly when some (N2−1)-minor is nonzero. Every product flag variety has an affine big cell of dimension N2 over k. Its intersection with Fs is nonempty by irreducibility, so on that cell one such minor is a nonzero polynomial over k of fixed degree. A nonzero degree-D polynomial in d variables has at most DQd−1 zeros over FQ, by induction on variables and the one-variable root bound. Therefore ∣Fs(FQ)∣≥c1QN2 for large Q. The full flag counts, or a finite cover by the standard cells [F4], give ∣F(FQ)∣≤c2QN2. Every orbit in Fs(FQ) has cardinality ∣GL⁡N(FQ)∣/(Q−1), because its endomorphisms are exactly the scalars. By [F4] that orbit cardinality is bounded above and below by fixed positive constants times QN2−1. Hence its number of rational orbits is bounded above and below by fixed positive constants times Q.

5.1F1step 4.1algebra

Let S be the geometric Schur classes of the representations just constructed, with the injection/isomorphism conditions on the arrows. These conditions are invariant under Frobenius and base extension. The finite-field descent lemma [F1] shows that Frobenius-fixed classes have rational models; all these rank conditions hold on that model because they hold after scalar extension. Two rational models in one geometric Schur class are rationally isomorphic by the same lemma. After normalizing the chain isomorphisms and forgetting the arm bases, their classes are precisely the rational flag orbits counted in step 4.1. Thus the fixed-class numbers are comparable to qm, and [F1] gives the claimed exponential lower bound for the chosen orientations.

6.1F1F2F3step 1.1step 1.2step 5.1algebra∎

For an arbitrary orientation of the same tree, use a finite sequence of source/sink firings from [F3]. The null-vector equations checked in steps 1.1–1.2 imply siδ=δ at every vertex. A δ-dimensional indecomposable is never a vertex simple. The reflection equivalences [F2] therefore give bijections of Schur classes of dimension δ through the whole firing sequence. They commute with extension and Frobenius and hence preserve all fixed-class counts and exact Frobenius orbit lengths. Apply [F1] again to get the bound in the target orientation. Every path of length at least the number of vertices in a tree orientation is zero, so all constructed representations are nilpotent. This completes the full orientation and category assertions.

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The full Hall algebra is simple-generated exactly in componentwise finite Dynkin type

Statement

Let Q be a finite loopless quiver over k=Fq, using finite-dimensional nilpotent representations when oriented cycles occur, and use the Euler-twisted Hall algebra over Q(q). Its vertex-simple-generated composition subalgebra equals the full Hall algebra if and only if every connected component of the underlying multigraph is a finite ADE Dynkin diagram. Thus adjoining the declared Cartan torus gives the full extended Hall algebra exactly under the same componentwise finite-type condition. The empty quiver is included.

No injectivity theorem for the Ringel map is a premise. The only quantum rank input is the independent surjection from the specialized divided-power integral half onto the composition algebra, which supplies an upper bound by classical PBW ranks.

Facts & Assumptions

Given: The quiver, finite field, nilpotence convention, Hall normalization and composition subalgebra in the statement, with inherited Choice.

[F1]

Hall products have positive nonzero Euler scalars times subobject counts, preserve dimension, and the composition algebra is generated by vertex simples (The Euler-twisted Hall algebra, The extended Hall algebra and composition subalgebra).

[F2]

Finite ADE forests have full Hall algebra generated by their simples (Finite-Dynkin Hall algebras are generated by vertex simples).

[F3]

For every orientation of an affine D or E tree, at least cqm/m indecomposables have dimension mδ, for all large m (Explicit affine D and E flag families give exponentially many indecomposables).

[F4]

The specialized integral divided-power half surjects onto the composition algebra, so each composition degree is at most its classical PBW rank; this surjection uses Green positivity and does not use specialized nondegeneracy or Ringel injectivity (Green positivity specializes the integral half into the composition algebra).

[F5]

For untwisted affine ADE the roots are α+nδ of multiplicity 1 and nonzero nδ of multiplicity the finite rank (Roots of an untwisted affine Lie algebra). PBW counts enveloping monomials in a homogeneous root-space basis (PBW for countably presented Kac Moody Lie algebras).

Proof

1.1F1givenalgebra

Restrict to a full induced subquiver on a vertex subset I. Objects of dimension supported on I have zero vector spaces elsewhere, so their representations, flags, nilpotence and Euler factors are exactly those of the induced subquiver. A word in simples with this degree cannot involve a vertex outside I, since all simple degrees are nonnegative. Thus its Hall and composition homogeneous components agree with those of the subquiver. A proper composition component for an induced subquiver therefore proves properness for Q.

1.2F4F5algebra

On an affine D or E subtree let Hδ be the positive total height of its null vector. There is a constant C bounding the sum of root-space multiplicities at every total height: by [F5] each finite root α contributes at most one integer mode n to a given height ht⁡(α)+nHδ, and imaginary modes contribute at most the finite rank. PBW therefore bounds the total-height generating series of the classical positive enveloping algebra coefficientwise by P(t)=∏h≥1(1−th)−C. For s>0, log⁡P(e−s)=C∑j≥11/[j(esj−1)]≤(C/s)∑j≥1j−2. The series and rearrangements converge absolutely because their terms are positive and e−s<1. A coefficient of height L is at most esLP(e−s); putting s=L−1/2 gives a bound exp⁡(C′L) for a fixed C′. In particular the classical PBW rank in root degree mδ is at most exp⁡(C′′m). By the surjective upper-bound input [F4], the same bound holds for the composition degree.

2.1F1step 1.1algebra

If two vertices have r arrows one way and s the other, with r+s≥2, use degree (1,1). Nilpotence forces at least one of the two scalar-arrow vectors to be zero: a nonzero scalar in each direction would give a nonzero arbitrarily repeatable two-cycle. Conversely either one-direction vector is nilpotent. Changes of vertex bases scale a nonzero vector by a common scalar, so the isomorphism classes are the zero representation and the two projective sets of nonzero vectors. Their number is 1+(qr−1)/(q−1)+(qs−1)/(q−1)>2. The composition degree is spanned by the two simple words. Hence it is proper, with no quantum rank input.

2.2F1step 1.1algebra

Suppose the simple underlying graph contains a chordless cycle of length n≥3. On that induced subquiver use dimension 1 at every vertex. Each proper subset of the n edges specifies a representation by setting those arrows to 1 and the rest to zero. Its support is a forest, so it is nilpotent in every original orientation. The 2n−1 distinct zero/nonzero supports give distinct isomorphism classes. For two nonadjacent vertices an extension of one vertex simple by the other is supported only at those vertices and has no arrow coordinates, so it splits. Their Hom space is zero by disjoint support, their cross Euler values vanish, and the split sum has a unique subobject of either prescribed vertex-simple type. Thus both Hall products are the same direct-sum class, and nonadjacent vertex simples commute. Permutations of the n letters modulo adjacent swaps of nonneighbors correspond to acyclic orientations of the cycle: orient an edge from its earlier letter to its later one. Every acyclic orientation has a topological ordering. Any two such orderings for it are linear extensions of the same partial order; move the first letter of one left in the other, crossing only incomparable letters, and induct to connect them by the allowed swaps. Exactly two of the 2n edge orientations are cyclic. Thus the composition degree has dimension at most 2n−2, less than the Hall degree. This proves properness for every orientation, including the nilpotent oriented-cycle case.

3.1step 1.1step 2.1step 2.2algebra

It remains to classify connected simple trees not of finite ADE type. A vertex of degree at least 4 contains the induced four-leaf star D~4. If there are two vertices of degree 3, choose a closest pair. Their joining path has no branch vertex inside; attach two outward neighbors at each end. The induced subgraph is an affine D tree with two branch vertices and four leaves. If there are no branch vertices, the tree is a path of type A. In the remaining case there is exactly one branch vertex of degree 3, with three arms of lengths p−1≤q−1≤r−1, where 2≤p≤q≤r. The cases (2,2,r) and (2,3,3),(2,3,4),(2,3,5) are precisely finite D and E; if p≥3, truncating arms gives (3,3,3); if p=2,q≥4, it gives (2,4,4); and if p=2,q=3,r≥6, it gives (2,3,6). These are respectively the affine E6,E7,E8 induced subtrees. Thus any remaining non-ADE tree contains an affine D or E induced subtree. An arbitrary graph either has the parallel-edge case, has an induced chordless cycle (take a shortest cycle), or is a forest to which this classification applies.

4.1F3step 1.1step 2.1step 2.2step 3.1step 1.2algebra

The Hall basis contains each of the pairwise nonisomorphic indecomposables from [F3], so its degree mδ has dimension at least cqm/m. For large m this exceeds exp⁡(C′′m), since mlog⁡q−log⁡m−C′′m→+∞. Hence composition is proper on the affine subtree. Steps 1.1 and 3.1, together with steps 2.1–2.2, prove properness whenever any component is not finite ADE. This argument used only the surjection in [F4], not an injection or an equality of quantum and Hall dimensions.

5.1F1F2step 4.1algebra∎

If every component is finite ADE, [F2] gives equality of composition and full Hall. Otherwise step 4.1 gives properness in a supported degree. The torus extension is a direct sum of its declared toral normal-form copies of the positive Hall algebra, so adjoining the torus neither removes nor creates the difference between these positive subspaces. This proves the entire componentwise criterion and its extended version.

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Rank-one skew kernels in a numerical quantum Serre algebra

Statement

Let I be finite, A=(ajk) a symmetric generalized Cartan matrix, and q>0 a real number with q≠1. Let S be the complex associative algebra on generators ej for j∈I, with only the numerical quantum Serre relations ∑s=0N+1(−1)s[N+1s]qejN+1−sekejs=0,j≠k,N=−ajk. Here [r]q=(qr−q−r)/(q−q−1), divided powers are ej(n)=ejn/[n]q!, and S is graded by deg⁡ej=αj. Fix i∈I and write m(β)=∑jaijβj for a root degree β=∑jβjαj.

The operators on words specified by D(ej)=D′(ej)=δij,D(xy)=D(x)y+qm(deg⁡x)xD(y),D′(xy)=qm(deg⁡y)D′(x)y+xD′(y) descend to S, commute, and are locally nilpotent. Set Bi=ker⁡D. Then S=⨁n≥0ei(n)Bi. For homogeneous b∈Bi put R(b)=eib−q−m(deg⁡b)bei,F(b)=−D′(b)q−q−1,K(b)=qm(deg⁡b)b. These define an integrable type-one Uq(sl2) action on Bi, with conventions KRK−1=q2R, KFK−1=q−2F, and RF−FR=(K−K−1)/(q−q−1). The algebra Bi is generated by the finite root strings Rr(ej), j≠i, 0≤r≤−aij. In particular, if 0≠z∈Sβ satisfies D(z)=D′(z)=0, then m(β)≤0.

Facts & Assumptions

Given: Exactly the symmetric numerical Serre presentation in the statement, with q>0 and q≠1. No presentation comparison, pairing nondegeneracy, triangular decomposition, Casimir operator, or ambient quantum-group realization is assumed.

[F1]

The numbers [r]q are nonzero for nonzero integers r, and the symmetric quantum binomials satisfy [r−s]q[rs]q=[s+1]q[rs+1]q and ∑s=0r(−1)s[rs]qzr−s=∏t=0r−1(z−qr−1−2t). The factorial definition gives the first identity and the recurrence [rs]q=q−s[r−1s]q+qr−s[r−1s−1]q. The product on the right satisfies the same recurrence for its signed coefficients: it equals (z−qr−1)q−(r−1)∏t=0r−2(qz−qr−2−2t). Induction from r=0 therefore proves the second identity.

Proof

technique · direct
1.1givenF1constructalgebra

First define D,D′ on the free algebra by the displayed word rules. Write e=ei. Both operators lower the number of letters e in a word by one, so are locally nilpotent there. For each Serre polynomial on letters ej,ek, put r=1−ajk. If i is distinct from j,k, its image under D is zero. If i=j, set a=ajk=1−r. The two terms in D(er−sekes) have respective coefficients qr−s−1[r−s]q and q2(r−s)+a+s−1[s]q on the words with the appropriate one fewer e. On a fixed resulting word er−s−1ekes, the contributions from indices s and s+1 cancel: their common q-power is qr−s−1 and their remaining coefficients cancel by [F1]. If i=k, removing its single letter gives ejr times ∑s(−1)s[rs]qqaij(r−s). Symmetry gives aij=akj=ajk=1−r, so this sum is zero by [F1]. Thus D kills every generating Serre polynomial. Its skew product rule then preserves their two-sided ideal, so it descends to S. Reversing word order interchanges D,D′ and preserves that ideal, since reversal multiplies each Serre polynomial by (−1)r. Hence D′ also descends. The degree-lowering argument proves local nilpotence on S.

2.1step 1.1algebra

The operators commute. To check this without any presentation comparison, induct on word length in the free algebra. For homogeneous words x,y of i-weights mx,my, both DD′(xy) and D′D(xy) expand to qmyDD′(x)y+D(x)D′(y)+qmx+my−2D′(x)D(y)+qmxxDD′(y), using the inductive commutation on x,y. They agree on generators, so agree on all words and on S. In particular D′ preserves Bi. The skew product rule shows that Bi is a graded subalgebra.

3.1step 1.1step 2.1constructalgebra

For homogeneous b∈Bi of i-weight m, D(eb)=b and D(be)=qmb, so R(b)=eb−q−mbe belongs to Bi. For homogeneous b,c∈Bi one has R(bc)=R(b)c+q−mbbR(c). Moreover direct application of the second skew rule gives D′(R(b))=(qm−q−m)b+R(D′(b)), since D′(b) has weight m−2. With F=−D′/(q−q−1), this is RF(b)−FR(b)=[m]qb. The grading gives KRK−1=q2R and KFK−1=q−2F, and K is invertible. Thus these operators satisfy every defining relation of Uq(sl2) on Bi. Their product rules are R(bc)=R(b)c+K−1(b)R(c), F(bc)=F(b)K(c)+bF(c), and K(bc)=K(b)K(c).

4.1givenF1step 3.1algebra

For j≠i put N=−aij. Iterating the definition of R gives Rr(ej)=∑s=0r(−1)sq−s(aij+r−1)[rs]qer−sejes. Indeed the case r=0 is immediate, and passing from r to r+1 uses R(Rrej)=eRrej−q−aij−2r(Rrej)e and the quantum-binomial recurrence. At r=N+1 the extra q-factor is 1, so the numerical Serre relation is exactly RN+1(ej)=0. Since F(ej)=0 and its weight is −N, the commutator in step 3.1 gives by induction F(Rrej)=[r]q[N−r+1]qRr−1ej for r≥1. The needed scalar identity is ∑t=0r−1[m+2t]q=[r]q[m+r−1]q, obtained by summing the defining geometric series. Therefore Vj=span⁡{Rr(ej):0≤r≤N} is a finite-dimensional invariant subspace with weights −N,−N+2,…,N.

5.1step 3.1step 4.1constructalgebra

Let B0 be the subalgebra generated by all these Vj, j≠i. It is contained in Bi and stable under R, by its product rule and the terminating strings of step 4.1. The normal-order identity be=qmeb−qmR(b) for homogeneous b∈B0 shows that ∑n≥0enB0 is stable under right multiplication by e. It is also stable under right multiplication by every ej with j≠i, since these lie in B0. It contains 1, hence every word in the generators and all of S. Thus S=∑n≥0enB0.

6.1F1step 1.1step 5.1algebra

This sum is direct. For b∈Bi, iterating D gives D(enb)=qn−1[n]qen−1b and Dn(enb)=qn(n−1)/2[n]q!b. If ∑n=0denbn=0 with bn∈Bi and bd≠0, application of Dd gives qd(d−1)/2[d]q!bd=0, impossible by [F1]. Consequently the expression in step 5.1 is unique. Applying D to that expression and using the directness just proved shows that an element in ker⁡D has bn=0 for every n>0. Hence Bi=B0, and rescaling en by the nonzero [n]q! gives the asserted divided-power direct sum.

7.1step 3.1step 4.1step 6.1constructalgebra

The action on Bi is integrable. Each Vj in step 4.1 is finite-dimensional with a finite set of integer weights, so its raising and lowering operators are nilpotent. The product formulas of step 3.1 make multiplication Vj1⊗⋯⊗Vjt→Bi equivariant for the coproducts Δ(R)=R⊗1+K−1⊗R, Δ(F)=F⊗K+1⊗F, Δ(K)=K⊗K. These coproduct formulas satisfy the same rank-one relations, as is verified directly using KR=q2RK and KF=q−2FK. Each finite tensor product has only finitely many weights; R increases weight by two and F decreases it by two, so both are nilpotent on it. Every element of Bi=B0 is a finite sum of products of root-string generators, hence lies in a finite sum of such invariant images. Thus R,F are locally nilpotent and K acts with eigenvalues qm, m∈Z. No complete reducibility theorem for rank-one representations is used.

8.1F1step 3.1step 4.1step 7.1algebra∎

Finally let 0≠z∈Sβ satisfy D(z)=D′(z)=0, and put m=m(β). Then z∈Bi and Fz=0. By step 7.1 there is an integer n≥0 with Rnz≠0 and Rn+1z=0. The same commutator induction as in step 4.1 yields FRrz=−[r]q[m+r−1]qRr−1z. At r=n+1 it follows that [n+1]q[m+n]qRnz=0. Both [n+1]q and Rnz are nonzero, so [m+n]q=0. Since q>0 and q≠1, a symmetric quantum integer [r]q vanishes only when r=0. Thus m=−n≤0, as required.

Source notes

This is a direct proof from the stated numerical Serre relations. The source references identify the surrounding classical literature, not a claim that their full relevant proofs have been accessed. In particular Joseph's §4.1.17 is not used as a premise here. The formulas apply directly at q=pf>1.

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The nondegenerate integral specialization has a quantum Casimir

Statement

Let ν=pa>1, K=Q(ν), and choose t∈{ν,ν−1}. Let Ut be the actual specialization at t of the Lusztig integral form for a finite symmetric Cartan datum, extended to a regular realization. Use the source coproduct ΔEi=Ei⊗1+Ki⊗Ei, ΔFi=Fi⊗Ki−1+1⊗Fi at parameter t. Its two halves are the actual integral specializations, without any numerical Serre-only presentation assertion. Write Q=⨁iZαi and put f(λ)=(λ,λ)+2∑ini for λ=∑iniαi∈Q.

On every Q-label-graded Ut-module whose weights lie in a finite union of translates of −Q+, there is a natural operator Ct, commuting with Ut, such that its action on a highest-weight vector of label λ∈Q is tf(λ). Consequently it acts by 1 on each Verma module MUt(−αi) and its subquotients. A nonzero highest-weight vector of label −β in a subquotient of ⨁iMUt(−αi) must satisfy (β,β)=2ht⁡β.

Facts & Assumptions

Given: The symmetric datum with a regular label realization, the actual integral specialization Ut, and a module with the stated bounded-above label support. The inherited Choice hypothesis is that of the integral/global-basis suppliers.

[F1]

The two specialized halves have nondegenerate homogeneous pairings, including at the inverse parameter (Prime-power specializations of the integral quantum half have a nondegenerate Green form). The integral factors are free, with finite homogeneous half components, and have integral triangular decomposition (Integral triangular decomposition and freeness of the Lusztig form).

[F2]

The generic library quasi-R family has degree components in the positive half tensor the negative half, is normalized by Θ0=1, and satisfies Δ(u)Θ=ΘΔˉ(u). Each component is a coevaluation matrix for the generic nondegenerate homogeneous pairing; it is constructed by inverting its finite Gram matrix (Existence and uniqueness of the weightwise quasi-R intertwiner).

[F3]

Integral bar exchanges the two coefficient parameters and fixes divided powers (The bar involution and the contravariant anti-involution preserve UA).

Proof

1.1F1givenalgebra

First the specialization has the usual triangular factors. Since t∈{ν,ν−1}, we have t>0 and t≠1, so every quantum integer factorial and every toral-binomial denominator ∏r=1n(tr−t−r) is nonzero. Hence every specialized divided power and toral binomial is a scalar multiple of a polynomial in the undivided root generators and the group-like torus. Conversely the torus remains precisely its group algebra: for one simple direction the integral toral basis KδT0,r, δ∈{0,1}, is Laurent triangular, since T0,r has powers Kr,Kr−2,…,K−r with nonzero extreme coefficients; ordered by the new extreme powers, this is an invertible triangular change of basis with all coefficients evaluable at t. Tensor the finitely many simple directions and the unchanged lattice-coset representatives. Together with [F1], this proves Ut≅Ut−⊗K[P∨]⊗Ut+ as a vector space. In particular MUt(λ)=Ut−vλ has the expected free half coordinates for every integral label λ. This uses only actual integral specialization.

1.2F2F3algebra

Transport the generic library algebra to the displayed source convention by q↦t−1, Eilib↦Fi, Filib↦Ei, and Khlib↦Kh. The toral actions hold because the root signs and parameter are both inverted. The mixed relation changes sign in both its commutator and its denominator. Symmetric quantum integers are invariant under parameter inversion, so every Serre relation is preserved. The library coproducts become exactly those in the statement. Thus [F2] transports to a generic tensor Θ=∑γΘγ with Θγ∈U−[−γ]⊗U+[γ] and source identity Δ(u)Θ=ΘΔˉ(u), where ΔˉEi=Ei⊗1+Ki−1⊗Ei and ΔˉFi=Fi⊗Ki+1⊗Fi. This transported tensor is normalized by Θ0=1.

2.1F1F2step 1.2algebra

Each transported coefficient is regular at the chosen parameter t: in global bases its construction in [F2] uses inverses of homogeneous Gram matrices, quantum factorials and nonzero generator normalization scalars. By [F1] the Gram matrices at q=t−1∈{ν,ν−1} are invertible, and every other displayed denominator is nonzero. Thus every finite-degree tensor identity of step 1.2 can be evaluated, yielding a well-defined specialized Θ satisfying the same identities on the actual Ut. This is an evaluation of established identities at a separately proved nondegenerate value, not an assumption that a generic nonzero determinant remains nonzero.

3.1step 2.1algebra

Write Θγ=∑aaγ,a⊗bγ,a, in negative and positive degrees respectively, and define Ω=∑γ,aS(aγ,a)bγ,a. On any vector of label λ in the stipulated module this is a finite sum: a nonzero bγ,av requires λ+γ in the bounded-above support, bounding the height of γ. Apply m(S⊗1) to the source Ei intertwining identity from step 2.1. The two terms on its left cancel, because S(Ei)=−Ki−1Ei. The terms on its right are −Ki−1EiΩ+KiΩEi. Hence Ki−1EiΩ=KiΩEi. For Fi, the two left terms cancel because S(Fi)=−FiKi, leaving −FiKiΩKi+ΩFi=0. Toral weight zero gives KhΩ=ΩKh. These computations can first be truncated in root height; all boundary terms contain a positive-degree factor of height tending to infinity acting on v, Eiv or Fiv and vanish for a sufficiently large truncation. Therefore the operator identities are valid on every vector.

4.1step 3.1givenalgebra

For a homogeneous vector v of label λ∈Q, set Ct(v)=tf(λ)Ωv. Since (αi,αi)=2, f(λ)−f(λ−αi)=2(λ,αi). The Ei identity of step 3.1 says EiΩv=t2(λ+αi,αi)ΩEiv, which, with f(λ+αi)−f(λ)=2(λ+αi,αi), gives CtEi=EiCt. The Fi identity says FiΩv=t−2(λ,αi)ΩFiv, giving the other commutation by the first difference formula. The toral identity handles all group-likes. Thus Ct commutes with Ut, is natural for graded module maps and descends to subquotients. If vλ is highest, all positive-height bγ,a kill it, and Θ0=1 gives Ωvλ=vλ. Hence Ct is tf(λ) on its cyclic module.

5.1step 1.1step 4.1algebra∎

For λ=−αi, f(λ)=2−2=0, so Ct=1 on MUt(−αi), its finite direct sum over I, and every graded subquotient. A nonzero highest vector of label −β in such a subquotient also has eigenvalue tf(−β) by step 4.1. Since t>0 and t≠1, equality with 1 implies f(−β)=0, namely (β,β)=2ht⁡β. This proves all claims.

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A minimal numerical Serre kernel obeys the quantum Casimir constraint

Statement

Let ν=pa>1, K=Q(ν), t∈{ν,ν−1}, and let Ut be the actual integral-form specialization from The nondegenerate integral specialization has a quantum Casimir. Let T=K⟨Fi:i∈I⟩ be the free negative tensor algebra, let J=ker⁡(T→Ut−), and let S⊆J be the two-sided numerical quantum Serre ideal at parameter t. If J/S≠0 and β∈Q+ has least height with (J/S)[−β]≠0, then (β,β)=2ht⁡β>0. The quantum Casimir is used only on the already established actual specialization Ut, whose pairing is nondegenerate; it is not assumed to act on the numerical Serre-only algebra.

Facts & Assumptions

Given: The free half T, its map to the actual integral-specialized half Ut−, the ideals J and S at parameter t, and a least-height residual degree −β.

[F1]

The actual specialization Ut has triangular decomposition, MUt(λ)=Ut−vλ, and on every subquotient of ⨁iMUt(−αi) a nonzero highest vector of label −β has (β,β)=2ht⁡β (The nondegenerate integral specialization has a quantum Casimir).

[F2]

The explicit Serre-free crossing calculation and opposite-Serre commutator calculation of The generic quantum halves form a Drinfeld–Jimbo crossed double use only Laurent monomials, quantum Gaussian identities and the denominators q−q−1. In its opposite-generator commutator computation, the opposite commutator of every Serre generator is zero by the identities Cr[N−r]=Cr+1[r+1] and ∑r(−1)rCrq±(N−1)r=0. These identities remain valid at q=t, since t>0, t≠1, and their sole denominator is nonzero. No field PBW dimension assertion is being specialized.

Proof

1.1givenalgebra

Let U~ be the algebra generated by all Ei,Fi,Kh with the toral, toral-action and mixed relations, and no relations within either root half. For every integral label λ, its universal highest module is freely based by Tvλ. To verify this without a presentation freeness assumption, define Fi by left concatenation, Kh on the word of degree −γ by t⟨λ−γ,h⟩, and, for w=Fi1⋯Fin, define Ejwvλ to be the sum over r with ir=j of [⟨λ−∑s>rαis,hj⟩]t times the word with its rth letter deleted. The deletion formula satisfies EiFjw=FjEiw+δij(Ki−Ki−1)w/(t−t−1); its labels verify both toral action relations. There are no further root-half relations to check. Thus these are U~-modules. Conversely the crossing relations move every positive and toral letter to the right in a highest module, so negative words span; the displayed representation makes them independent and proves the universal property. Denote this module by M~(λ).

2.1F1step 1.1algebra

The actual algebra Ut is a quotient of U~: by [F1] its undivided roots and torus generate it and satisfy all the required mixed and toral relations. The canonical module map M~(λ)→MUt(λ) is, on negative coordinates, exactly T→Ut−. Its kernel is consequently Jvλ for every λ, so this subspace is a U~-submodule. At λ=0 the augmentation subspace T+v0 is also a submodule: the deletion formula cannot produce a scalar except from a single letter, whose coefficient is [0]t=0. Each Fiv0 is highest of label −αi. Therefore the maps M~(−αi)→T+v0, v−αi↦Fiv0, are module maps, and their direct sum is an isomorphism because T+=⨁iTFi is the unique last-letter decomposition.

3.1F1step 2.1algebra

Induce that direct sum along U~→Ut. The universal property, or the mutually inverse maps u⊗(avλ)↦uavλ and avλ↦a⊗vλ, gives V:=Ut⊗U~(T+v0)≅⨁iMUt(−αi). Define ℓ:J→V by ℓ(a)=1⊗av0. Since Jv0 is a submodule by step 2.1, its image ℓ(J) is a Ut-submodule of V. For a=∑iuiFi, the direct-sum coordinates of ℓ(a) are (π(ui)v−αi)i. By [F1], this is zero if and only if each ui∈J. Consequently ker⁡ℓ=∑iJFi=JT+; the last equality follows by splitting the last letter of a nonempty right factor and using that J is a two-sided ideal. No flatness of tensor induction was assumed: its kernel is computed directly in the known Verma coordinates.

4.1F1F2step 1.1step 3.1algebra

The subspace Sv0 is a U~-submodule. Multiplication by a negative generator and toral action preserve it. For a positive generator, the specialized opposite-Serre commutator of [F2] vanishes on every Serre generator s. Expanding [Ei,asb]=[Ei,a]sb+as[Ei,b] leaves a Serre factor in each term; moving its toral factors across this homogeneous factor multiplies it only by a scalar. The deletion formula therefore sends Sv0 into itself. It follows that ℓ(S) is a Ut-submodule of V, contained in ℓ(J), and ℓ(J)/ℓ(S) is a submodule of V/ℓ(S). By [F1], the Casimir acts by 1 throughout this quotient.

5.1F1step 2.1step 3.1step 4.1givenalgebra∎

Choose a∈J[−β] with a∉S. Its image ℓ(a)+ℓ(S) is nonzero. Otherwise a−s∈ker⁡ℓ=JT+ for a homogeneous s∈S[−β]; writing a−s=∑iuiFi gives ui∈J[−β+αi] of smaller height, hence ui∈S by minimality. This would give a∈S, a contradiction. Moreover Eiav0 belongs to Jv0 in lower degree by step 2.1, and therefore belongs to Sv0. Thus the nonzero image of a in ℓ(J)/ℓ(S) is highest of label −β. Apply [F1] to the containing subquotient V/ℓ(S): (β,β)=2ht⁡β. Degree zero and every pure simple-root polynomial component survive T→Ut− by the integral rank-one half, so in particular β≠0; its positive height makes the right side strictly positive. This proves the claim.

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

The prime-power numerical Serre half is the integral specialization

Statement

Assume the inherited Choice hypothesis of the integral/global-basis suppliers. Let A=(aij) be a symmetric generalized Cartan matrix on a finite index set; finite, affine and indefinite type are all allowed. Let ν=pa>1, K=Q(ν)⊂R, and ϵ∈{1,−1}. The algebra over K on generators Ei with only the symmetric numerical quantum Serre relations at parameter νϵ is canonically isomorphic, by Ei↦Ei, to the actual Lusztig integral-half specialization K⊗Z[t,t−1],t↦νϵUA+. For both signs, its finite homogeneous components have the classical PBW ranks and the nondegenerate specialized half form. The Green-form assertion is specifically for ϵ=−1: on H−:=K⊗Z[t,t−1],t↦ν−1UA−, relabeling its generators Fi as Ei, the primitive-generator coproduct has tensor multiplication (x⊗y)(x′⊗y′)=ν(deg⁡y,deg⁡x′)xx′⊗yy′, and the rescaled form G(x,y)=(pa−1)−ht⁡αBν−1(x,y) for x,y∈H−[−α], zero in different degrees, has G(Fi,Fj)=δij/(pa−1) and satisfies both Hopf adjunctions.

Facts & Assumptions

Given: The finite symmetric datum, the prime-power parameter, and for each t∈{ν,ν−1} the numerical Serre half at t and actual integral specialization Ht+.

[F1]

The actual integral specialization has nondegenerate homogeneous half forms at ν and ν−1, with classical PBW component ranks and the stated Green normalization at the inverse parameter (Prime-power specializations of the integral quantum half have a nondegenerate Green form).

[F2]

For the kernel of the map from the free negative tensor algebra to the actual half, modulo the numerical Serre ideal, a nonzero least-height residual degree −β satisfies (β,β)=2ht⁡β>0 (A minimal numerical Serre kernel obeys the quantum Casimir constraint). Its quantum Casimir is constructed on the actual nondegenerate integral specialization only (The nondegenerate integral specialization has a quantum Casimir).

[F3]

In the numerical Serre half at any real parameter q>0, q≠1, a nonzero homogeneous element z killed by both i-skew derivatives has ∑jaijdeg⁡jz≤0 (Rank-one skew kernels in a numerical quantum Serre algebra).

[F4]

The negative and positive separate Serre presentations are identical after renaming generators. The two skew derivatives on words can be read from the mixed commutator, and its expression has distinct toral factors (The generic quantum halves form a Drinfeld–Jimbo crossed double). The actual specialized torus and triangular factors are independent by The nondegenerate integral specialization has a quantum Casimir, step 1.1.

Proof

1.1givenF1F2F4assume-contrachoosealgebra

For an empty index set interpret both empty-generator halves as their coefficient ring; the assertion is then the identity map. Otherwise choose a regular Cartan datum without changing the matrix: take P=P∨=Z2I with evaluation pairing, hi=(ei,0), and αj=((aij)i,ej). The simple roots and coroots are independent and their pairings are aij, as required by Symmetrizable Cartan data for quantum groups. The separate generic halves and their divided-power subalgebras depend only on these matrix relations, so this introduces no restriction. There is a canonical surjection π:Sν→Hν+. The actual half satisfies every numerical Serre relation by evaluation of their generic polynomial identities. It is generated by the images of the Ei, since the divided-power generators equal Ein/[n]ν! and the denominators are nonzero. Suppose for contradiction that ker⁡π≠0, and choose a nonzero homogeneous z∈ker⁡π of least positive height, of degree β=∑iniαi. The degree-zero map is injective, so this height is positive. Renaming Ei as Fi identifies this kernel with the residual kernel of [F2]; hence (β,β)=2ht⁡β>0.

2.1F3F4step 1.1algebra

Both skew derivatives of z lie in ker⁡π. Here is a direct justification that requires no numerical presentation comparison. For homogeneous x in the actual positive half, with i-weight m, define the two word deletions Di,Di′ with product rules from [F3]. The source mixed relations give [x,Fi]=(Di′(x)Ki−Ki−1Di(x))/(ν−ν−1); it is true on a simple generator and its extension to a product follows by expanding the commutator and crossing the torus. The deletion formulas also define Di,Di′ on Sν by [F3]. Apply the mixed identity to the word expression z whose image in the actual half is zero. Independence of the toral factors Ki,Ki−1 in [F4], after moving them to one side, forces π(Diz)=π(Di′z)=0. Each derivative lowers height, so minimality of z gives Diz=Di′z=0 in Sν, for every i.

3.1F3step 1.1step 2.1contradiction

Extend scalars from K to C; the nonzero vector stays nonzero because this is a field extension. Apply [F3] for every i to the common-kernel vector of step 2.1. It gives β(hi)=∑jaijnj≤0. Symmetry of the Cartan matrix and its normalization (αi,αj)=aij yield (β,β)=∑iniβ(hi)≤0. This contradicts the strictly positive value in step 1.1. Therefore the assumed kernel vanishes, and the canonical surjection is an isomorphism.

4.1F1F2F3F4step 1.1step 2.1step 3.1algebradischarge-contradiction∎

Now set t=ν−1 and repeat steps 1.1–3.1 with t in place of ν. The same proof applies: t>0, t≠1, the symmetric quantum integers and Serre coefficients are invariant under parameter inversion, [F1] supplies the nondegenerate pairing and PBW ranks at both specializations, [F2] gives the Casimir constraint for Ut, [F3] applies at q=t, and [F4] supplies the specialized toral and triangular factors. Thus the least-height contradiction proves injectivity of the canonical map at t=ν−1 directly. The remaining form and Green-pairing assertions are exactly the inverse-parameter assertions in [F1]; under the generator renaming Fi↔Ei, they have the displayed values and coproduct twist. No semilinear map between coefficient-field fibers is used.

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The Ringel map embeds the extended positive Borel and is full Hall exactly in finite Dynkin type

Statement

Assume the Axiom of Choice inherited from the quantum global-basis suppliers. Let Q be a finite loopless quiver over Fq, using finite-dimensional nilpotent representations when Q has oriented cycles. The assignment Ei↦[Si], Ki↦ki embeds the extended positive Borel for the symmetric Cartan matrix of the underlying graph into the extended Hall algebra, with image the torus extension of the composition subalgebra. Its positive half maps onto the full Hall algebra exactly when the underlying graph is finite Dynkin, meaning that each connected component is a finite ADE Dynkin diagram (including the empty graph).

Facts & Assumptions

Given: The finite loopless quiver, its nilpotent convention, q=pa, ν=q>1, K=Q(ν), and inherited Axiom of Choice.

[F1]

The selected quiver category is a small finite-field hereditary Hall category, with K0=ZQ0 and the vertex-simple Euler values (Finite loopless quiver nilpotent representation categories are hereditary and finitary).

[F2]

The assignment on simples and torus is a well-defined bialgebra homomorphism with extended composition image (The Ringel assignment is a bialgebra homomorphism onto the extended composition subalgebra).

[F3]

The numerical symmetric Serre-only half at ν is canonically the actual divided-power integral specialization at ν−1 after renaming the half generators; its homogeneous Green-normalized form is nondegenerate. The proof supplies numerical skew-kernel integrability and the actual-quotient Casimir argument, rather than specializing a generic determinant (The prime-power numerical Serre half is the integral specialization, Prime-power specializations of the integral quantum half have a nondegenerate Green form).

[F4]

That actual integral specialization surjects isometrically onto the Hall composition algebra, sending its generators to [Si] (Green positivity specializes the integral half into the composition algebra). The target Green form has diagonal values 1/aM (The Green Hall pairing is nondegenerate and adjoint to product and coproduct).

[F5]

The composition algebra equals the full Hall algebra exactly when each graph component is finite ADE, including the empty graph (The full Hall algebra is simple-generated exactly in componentwise finite Dynkin type).

[F6]

The numerical extended positive Borel has the displayed torus action and homogeneous Serre presentation (The Hall-normalized extended positive Borel of a loopless quiver). The extended Hall algebra uses actual left-torus normal order kαx, whose product scalar is ν−(β,deg⁡x) (The extended Hall algebra and composition subalgebra).

Proof

1.1F3F4F6algebra

If the vertex set is empty, the representation category has only its zero object, both presented halves are K, the torus is trivial, and the assignment is the identity; every assertion follows directly. Assume henceforth that the vertex set is nonempty. Let Sν denote the numerical Serre-only positive half in [F6]. By [F3], its generator map to the actual integral-half specialization at the inverse parameter is an isomorphism; the symmetric Serre coefficients are unchanged by ν↔ν−1. Compose with [F4] to obtain the Hall assignment ϕ:Sν→CK. It is surjective and isometric for a nondegenerate source form. If ϕ(x)=0, then for every y in the same homogeneous component its source pairing is (ϕ(x),ϕ(y))G=0, forcing x=0 by [F3]. Separate the finitely many homogeneous components for an arbitrary vector. Thus the positive Hall assignment is injective, with image exactly the composition algebra.

1.2F1F6constructalgebra

The source Borel has the actual normal-form vector space K[ZQ0]⊗KSν. Indeed, homogeneity of the Serre relations makes x↦ν(α,deg⁡x)x an automorphism of Sν for every α; on the displayed vector space define (Kαx)(Kβy)=ν−(β,deg⁡x)Kα+βxy for homogeneous x,y. Bilinearity of the symmetric form makes this product associative: on a triple the exponents are −(β,deg⁡x)−(γ,deg⁡x+deg⁡y) and −(γ,deg⁡y)−(β+γ,deg⁡x), which agree. It satisfies all relations in [F6]. Conversely moving torus letters left in that presentation defines the inverse map; both composites fix every Ei,Ki±1. Thus this is an isomorphism of algebras, proving the source normal form directly.

2.1F1F2F6step 1.1step 1.2algebra

By [F1] and [F6], the target has the matching vector space K[ZQ0]⊗KH, in the same left-torus order. Under these normal forms the map of [F2] is the identity on the torus factor tensor ϕ of step 1.1. Write an element as a finite sum ∑αKαxα. If its image is zero, independence of the distinct target toral basis factors gives ϕ(xα)=0 for every α, and step 1.1 gives xα=0. The source map is therefore injective. Its image and bialgebra compatibility are those in [F2]. Every object in the selected representation category has finitely many subobjects, since its underlying vector spaces are finite sets; hence its coproduct has the ordinary finite-support tensor target. This argument requires no nondegeneracy of a torus pairing.

3.1F5step 1.1step 2.1algebra∎

The full-Hall criterion for the positive half is [F5]. The two normal forms show that adjoining the full torus preserves equality or properness of the positive subspaces. Hence the embedding is onto the full extended Hall algebra exactly in the same componentwise finite ADE cases, including disconnected and empty quivers. The nilpotent convention is retained for every oriented-cycle case.

5 · Examples, counterexamples and false statements

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