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KLR Algebras, Induction, and Quantum-Serre Categorification

1 · Prerequisites

2 · Summary

Objective. This page builds the generic theory of quiver Hecke (KLR) algebras and their categorification of the negative half of a symmetrizable quantum group. It starts from the polynomial presentation of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum and the internal grading of The KLR grading and the diagrammatic multiplication, proves the faithful divided-difference polynomial representation Faithful polynomial representation of a KLR algebra, and deduces the PBW (monomial) basis theorem The PBW (monomial) basis theorem for KLR algebras with finite-dimensional graded components. On that foundation it defines the induction and restriction bimodules Induction and restriction bimodules for KLR algebras, proves exactness, projective preservation and the two adjunctions (left Ind⊣Res, right coinduction as reversed-block induction) together with the Mackey filtration in Generic KLR induction and restriction adjunctions preserve projectives, constructs the nil-Hecke divided-power idempotents and projectives Nil-Hecke idempotents and divided-power KLR projectives, and records the local graded Krull-Schmidt and shift-orbit basis facts Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules and the maximal-tail/unique-head/absolute-simplicity package Maximal KLR tails give a unique induction head and absolute simple modules.

Quantum Serre and the Cartan form. The induction product on the split Grothendieck group satisfies the divided-power quantum Serre relations (The KLR Grothendieck ring satisfies the divided-power quantum Serre relations), so it receives the isomorphism γ from the divided-power form of the negative half. The graded Hom (Cartan) pairing is defined in The KLR Cartan (graded Hom) pairing on the projective Grothendieck group and identified with the Lusztig-normalized half form in The KLR Cartan pairing is the Lusztig-normalized half form; the combined statement is the categorification theorem The KLR category categorifies the negative quantum half, an isomorphism of graded twisted bialgebras with compatible coinvolutions.

Scope and guards. All of the above holds for every field and every graded hermitian KLR parameter satisfying (Q1)-(Q4). The final global-basis identification Self-dual indecomposable KLR projectives give the lower global basis (symmetric type) is stated only for symmetric Cartan data with di=1, characteristic zero and finite loopless quiver parameters Qij=(−1)hij(u−v)hij+hji, with arbitrary arrow multiplicities; it consumes the geometric suppliers on signed-quiver-flag-convolution-and-klr-ext-realization and quiver-full-flag-projective-semisimplicity and the positive first-string supplier Self-dual KLR projectives have positive first-block divided-string leading terms. The companion page klr-algebras-induction-and-quantum-serre-categorification-examples works the small cases, the double-edge braid correction, the degenerate-parameter boundary and the rank-two nil-Hecke projective.

3 · Logical flowchart

4 · Definitions, theorems and proofs

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The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum

Definition

Let (I,A,D,P,P∨,q) be a symmetrizable Cartan datum with no imaginary simple roots, so aii=2, and put bij:=di aij=(αi∣αj), a symmetric matrix with bii=2di>0 (Symmetrizable Cartan data for quantum groups, Kac Moody root lattice height and positive cone). Fix a field k. A KLR datum on it is a family Q=(Qij)i≠j of polynomials Qij∈k[u,v] such that

(Q1) Qij≠0 for i≠j and Qii:=0;

(Q2) Qij(u,v)=Qji(v,u) for all i≠j;

(Q3) Qij is homogeneous of total degree −2bij for the degree assignments deg⁡u:=2di, deg⁡v:=2dj;

(Q4) the two extremal coefficients of Qij, namely that of u−aij and that of v−aji, are nonzero.

For a chosen finite quiver with a compatible automorphism having no arrow within a vertex orbit, write i⋅j=bij and let dij be the number of arrow orbits directed from vertex orbit i to vertex orbit j; the specialization applies when its induced Cartan datum is the fixed one. Then one takes Qij(u,v)=(−1)dij(ul/(i⋅i)−vl/(j⋅j))−2(i⋅j)/l with l=lcm(i⋅i,j⋅j), and Qij=1 when aij=0; the cyclic affine A1(1) double edge aij=aji=−2 is the instance Qij(u,v)=−(u−v)2 up to the fixed normalization of the top coefficients. The simply-laced standard choice is Qij(u,v)=u+v for aij=−1.

The algebra. For n≥0 let In be the set of sequences, let e(ν) for ν∈In be idempotents, and let xa (1≤a≤n) and τa (1≤a≤n−1) be generators. The KLR algebra Rn(Q) is the unital associative k-algebra generated by the e(ν),xa,τa subject to the relations, for all ν∈In (with sa the adjacent transposition acting on positions a,a+1):

(1) e(ν)e(ν′)=δνν′e(ν) and ∑ν∈Ine(ν)=1;

(2) xae(ν)=e(ν)xa and xaxb=xbxa;

(3) τae(ν)=e(saν)τa;

(4) τa2e(ν)=Qνaνa+1(xa,xa+1)e(ν);

(5) τaτb=τbτa whenever ∣a−b∣>1;

(6) (τaxb−xsa(b)τa)e(ν)=0 if b∉{a,a+1} or νa≠νa+1, while if νa=νa+1 one has (τaxa−xa+1τa)e(ν)=e(ν) and (τaxa+1−xaτa)e(ν)=−e(ν) (the sign normalization of the divided difference τa(f)=(f−saf)/(xa−xa+1); Rouquier's printed relation has the opposite global sign, the two conventions being exchanged by τa↦−τa);

(7) (τa+1τaτa+1−τaτa+1τa)e(ν)=0 if νa≠νa+2, and (τa+1τaτa+1−τaτa+1τa)e(ν)=Qνaνa+1(xa,xa+1)−Qνaνa+1(xa+2,xa+1)xa+2−xae(ν) if νa=νa+2, the numerator carrying the sign of the τ-normalization of (6) (Rouquier's printed numerator is its negative); the quotient is a polynomial in xa,xa+1,xa+2 because Qij is a polynomial in its first variable and the numerator vanishes at xa+2=xa (The polynomial ring over a commutative ring as finitely supported coefficient sequences with convolution, Polynomial rings in finitely many commuting indeterminates by iteration).

For β∈Q+ put Iβ:={ν∈I∣β∣:∑aανa=β}, e(β):=∑ν∈Iβe(ν) and R(β):=e(β)R∣β∣(Q)e(β)=⨁ν,η∈Iβe(ν)R∣β∣(Q)e(η), and put R:=⨁β∈Q+R(β). The presentation is the sequence form of Rouquier's Hn(Q) via 1ν=e(ν), xa,ν=xae(ν), τa,ν=τae(ν); no sign or orientation beyond Q is part of the datum, and R(0)=k.

Remarks

Well-definedness. Rn(Q) is defined as the quotient of the free unital associative k-algebra on the symbols e(ν) (ν∈In), xa, τa by the two-sided ideal generated by the displayed relations, so no existence issue arises. Two points deserve record. First, relation (7) is stated as an equality in k[xa,xa+1,xa+2]e(ν): writing Q(u,v)=∑auaqa(v), the difference Q(u,v)−Q(w,v)=∑a(ua−wa)qa(v) is divisible by u−w in the polynomial ring, and its quotient evaluated at (u,w)=(xa,xa+2), v=xa+1 gives the displayed correction; the special case aij=0 with Qij a nonzero constant is included, where the correction vanishes and the ordinary braid relation holds on νa=νa+2. Second, the mixed relations are word-component identities: the final e(ν) is essential, since a global dot commutator has different components on equal and unequal colors. On an equal-color component they are the identities ∂axa−xa+1∂a=1 and ∂axa+1−xa∂a=−1 for ∂a=(1−sa)/(xa−xa+1). The two global sign conventions for τa are exchanged by τa↦−τa, which preserves (4) and flips the signs in (6) and (7); this page fixes the convention of (6) once and for all and every later item uses it.

Choice. The definitional clauses are choice-free: they name a presented algebra and its weight decomposition over a fixed datum, with no selection of representatives or of auxiliary sets.

Sources

Source comparison: Rouquier §3.2.1-3.2.4 (presentation, Cartan specialization, quiver-with-automorphism formula); Khovanov–Lauda I §2.1-2.2 and Khovanov–Lauda II §1-§2 (diagrammatic presentation with the dot counts dij); Kleshchev §2.11 Definition 2.14 (the affine presentation). The printed Rouquier sign in relation (6) is the opposite of the one fixed here; the passage is τa↦−τa as recorded above.

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

The KLR grading and the diagrammatic multiplication

Definition

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum. Assign degrees deg⁡e(ν):=0, deg⁡(xae(ν)):=(ανa∣ανa)=2dνa and deg⁡(τae(ν)):=−(ανa∣ανa+1)=−bνaνa+1 in the presentation; then every relation (1)-(7) is homogeneous (## Verification), so Rn(Q)=⨁m∈ZRn(Q)m is a Z-graded unital associative k-algebra with Rn(Q)m=⨁ν,η∈Ine(ν)Rn(Q)me(η), and each R(β)=⨁mR(β)m is a graded subalgebra (Associative graded algebras, bimodules, and internal shifts). The global sums xa=∑νxae(ν) and τa=∑ντae(ν) need not be homogeneous; displayed generator degrees always refer to their word components. Equivalently, the weight refinement by Q+ is available: the idempotent e(ν) carries weight ∑aανa, and xa and τa are weight-preserving operators of the displayed scalar degrees.

Diagram dictionary. Read a planar diagram bottom to top. A local dot on strand a is xa, a crossing of strands a,a+1 is τa, the identity is the collection of straight diagrams e(ν), and vertical concatenation of diagrams with matching bottom labels ν and top labels sar⋯sa1ν is the algebra product: in ab the diagram for b is placed below the diagram for a, matching operator composition. Isotopies of the plane that do not change the combinatorial type act as the identity, and the local relations (2.3)-(2.8) of Khovanov–Lauda I (quadratic relation, dot-sliding over a crossing, and the braid relation) in the simply-laced Khovanov–Lauda parameter specialization are relations (4), (6) and (7); for general Q the local diagram relations are defined by the full presentation of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum. In particular the degree of a monomial equals the sum of the individual dot degrees plus the signed sum of the crossing degrees, and a dot contributes (ανa∣ανa)=2dνa, while a crossing contributes −bνaνa+1.

All grading shifts on this page are the internal shifts of Associative graded algebras, bimodules, and internal shifts, (M{r})m=Mm−r, and q acts on graded Grothendieck groups by q[P]=[P{1}].

Facts & Assumptions

Given: A KLR datum Q and the presented algebra Rn(Q) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum with its relations (1)-(7), together with the degree assignment deg⁡e(ν)=0, deg⁡xa=2dνa, deg⁡τa=−bνaνa+1 and the symmetric matrix bij=diaij with bii=2di>0 of Kac Moody root lattice height and positive cone.

[F1]

The relation list of the KLR algebra: relations (1)-(7) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum, including the symmetry bij=bji and bii=2di.

[F2]

The parameter conditions (Q1)-(Q4) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum, in particular (Q3): Qij is homogeneous of total degree −2bij for deg⁡u=2di, deg⁡v=2dj.

Verification

technique · direct; check homogeneity of each defining relation for the displayed degree assignment and then transfer it to the quotient
1.1givenF1algebra

Relation (1) has degree 0 on both sides, and in (2) the identity xae(ν)=e(ν)xa has degree 2dνa while xaxb=xbxa has degree 2dνa+2dνb on the ν-component; relation (3) has degree −bνaνa+1=−bνa+1νa on both sides by the symmetry of b from [F1].

2.1step 1.1F1F2algebra

Relation (4) is homogeneous of degree −2bνaνa+1: the left side τa2e(ν) has degree 2(−bνaνa+1), and the right side Qνaνa+1(xa,xa+1)e(ν) has degree −2bνaνa+1 by [F2], since a monomial urvs of Qij contributes r(2di)+s(2dj).

2.2step 1.1F1algebra

Relations (5) and (6) are homogeneous with their actual label-dependent degrees. In far crossing commutation, both products have degree −bνaνa+1−bνbνb+1 because the disjoint crossings interchange the same two color pairs. A far dot move has degree 2dνb−bνaνa+1 on both sides, as its untouched strand keeps the dot color. For adjacent unequal colors, dot sliding likewise preserves the degree of the crossing plus the transported dot. For equal colors i, the dot degree is 2di and the crossing degree is −2di, so both terms of τaxa−xa+1τa=e(ν) and τaxa+1−xaτa=−e(ν) have degree 0, equal to the degree of the idempotent on the right. Thus every dot and far-crossing relation is homogeneous, without asserting that its common degree is always zero.

3.1step 2.2F1F2algebra

Relation (7), unequal outer colours: for colours (νa,νa+1,νa+2)=(a′,b′,c′) both braid words are sums of terms each moving the same three crossings over the same three pairs, so each has degree −ba′b′−ba′c′−bb′c′, and the right side is 0; on the equal-outer-colour case (i,j,i) each braid word has the same degree −2bij−2di, while the correction numerator has degree −2bij and its division by xa+2−xa, of degree 2di, lowers the degree to −2bij−2di; for three equal colours Qii=0 and the ordinary nil-Hecke braid relation is homogeneous of degree −6di.

4.1step 1.1step 2.1step 2.2step 3.1algebra∎

Use the free path algebra with vertices ν, loops xae(ν) and arrows τae(ν):ν→saν, assigned the displayed degrees. Its vertex sum is the unit because I is finite; decomposing the global generators by word idempotents identifies its presented quotient with Rn(Q). Every defining component relation is homogeneous, so the two-sided ideal they generate is graded, and the quotient Rn(Q) inherits a Z-grading with Rn(Q)m=⨁ν,ηe(ν)Rn(Q)me(η); the weight refinement is inherited because each generator preserves the weight ∑aανa and each relation is weight-homogeneous, and R(β)=e(β)R∣β∣(Q)e(β) is a graded subalgebra for every β∈Q+.

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Faithful polynomial representation of a KLR algebra

Statement

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum. Choose a factorization Qij(u,v)=Pij(u,v)Pji(v,u) with Pij∈k[u,v] nonzero for all i≠j; with (Q1) one may order the pairs and take Pij=Qij, Pji=1. On the graded space Poln:=⨁ν∈Ink[x1,…,xn]e(ν) define operators: e(ν) projects to the ν-summand; xa multiplies by xa; for νa≠νa+1 set τa(fe(ν)):=Pνaνa+1(xa+1,xa) sa(f) e(saν) where sa permutes the variables; for νa=νa+1 set τa(fe(ν)):=f−sa(f)xa−xa+1e(ν), the divided difference operator of the sign convention fixed in relation (6) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum (the quotient lies in k[x1,…,xn] because f−saf vanishes at xa=xa+1; the variable permutation of Polynomial rings in finitely many commuting indeterminates by iteration makes this precise). Give Poln the grading of The KLR grading and the diagrammatic multiplication with deg⁡xae(ν):=2dνa, together with the summand shifts that make each τae(ν) homogeneous of degree −bνaνa+1 (they exist by the antisymmetry of the increments −bij−deg⁡Pij and are unique up to one constant on each fixed-weight sequence orbit). Then each word-component generator acts homogeneously of its degree, the operators satisfy relations (1)-(7), and they define a homomorphism of graded algebras ρ:Rn(Q)→Endkgr(Poln), the graded algebra of homogeneous endomorphisms, with ρ(Rn(Q)m) Poln,d⊆Poln,d+m. For nonzero Pij this homomorphism is injective. After localizing at the nonzero polynomials Pij(xa,xb) (νa≠νb) and the differences xa−xb (νa=νb), it becomes an isomorphism onto the localization of the skew group algebra An(I)=(⨁ν∈Ink[x1,…,xn]e(ν))⋊Sn; consequently Rn(Q) has finite-dimensional homogeneous components and ρ is a faithful representation.

Facts & Assumptions

Given: A KLR datum Q of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum with bij=diaij=bji and bii=2di>0, a factorization Qij(u,v)=Pij(u,v)Pji(v,u) with all Pij≠0, and the space Poln=⨁ν∈Ink[x1,…,xn]e(ν) with the degree assignment deg⁡xa=2dνa and idempotents of degree~0.

[F1]

(Q3) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum: Qij is homogeneous of total degree −2bij for deg⁡u=2di, deg⁡v=2dj.

[F2]

Homogeneity of factors: for the positive weighting [i,j] with deg⁡u=2di, deg⁡v=2dj, the least and greatest weighted degrees of a product of nonzero polynomials are the sums of those of its factors, since the polynomial ring over k is a domain. Thus (Q3) and Qij=Pij(u,v)Pji(v,u) force both factors to be homogeneous, with deg⁡[i,j]Pij+deg⁡[j,i]Pji=−2bij. No homogeneity for the swapped weighting is asserted.

[F3]

Relation list (1)-(7) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum, and the identity for divided differences: with sa acting on polynomials by xa↔xa+1 and ∂a=(1−sa)/(xa−xa+1), one has ∂axa−xa+1∂a=1, ∂axa+1−xa∂a=−1, ∂a2=0 and ∂a(fg)=∂a(f) g+sa(f) ∂a(g) for all polynomials f,g.

[F4]

Matsumoto's theorem: braid connectivity of reduced expressions, with singleton detection in dihedral subgroups, clauses (1)–(2), connects reduced expressions by braid moves and transforms a nonreduced word by braid moves to an adjacent repeat; here the Coxeter system is that of adjacent transpositions in Sn.

Proof

technique · direct; construct the shifts, verify the relations case by case, then prove injectivity and the localized isomorphism
1.1givenF2algebra

(Shifts.) Write pij:=deg⁡[i,j]Pij and Δij:=−bij−pij for i≠j. By [F2], pij+pji=−2bij, so Δji=−Δij. Fix the given finite order on I and set w(ν):=∑a<b, νa>νbΔνbνa. An adjacent unequal swap only changes the contribution of that pair, hence w(saν)−w(ν)=Δνaνa+1. This explicit formula supplies the shifts on every sequence; any two shift functions differ by a constant on each fixed-content orbit, since adjacent unequal swaps connect it.

1.2F3F4algebrainduction

(Spanning.) Move dots to the right using relation (6), inducting on the number of dot/crossing inversions and the crossing length of correction terms. By [F4], any nonreduced transposition word admits finitely many braid moves exposing an adjacent repeat, and any reduced word connects to the chosen one by braid moves. Each braid correction has three fewer crossings and each quadratic substitution removes two; induction on crossing length therefore reduces all correction terms, while the finite chosen sequence of braid moves handles the leading term. Hence the monomials τwxae(ν) span.

2.1givenF1F2algebraconstruct

(Definition and homogeneity.) Define e(ν) and xa as stated and τa by the two displayed formulas. Each formula is a finite sum of polynomials times a permutation of the variables, hence a well-defined k-linear endomorphism; the equal-colour quotient lies in k[x1,…,xn] because f−saf vanishes on xa=xa+1 (The polynomial ring over a commutative ring as finitely supported coefficient sequences with convolution, Polynomial rings in finitely many commuting indeterminates by iteration). With the shifts of step 1.1, on each word component xa is homogeneous of degree 2dνa (the shifts are constant on a summand and do not change dot degrees), and τa is homogeneous of degree −bνaνa+1: on unequal colours in the target summand saν, the variable xa+1 has color p and xa has color q, so the factor Ppq(xa+1,xa) has degree deg⁡[p,q]Ppq, so multiplying by it and passing to the summand saν with shift w(saν)=w(ν)+Δpq changes the total degree by deg⁡[p,q]Ppq+Δpq=−bpq; on equal colours the divided difference has degree −2dp=−bpp because its numerator has degree deg⁡f and the denominator has degree 2dp.

3.1step 2.1F3algebra

(Relations (1), (2), (3), (5), (6).) Relations (1)-(3) are immediate from the definitions: the e(ν) are orthogonal idempotents summing to 1, x's commute and commute with the e(ν), and both displayed τa's map the ν-summand to the saν-summand. Relation (5) holds because τa and τb with ∣a−b∣>1 act on disjoint sets of variables and their polynomial factors commute. For (6): if b∉{a,a+1} the multiplication by xb commutes with sa and with the factor Pνaνa+1(xa+1,xa), giving τaxb=xbτa=xsa(b)τa; if b=a and νa≠νa+1 then τaxaf=P(xa+1,xa)xa+1saf=xa+1τaf, and b=a+1 is the same with xa; if νa=νa+1 the two identities ∂axa−xa+1∂a=1 and ∂axa+1−xa∂a=−1 of [F3] are exactly the two displayed dot moves.

3.2step 2.1F1F3algebra

(Relation (4).) On equal colours τa2=∂a2=0=Qpp(xa,xa+1)e(ν) by [F3] and Qpp=0. On unequal colours (p,q) a double application gives τa2(fe(ν))=Pqp(xa+1,xa) sa(Ppq(xa+1,xa)saf)=Ppq(xa,xa+1)Pqp(xa+1,xa)f=Qpq(xa,xa+1)f, which is relation (4) because Qpq(u,v)=Ppq(u,v)Pqp(v,u) evaluated at (u,v)=(xa,xa+1) equals Ppq(xa,xa+1)Pqp(xa+1,xa).

4.1step 2.1step 3.2F3algebra

(Relation (7), equal outer colours (i,j,i).) Work on e(i,j,i) in variables x1,x2,x3=xa,xa+1,xa+2, write P=Pij, P′=Pji, Q=PP′(v,u), let s=(12), t=(23) and r=tst=sts=(13); write A=τa+1τaτa+1 and B=τaτa+1τa. Expanding the definitions on fe(i,j,i) and collecting the outer factor, Af=P(x3,x2)⋅t[∂a(P′(x3,x2) tf)] and Bf=P′(x2,x1)⋅s[∂a+1(P(x2,x1) sf)]. Using t∂at=(1−r)/(x1−x3) and ∂a+1(hg)=∂a+1(h)g+t(h)∂a+1(g) with h=P′(x3,x2) first, then the mirrored expansion of B with h=P(x2,x1), gives Af=P(x3,x2)[P′(x2,x3)f−P′(x2,x1)rf]/(x1−x3) and Bf=P′(x2,x1)[P(x1,x2)f−P(x3,x2)rf]/(x1−x3). Subtracting, the two rf-terms cancel and the remaining coefficient is P(x3,x2)P′(x2,x3)−P(x1,x2)P′(x2,x1)=Q(x3,x2)−Q(x1,x2), so (A−B)f=Q(x1,x2)−Q(x3,x2)x3−x1f, which is relation (7) on e(i,j,i).

5.1step 3.1step 4.1F1F3algebra

(Relation (7), remaining colours.) If νa=νa+1=νa+2=i, then all three operators are divided differences and both braid words equal the same antisymmetrizer expression ∑w∈S3sgn⁡(w)w/∏i<j(xi−xj), so A−B=0, consistent with Qii=0; if exactly the outer two colours agree, step 4.1 applies with the two adjacent colours distinct; if only the first two colours agree, say (i,i,j), then with h=Pij(x2,x1)Pij(x3,x1), which is symmetric in x2,x3, the two expansions give Af=∂a+1(h⋅stf) and Bf=h⋅st ∂a(f), and the product rule plus the Demazure identity ∂a+1st=st ∂a valid for the 3-cycle w=st yield A−B=0; the case (i,j,j) is the mirror image, obtained by reading the same identities from the other end. If the three colours are distinct, both A and B act as the same product PijPikPjk (with arguments placed by the two expansions, all three factors read off the three crossed pairs) times the longest permutation r, and A=B; the expansion is by the same substitution t∂at=(1−r)/(x1−x3) as in step 4.1 applied to three distinct colours, where the two middle expressions coincide because the two factorizations of the long element have the same length. Hence relation (7) holds in every case.

6.1step 2.1step 3.1step 3.2step 4.1step 5.1construct

(The homomorphism.) Steps 3.1, 3.2, 4.1 and 5.1 verify relations (1)-(7) for the operators, and step 2.1 shows each word-component generator acts homogeneously of its assigned degree, so the universal property of the presented algebra gives a homomorphism ρ:Rn(Q)→Endkgr(Poln{w}) of graded algebras with ρ(Rn(Q)m)Poln,d⊆Poln,d+m.

7.1step 6.1step 1.2choosealgebra

(Faithfulness.) Localize for this step only at the nonzero elements {Pij(xa,xb):νa≠νb} and {xa−xb:νa=νb}; the localized operators of a reduced word w=si1⋯sir on a fixed source sequence ν have the form cw⋅w+∑u<wcuu where cw≠0 is the product of the nonzero P-factors (unequal crossings) and the nonzero coefficient −1/(xa−xa+1) (equal crossings), and the terms u<w are strictly shorter permutations. Suppose ∑ν∑w,acw,aτwxae(ν) acted as zero; for the maximal w occurring in a fixed source/destination block the leading terms give a nontrivial linear relation ∑wdww=0 among distinct automorphisms w of the field k(x1,…,xn). Distinct automorphisms are linearly independent: take a relation with the least positive number of nonzero coefficients; one term cannot vanish on 1. With at least two terms, choose w≠w0 and g with w(g)≠w0(g), evaluate on fg, and subtract w0(g) times the evaluation on f. The w0 term disappears and the w coefficient stays nonzero, contradicting minimality; hence no nonzero combination of the spanning monomials of step 1.2 acts as zero and ρ is injective.

8.1step 1.2step 7.1algebra∎

(Localized isomorphism and finiteness.) Inverting the factors and differences makes every unequal-colour crossing τa equal to sa up to an invertible scalar, and every equal-colour crossing satisfy sa=1−(xa−xa+1)∂a, so the localized image contains all variable permutations sa and all multiplications xa, i.e. the localization of the skew group algebra An(I)=(⨁ν∈Ink[x1,…,xn]e(ν))⋊Sn; with injectivity from step 7.1 and the evident containment of the image in the localized algebra, ρ becomes an isomorphism after localization. For finiteness of homogeneous components: by step 1.2 the monomials with w∈Sn and dot exponents aj≥0 span Rn(Q); for fixed weight β and degree m the finitely many w and ν occur, each crossing degree is one of finitely many integers bounded below, and each dot has positive degree 2dνa, so the total dot degree of a spanning monomial of degree m is bounded, leaving only finitely many exponent tuples; hence dim⁡kR(β)m<∞.

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The PBW (monomial) basis theorem for KLR algebras

Statement

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum and fix a reduced-expression system: for each w∈Sn one reduced word w=si1⋯sir, and for ν∈In put τw:=τi1⋯τir∈Rn(Q). Then the monomials τwx1a1⋯xnane(ν), over all w∈Sn, a1,…,an≥0 and ν∈In, form a k-basis of Rn(Q); equivalently Rn(Q) is a free k-module on these monomials, and R(β) has the corresponding basis. Moreover each R(β) has finite-dimensional homogeneous components, and the graded dimension of the summand e(ν)Rn(Q)e(ν′) is the formal Laurent Hilbert series counting the monomials (bounded below, equivalently the finite sum of the corresponding rational geometric series), so the graded ranks are independent of the parameters Q: for each fixed β, dim⁡kR(β)m<∞ for all m and R(β)m=0 for m≪0; if I is finite the same holds for Rn(Q). In particular R(β) is a locally finite graded algebra; its degree-zero part need not be one-dimensional (already x1τ1∈R(2αi)0 is a nontrivial idempotent).

Facts & Assumptions

Given: A KLR datum Q with the algebra Rn(Q) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum, its grading of The KLR grading and the diagrammatic multiplication, a reduced-expression system for Sn, and the faithful graded polynomial representation of Faithful polynomial representation of a KLR algebra on Poln.

[F1]

Faithfulness (Faithful polynomial representation of a KLR algebra): the operators of the polynomial representation satisfy relations (1)-(7) and the homomorphism ρ:Rn(Q)→Endkgr(Poln{w}) is injective for nonzero Pij, and it becomes an isomorphism onto the localized skew group algebra k(I)[x]⋊Sn after inverting the nonzero polynomials Pij(xa,xb) and differences xa−xb.

[F2]

Relations (4), (5), (6), (7) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum, used as rewriting rules for words in the generators, and the degree assignment deg⁡xa=2dνa>0, deg⁡τa=−bνaνa+1 of The KLR grading and the diagrammatic multiplication.

[F3]

Reduced-word moves and deletion: Matsumoto's theorem: braid connectivity of reduced expressions, with singleton detection in dihedral subgroups, clauses (1) and (2), applied to the type-A Coxeter system of adjacent transpositions, connects reduced words by far and three-term braid moves and transforms any nonreduced word by such moves to an adjacent repeat.

Proof

technique · direct; first reduce arbitrary words to monomials with reduced crossing words and right-hanging dots, then obtain independence from the faithful polynomial representation
1.1givenF2algebra

(Dots move right.) Move the word idempotents to the right using relations (2)–(3). On each resulting component, if xb stands immediately left of τa, relation (6) gives xbτae(ν)=τaxsa(b)e(ν) except for adjacent equal colours. In that case the exact rules are xaτae(ν)=τaxa+1e(ν)+e(ν) and xa+1τae(ν)=τaxae(ν)−e(ν). The leading term moves one dot past one crossing, and each correction removes that dot and crossing; hence every term has fewer dot/crossing inversions. Induction on their number puts all dots to the right of all crossings.

2.1step 1.1F2F3inductionalgebra

(Crossing words reduce.) Induct on crossing length. By [F3], a nonreduced transposition word can be changed by finitely many far and braid moves into a word with an adjacent repeat; each braid correction has three fewer crossings and is handled by induction after step 1.1, and relation (4) removes the repeated pair. For a reduced word, [F3] connects it to the chosen reduced word by finitely many braid moves; their correction terms again have fewer crossings. Thus every crossing word is a sum of chosen τw times dot polynomials, and step 1.1 puts the dots on the right. This proves spanning without a decreasing-length claim for braid moves themselves.

3.1step 2.1F1choosealgebra

(Independence.) Under the representation of [F1], the image of τwxae(ν) in the localization at the nonzero Pij(xa,xb) and xa−xb is triangular: expanding the operators of the chosen reduced word, its highest term is a nonzero scalar times the permutation w acting on the summand, and all other terms are permutations of strictly smaller length (an unequal crossing contributes its nonzero P-factor together with the transposition, an equal crossing contributes (1−sa)/(xa−xa+1)=−(sa−1)/(xa−xa+1), again transposition plus lower-length terms). A linear relation ∑cw,a,ντwxae(ν)=0 in Rn(Q) would therefore give, after applying ρ and looking at a source/destination block and the maximal occurring length, a nontrivial linear relation ∑wdww=0 among distinct permutations w of the field k(x1,…,xn). Distinct field automorphisms are linearly independent: in a shortest nonzero relation choose two different automorphisms w,w0 and g with w(g)≠w0(g). Evaluation on fg minus w0(g) times evaluation on f removes one term and leaves the w term nonzero, contradicting minimality; a one-term relation is impossible by evaluation on 1. Hence the spanning monomials of step 2.1 have linearly independent images, and since ρ is injective by [F1] applied to the fixed factorization, the monomials themselves are linearly independent; together with step 2.1 they form a basis.

4.1step 3.1F2algebra

(Grading bookkeeping.) The bidegree of the basis monomial τwx1a1⋯xnane(ν) is (ν,wν) together with the integer deg⁡(τw on ν)+∑jaj⋅2dνj, where deg⁡(τw on ν) is the sum of the degrees −bνrνr+1 of its crossings read in the successive permuted sequences; this is independent of the parameters Q and of the factorization. The summand e(ν)Rn(Q)e(ν′) therefore has the Laurent Hilbert series ∑w:wν′=νqdeg⁡(τw on ν′)∏j=1n(1−q2dνj′)−1, a finite sum of rational geometric series bounded below (each dνj>0 and the finitely many crossing degrees are bounded below), which proves the displayed graded-dimension claim and shows that R(β)m=0 for m below the finite minimum of the finitely many crossing contributions over the finitely many ν,w with wν=ν′ and ∑jανj=β.

5.1step 3.1step 4.1algebra∎

(Local finiteness.) Fix β∈Q+ and a degree m. The basis monomials of R(β)m involve only the finitely many sequences ν∈Iβ and the finitely many w∈S∣β∣; each crossing degree is one of the finitely many integers −bpq and each dot degree 2dνj is at least 2min⁡idi>0, so ∑jaj is bounded, leaving finitely many exponent tuples; hence dim⁡kR(β)m<∞. If I is finite, Iβ is finite for every ∣β∣, so the same argument applies to Rn(Q) degree by degree. The element x1τ1∈R(2αi)0 is nonzero by the basis of step 3.1 and squares to itself by the nil-Hecke dot move, so degree zero need not be one-dimensional.

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Induction and restriction bimodules for KLR algebras

Definition

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum. For β,γ∈Q+ put e(β,γ):=∑ν∈Iβ,ν′∈Iγe(ν∗ν′)∈R(β+γ), where ν∗ν′ is concatenation; this is an idempotent. The block inclusions R(β)↪R(β+γ), r↦r⊗1 and R(γ)↪R(β+γ), s↦1⊗s combine into an injective k-algebra map R(β)⊗kR(γ)→R(β+γ) whose image is the separated-block subalgebra of the corner e(β,γ)R(β+γ)e(β,γ); the inclusion generally is proper; in the diagram calculus it is horizontal concatenation of diagrams. Induction and restriction are the functors on graded left modules Indβ,γ(M⊠N):=R(β+γ)e(β,γ)⊗R(β)⊗kR(γ)(M⊗kN),Resβ,γL:=e(β,γ)L, where ⊗R(β)⊗kR(γ) is the graded balanced tensor product of Graded balanced tensor product and homogeneous Hom (total-degree grading) and M⊗kN carries the graded tensor product structure; Ind is a functor on graded modules over the graded algebra R(β)⊗kR(γ) (through the tensor product of the two graded modules) and, since R(β+γ)e(β,γ) is a graded (R(β+γ),R(β)⊗kR(γ))-bimodule and e(β,γ)R(β+γ) is its right-module counterpart, the two tensor functors are of the two sidedness types of Associative and graded bimodule tensor–Hom adjunction. Both functors are additive and degree-zero on degree-zero maps and extend to the direct sums over weights. Shifts satisfy Indβ,γ(M{r}⊠N{s})≅Indβ,γ(M⊠N){r+s} and Resβ,γ(L{r})≅(Resβ,γL){r} (Graded associativity, units, and internal-shift tensor isomorphisms). For a partial flag β=β1+⋯+βr the iterated functors are defined by iteration, and the parenthesization-independent identification is the one consumed below.

Remarks

Well-definedness. Concatenation sends the two tensor-factor identities to e(β,γ) and respects the relations of each block, so r⊗s↦r⋅(image of s) is a unital algebra homomorphism from R(β)⊗kR(γ) onto the separated-block subalgebra of the corner; note that it is unital into the corner, not into all of R(β+γ), and the two block images commute because separated generators commute by relations (3), (5) and (6) with ∣a−b∣>1. Injectivity is read off the PBW basis of The PBW (monomial) basis theorem for KLR algebras: the monomials whose permutation word lies in the parabolic subgroup S∣β∣×S∣γ∣ (in the appropriate block positions) and whose dot exponents are arbitrary are exactly the images of the tensor products of the two PBW bases, hence are linearly independent. The image can be strictly smaller than the corner: for β=γ=αi the corner is the nil-Hecke algebra R(2αi)≅NH2, while the image is k[x1,x2]e(ii) (with x1,x2 acting blockwise), which does not contain τ1.

Functoriality and shifts. The balanced tensor product of a right and a left module over the graded algebra R(β)⊗kR(γ) is defined by the universal property with respect to balanced bilinear maps of degree 0, and both balance relations and the outer R(β+γ)-action preserve degrees; moving an internal shift through the total-degree tensor grading gives the two displayed shift isomorphisms. For an iterated flag, the maps a⊗(b⊗m)↦ab⊗m identify the balanced tensors of the different parenthesizations, so the iteration is defined up to canonical degree-zero isomorphism; the classes in the Grothendieck groups below are unaffected. The construction is choice-free: no representatives or auxiliary data are selected.

Sources

Source comparison: Khovanov–Lauda I §2.6 (the embedding, the idempotent 1ν,ν′ and the functors); Kang–Kashiwara §3 (3.9)-(3.11) (the R(m)⊗R(n)-balanced form used here); Kleshchev §2.11 (multi-factor embeddings and the induced/restricted functors).

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Generic KLR induction and restriction adjunctions preserve projectives

Statement

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum and β,γ∈Q+. Put A=R(β+γ), B=R(β)⊗kR(γ), e=e(β,γ) and c=(β∣γ). The bimodules eA and Ae are ungraded free respectively as left and right B-modules, of rank (∣β∣+∣γ∣∣β∣). As GRADED modules they are finite projective direct sums of the appropriate principal idempotent B-modules with labelled shuffle shifts: for each concatenated word ξ=ν∗η the right-module summand e(ξ)B has shift δR(w,ξ)=deg⁡(τwe(ξ)) and the left-module summand Be(ξ) has shift δL(w,ξ)=deg⁡(e(ξ)τw)=δR(w,w−1ξ), using respectively the corresponding right and left minimal shuffle representatives w; these degrees depend on the labels, and no common shift for an entire B copy is asserted. The functors Ind=Ae⊗B− and Res=e(−) of Induction and restriction bimodules for KLR algebras are exact, commute with internal shifts, and preserve finitely generated graded projectives. Ind is left adjoint to Res. The right adjoint of Res is Coind=HOM⁡B(eA,−), with (a⋅f)(t)=f(ta), and the exact generic second-adjunction formula is Coindβ,γ(M⊠N)≅Indγ,β(N⊠M){c}. Thus the second adjunction reverses the two blocks and has the displayed shift; same-ordered unshifted biadjunction is not asserted. The formula is an isomorphism of functors and holds on arbitrary graded B-modules after interpreting the right side with the block-flip equivalence. This is distinct from the cyclotomic Ei/Fi biadjunction theorem. Moreover eR(β+γ)e′ has a finite Mackey filtration indexed by nonnegative four-block weight matrices with row sums β,γ and column sums β′,γ′, whose subquotient is the corresponding composite four-block restriction, flip of the middle blocks and induction bimodule, shifted by −(b∣c); the same statement holds for arbitrary numbers of blocks.

Facts & Assumptions

Given: A KLR datum Q, weights β,γ∈Q+, the algebra A=R(β+γ) with idempotent e=e(β,γ), the tensor algebra B=R(β)⊗kR(γ), the bimodules eA and Ae, and the functors Ind=Ae⊗B−, Res=e(−) of Induction and restriction bimodules for KLR algebras.

[F1]

PBW basis (The PBW (monomial) basis theorem for KLR algebras): monomials τwx1a1⋯xnane(ν) form a basis; every permutation w has a unique decomposition w=wPwshuffle as a product of a parabolic element of S∣β∣×S∣γ∣ and a minimal-length shuffle, with additive length.

[F2]

Exactness and projectives (Bimodule tensor exactness and preservation of finite projectives have separate hypotheses): if M is flat as an underlying right A-module then M⊗A− is exact on graded left modules; if M is finite graded projective as a left B-module then M⊗A− carries finite graded projective left A-modules to finite graded projective left B-modules.

[F3]

Tensor-Hom adjunction (Associative and graded bimodule tensor–Hom adjunction): Hom⁡B,0(M⊗AX,Y)≅Hom⁡A,0(X,HOM⁡B(M,Y)) naturally, with HOM⁡ the graded hom of finite sums of homogeneous maps.

[F4]

Shifts (Graded balanced tensor product and homogeneous Hom): the balanced tensor product carries the total-degree internal grading, and outer actions by graded algebras are homogeneous; all shifts below are internal shifts.

Proof

technique · direct; decompose $Ae$ as a right block module and $eA$ as a left block module, then establish exactness, projectivity, adjunctions and the double-coset filtration
1.1givenF1algebra

(Shuffle decomposition and freeness.) Choose reduced PBW words adapted to the parabolic subgroup S∣β∣×S∣γ∣. For each concatenated word ξ=ν∗η and minimal right coset representative w, the vectors τwe(ξ)b, with b ranging through the PBW basis of e(ξ)B, form precisely the PBW basis of the right B-module Ae: the permutation is a minimal shuffle followed by an internal block permutation, with additive length, and the right idempotent records the source word in the corner e. Thus Ae≅⨁w,ξe(ξ)B{δR(w,ξ)}, with the displayed degree of τwe(ξ). Reversal of products fixing dots, crossings and idempotents preserves the defining relations and is an anti-involution; it sends Ae to eA and τwe(ξ) to e(ξ)τw−1, giving the left B-module decomposition of eA into the corresponding Be(ξ) with shifts δL(w,ξ)=deg⁡(e(ξ)τw). Both decompositions are finite sums of principal graded projectives. Ungraded, for each shuffle the sum over all concatenated ξ is one copy of B, so both ranks are (∣β∣+∣γ∣∣β∣). Neither bimodule is replaced by eAe: its unconstrained opposite endpoint is essential for the shuffle basis.

1.2givenF3algebra

(Left adjunction.) For a graded left B-module X and a graded left A-module L, currying gives the natural degree-zero bijection Hom⁡A,0(Ae⊗BX,L)→Hom⁡B,0(X,eL), Φ↦(x↦Φ(e⊗x)), with inverse f↦(ae⊗x↦a f(x)), well defined on balanced tensors and inverse by the idempotence of e; this is the adjunction of [F3] for the (A,B)-bimodule Ae.

2.1step 1.1F2F4algebra

(Exactness and projectivity.) The right B-module Ae is projective, hence flat, by step 1.1, so Ind=Ae⊗B− is exact by [F2]. Idempotent restriction is exact on left modules: for a surjection L→N, a vector en∈eN lifts to eℓ∈eL, and kernels and images commute with multiplication by the degree-zero idempotent e; no right action on L is required. A finitely generated graded projective left B-module is a summand of a finite sum of shifts of B, so its induction is a summand of the corresponding sum of shifts of Ae. As a left A-module Ae is the image of the degree-zero idempotent endomorphism a↦ae of A, hence is finitely generated graded projective. Similarly, if P is a finitely generated graded projective left A-module, realize P as a summand of a finite sum of shifts of A and apply e(−) to its split inclusion and projection. Then eP is a summand of the corresponding sum of shifts of eA, which is finitely generated graded projective as a left B-module by step 1.1. Internal shifts commute with induction and restriction because their balance relations and idempotent action have degree zero. This proves exactness, shift compatibility and both finite-projective preservation clauses.

2.2step 1.1F1F3algebra

(Coinduction and the longest shuffle.) The right adjoint of Res is Coind=HOM⁡B(eA,−) by [F3] applied to M=eA, and explicit currying gives (a⋅f)(t)=f(ta). For the second-adjunction formula let y be the longest block shuffle of the two blocks, of degree −c (each of the ∣β∣∣γ∣ crossed positions contributes the negative pairing of the two colours), and let e′=e(γ,β) be the reversed-block idempotent. By PBW there is a well-defined B-balanced coefficient map t:eAe′→B projecting onto the y-coefficient, where the reversed block order is read in B through the flip equivalence R(β)⊗kR(γ)→R(γ)⊗kR(β); dot slides and block crossings preserve the longest-shuffle coefficient, while every dot or braid correction in a shorter shuffle has strictly smaller shuffle length and is killed by t. Hence the map Φ:Ae′→HOM⁡B(eA,B), z↦(u↦t(uz)), is a degree-c map of (A,B)-bimodules, and it is compatible with the flip identification.

2.3step 1.1F1algebra

(Mackey filtration.) Fix a second flag with idempotent e′=e(β′,γ′) and choose reduced double-coset representatives for the row block permutation group and the column block permutation group acting on the ∣β∣+∣γ∣ positions. Partition the PBW monomials of the corner eAe′ by the four intersection blocks (a,b;c,d) with row sums β,γ and column sums β′,γ′, and filter by the crossing length of the double-coset representatives. The span of the double cosets of strictly smaller length is a (B,B′)-sub-bimodule: sliding a block generator across a representative either stays in its double coset with an internal block permutation, or produces a quadratic/braid correction of strictly smaller length, which lies in the smaller span. In the associated quotient only the monomials whose permutation is the minimal double-coset representative survive; they are exactly tensor products of the PBW bases of the four blocks composed with the row and column induced bimodules and the unique minimal crossing of the two middle blocks, which carries the shift −(b∣c) because the crossed colours are precisely b and c. The basis bijection defines inverse maps between the associated quotient and the composite four-block restriction/induction bimodule, so the filtration is proved and not merely a character identity; iterating the same permutation argument gives the multi-block statement.

3.1step 2.2F1F3algebra

(Triangularity and the functor formula.) Pair the right B-module shuffle basis of Ae′ (through the block flip) with the left B-module shuffle basis of eA by complementary shuffles. Ordered by shuffle length, the coefficient matrix of the pairing u↦t(uz) is triangular: a complementary pair is exactly the reduced longest shuffle with coefficient 1 up to the absorbed equal-colour signs, and a noncomplementary pair either misses its permutation or reduces by a quadratic or braid correction to strictly smaller length, hence vanishes in the associated graded. Finite triangular elimination over B (division by the diagonal units 1) inverts the matrix, so Φ is an isomorphism of graded (A,B)-bimodules; consequently HOM⁡B(eA,B)≅Ae′{c} with the B-action transported by the block flip. Since eA is finite projective over B by step 1.1, evaluation identifies HOM⁡B(eA,B)⊗BX≅HOM⁡B(eA,X) for every graded B-module X (checked on finite free modules and finite summands), and tracking the outer right B-action through the flip gives the functorial isomorphism Coindβ,γ(M⊠N)≅Indγ,β(N⊠M){c}.

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

All clauses of the statement are now proved: step 1.1 gives the freeness and the labelled shuffle shifts, step 2.1 the exactness, shift compatibility and projective preservation, step 1.2 the left adjunction, steps 2.2 and 3.1 the right adjoint and its exact reversed-block formula, and step 2.3 the finite Mackey filtration and its multi-block version.

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Nil-Hecke idempotents and divided-power KLR projectives

Definition

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum. For i∈I and n≥1 the subalgebra R(nαi) is generated by the polynomial subalgebra k[x1,…,xn] and the crossings τ1,…,τn−1 with τa2=0 (because Qii=0), the braid and far commutation relations, and the nil-Hecke dot moves, i.e. it is the nil Hecke algebra of rank n; its PBW basis is {x1a1⋯xnanτw}a∈Z≥0n,w∈Sn (The PBW (monomial) basis theorem for KLR algebras). Fix a reduced expression w0=si1⋯si(n2) of the longest element and put ∂w0:=τi1⋯τi(n2) (independent of the reduced expression). The divided-power idempotent is ei,n:=x1n−1x2n−2⋯xn−1 ∂w0∈R(nαi), and its horizontal reflection is ψ(ei,n):=∂w0x1n−1⋯xn−1. Both are nonzero idempotents of degree 0, and ei,n≠0 because the PBW basis separates the monomials involved. The divided-power projective is Pi,n:=R(nαi) ψ(ei,n){−di(n2)}, where the shift is the one fixed by the source normalization: as a graded left module R(nαi)ψ(ei,n) is the polynomial representation, it is indecomposable projective, and with this shift R(nαi) is a finite direct sum of [n]i! shifted copies of Pi,n, where [n]i!=∏a=1nqia−qi−aqi−qi−1 is the qi-factorial of Quantum integers, factorials, Gaussian binomials and divided powers at qi (at qi=1 it is n!); hence Pi,n is the unique indecomposable projective summand up to shift and EndR(nαi)(Pi,n)0=k. For a divided-power sequence θ=i1(n1)⋯ir(nr) put β=∑anaαia and Pθ:=Ind(Pi1,n1⊠⋯⊠Pir,nr) along the ordered concatenation of the blocks of Induction and restriction bimodules for KLR algebras; then [Pθ] represents the ordered product of these divided powers; one may reorder only by the proved commuting/Serre relations, adjacent colours need not commute, and for a single colour θ=i(n) one has the indecomposability above.

Projective duality. For a finite graded projective left R(β)-module P put P#:=HOM⁡R(β)(P,R(β))ψ, the ψ-twisted graded Hom into the rank-one free module, where ψ is the horizontal-reflection anti-involution. Evaluation P#→ (dual of P) identifies (P#)#≅P for finite shifted free modules, and hence for every finite graded projective; the duality reverses internal shifts and fixes each normalized Pi,n after the displayed shift.

Remark

Nil-Hecke matrix calculation. Put V=k[x1,…,xn], C=k[e1,…,en]=VSn and N=(n2). The elementary symmetric functions are algebraically independent and generate the symmetric ring: subtracting the leading symmetric monomial orbit successively expresses every invariant as a polynomial in them, and their distinct leading monomials give independence. Adjoin x1 as a root of the monic polynomial Tn−e1Tn−1+⋯+(−1)nen, then x2 as a root of its quotient by T−x1, and continue. Eliminating coefficients recovers the polynomial ring in the roots; each monic extension is free on powers below its degree. Hence V is free over C on xa with 0≤ar≤n−r.

Write δ=(n−1,n−2,…,0). Expanding the divided differences gives ∂w0(f)=∑w∈Snsgn⁡(w)w(f)/∏a<b(xa−xb): the braid relations make this independent of the reduced word, and the numerator of xδ is the Vandermonde determinant. Thus ∂w0(xδ)=1, its values are symmetric, and it kills every other Artin basis monomial by degree. It is therefore the coefficient-of-xδ trace of the monic tower. This trace has a perfect C-bilinear pairing ⟨f,g⟩=∂w0(fg): for a monic extension of degree m, the coefficient-of-Tm−1 trace has matrix zero below the antidiagonal and ones on it in the power basis, hence determinant ±1; composing these perfect trace pairings through the tower preserves perfection. Choose the finite trace-dual Artin basis (ba∗) to (ba). The operators f↦ba∂w0(bb∗f) are matrix units, all lying in NHn; faithfulness of Faithful polynomial representation of a KLR algebra therefore identifies NHn=End⁡C(V) in every characteristic.

Idempotents, column and duality. In this faithful action, E=∂w0xδ sends f to ∂w0(xδf)∈C and fixes C, so E2=E. Reflection ψ fixes dots and crossings and reverses products, giving ei,n=ψ(E) also idempotent and nonzero. Both have degree zero. The map NHnE→V, aE↦a(1), is an isomorphism with inverse f↦mfE: E is the rank-one projection onto C⋅1, so aE=ma(1)E. Its endomorphism ring is C and its degree-zero part is k, proving graded indecomposability. The trace pairing has degree −2diN and satisfies ⟨af,g⟩=⟨f,ψ(a)g⟩: this is immediate for dots and follows for ∂r by expanding (1−sr)/(xr−xr+1) in the trace formula. Consequently V#≅V{−2diN}, and Pi,n=V{−diN} is self-dual. The Artin basis degrees yield NHn≅⨁aV{−2di∣a∣}, since End⁡C(V)=V⊗CV∗; centering gives multiplicity qiN∏m=1n(1+qi−2+⋯+qi−2(m−1))=[n]i!. This also proves uniqueness of the indecomposable projective shift orbit: a finite graded projective over the connected positively graded ring C is shifted-free, by lifting a basis modulo C+ and using its projective splitting and the least-degree argument on kernel and cokernel, and the matrix equivalence transports that assertion to NHn.

Duality and induction. For a finite graded projective B=R(β)⊗R(γ)-module M, finite-projective evaluation gives HOM⁡R(Re⊗BM,R)≅HOM⁡B(M,eR)≅HOM⁡B(M,B)⊗BeR. Twisting by reflection yields (Ind⁡M)#≅Ind⁡(M#) with the same block order and grading. The identities are checked on finite shifted-free M and then its summands. Thus ordered inductions of the normalized one-color columns are self-dual, as required for bar compatibility.

Two colours and order. For several colours Pθ is defined by induction along the ordered blocks, so the class is the ordered induction product; blocks of orthogonal colors commute by the invertible degree-zero block shuffle, since their Qij are nonzero constants, while adjacent colours are related only by the Serre relations proved later on this page, so no silent symmetrization of the word θ is made. The construction selects no representatives beyond the fixed reduced-expression system of The PBW (monomial) basis theorem for KLR algebras and uses no choice principle.

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Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules

Statement

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum and β∈Q+. (i) Every finitely generated graded left R(β)-module has a decomposition into finitely many indecomposable graded modules, unique as a finite multiset of degree-zero graded isomorphism classes, including the actual shifts of their summands; in particular the category GrMod0R(β) of finitely generated graded modules has the Krull-Schmidt property. (ii) Every simple graded R(β)-module is finite-dimensional, killed by the augmentation ideal Sym+(β) of the CENTRAL color-symmetric polynomial subalgebra Cβ; up to isomorphism and shift there are finitely many, and each has a projective cover which is finitely generated. (iii) The split Grothendieck group K0(R(β)) of finite graded projective modules is a free Z[q,q−1]-module: the classes of the indecomposable finitely generated graded projectives, modulo grading shifts, form a basis with the shift action q[P]=[P{1}]; equivalently the classes of all finitely generated indecomposable graded projectives form a shift-orbit basis. Similarly G0(R(β)) is free on the shift orbits of simple modules, and the Hom pairing of projective covers and simples has diagonal entries dim⁡kEnd⁡0(Sb), with the selected cover/simple shifts, under the Hom convention of Projective–module Hom pairing on class generators.

Facts & Assumptions

Given: A KLR datum Q, a weight β∈Q+, the locally finite graded algebra R(β) with its finite-dimensional homogeneous components of The PBW (monomial) basis theorem for KLR algebras, and the shift conventions (M{r})d=Md−r of Associative graded algebras, bimodules, and internal shifts.

[F1]

PBW basis (The PBW (monomial) basis theorem for KLR algebras): the monomials τwx1a1⋯xnane(ν) form a k-basis of Rn(Q), each R(β) has finite-dimensional homogeneous components and is bounded below, and its graded ranks do not depend on the parameters.

[F2]

Finite graded projectives (Finite graded projective modules): finite graded projectivity means projectivity in GrMod0 tested against degree-zero epimorphisms, plus finite generation; the zero module is allowed.

[F3]

The finite-dimensional shift-orbit basis theorem (Shift-orbit bases for graded simple and projective classes) applies to a finite-dimensional graded algebra; R(β) is infinite-dimensional (for β≠0), so it is not applied to R(β) itself but only to its finite-dimensional central quotients below.

Proof

technique · direct; establish freeness over the central color-symmetric subalgebra, then Krull-Schmidt and projective covers by finite-dimensional endomorphism-algebra arguments, then the orbit bases
1.1givenF1algebra

(Central polynomial subalgebra and freeness.) Let Cβ be the color-symmetric polynomial subalgebra: on the summand e(ν)R(β)e(ν) it is the polynomial ring in the elementary symmetric functions of the dots of each color separately. It is central: unequal crossings permute dot positions, and equal-color divided differences ∂a commute with symmetric polynomials in xa,xa+1 by the Leibniz rule ∂a(fg)=∂a(f)g+sa(f)∂a(g) applied to sa-invariant f. For a color occurring m times, start with A0=k[E1,…,Em] and f0(T)=Tm−E1Tm−1+⋯+(−1)mEm. Successively put Ar=Ar−1[Xr]/(fr−1(Xr)) and fr(T)=fr−1(T)/(T−Xr) for 1≤r≤m; the division has zero remainder in Ar[T] and fr is monic of degree m−r. Monic division makes Ar free of rank m−r+1 over Ar−1, with basis 1,Xr,…,Xrm−r. In Am the identity f0(T)=∏r=1m(T−Xr) identifies Ej with the elementary symmetric polynomial in the Xr. Thus k[x1,…,xm]→Am, xr↦Xr, is surjective, and its inverse sends Xr↦xr and Ej to that elementary symmetric polynomial: each successive root relation holds under this substitution. Consequently k[x1,…,xm] is free of rank m! over its symmetric coefficient subring, on the Artin monomials x1a1⋯xmam with 0≤ar≤m−r; only the first extension, not the full polynomial ring, has rank m. Combining with the PBW basis [F1], whose dot monomials factor over the color blocks, gives that R(β) is a finite free Cβ-module, of rank (∣β∣!)2 per weight counting the permutation basis; only centrality and this freeness are used below.

2.1step 1.1F2algebra

(Krull-Schmidt and splitting.) Every finitely generated graded module is bounded below and locally finite by [F1]. Choose finitely many homogeneous generators of degrees dj; evaluation on the generators injects End⁡0(M) into the finite product of the finitely many finite-dimensional pieces Mdj, so every degree-zero endomorphism algebra is finite-dimensional, and a nontrivial homogeneous idempotent splits M into two nonzero summands with strictly smaller endomorphism algebras; splitting terminates. For an indecomposable M, every endomorphism f satisfies a polynomial minimal equation because End⁡0(M) is finite-dimensional; factoring it as Trg(T) with g(0)≠0, Bezout gives a polynomial projector separating the nilpotent part from the invertible part, so indecomposability forces f or 1−f to be invertible. Hence the nonunits form the unique maximal ideal, and the usual comparison of two decompositions ⨁piijpj=id produces a matching summand and cancellation, proving uniqueness in the degree-zero category; the shifts are recorded as part of each summand.

3.1step 1.1step 2.1F1algebra

(Simples and covers.) For a graded simple S and a positive-degree central c∈Cβ+, the kernel and image of c are graded submodules; if c acted nontrivially it would be injective and hence surjective, contradicting the least nonzero degree of the bounded-below module S; so Cβ+S=0 and S is finite-dimensional because Rˉ=R(β)/Cβ+R(β) is finite-dimensional by step 1.1. The finite-dimensional basis theorem [F3] applies to Rˉ: it has finitely many graded simple shift orbits, and the same then holds for R(β), since any simple R(β)-module is one. Projective covers are then lifted to R(β): choose a finite shifted-free R-module F whose reduction Fˉ surjects onto the projective cover Qˉ↠Sˉ. That surjection splits by projectivity of Qˉ, giving an idempotent of End⁡Rˉ0(Fˉ); entrywise reduction End⁡R0(F)→End⁡Rˉ0(Fˉ) is surjective; the reduction kernel in End⁡R0(F) is nilpotent because its entries have positive central degree and a long product has degree exceeding every fixed difference of generator degrees minus the lower bound of F, so the projector onto Qˉ is lifted by the finite nilpotent-ideal idempotent-lifting iteration e↦e−(2e−1)(e2−e); the image Q of the lifted projector is projective, its kernel is graded superfluous (after reduction by C+ it is superfluous for Qˉ, and a bounded-below graded quotient X=C+X vanishes by its least nonzero degree), so Q is an indecomposable projective cover, and every indecomposable projective is such a cover up to shift.

4.1step 2.1step 3.1F3algebra∎

(Orbit bases.) Finite decompositions into indecomposables give that K0(R(β)) is free on the shift orbits of indecomposable finite graded projectives, with q[P]=[P{1}], and finite length of finite-dimensional modules gives that G0(R(β)) is free on the simple shift orbits; both are Z[q,q−1]-modules in the sense of Graded Grothendieck groups, shift action, and Cartan map, the shift action is free because a nonzero finite-dimensional graded module is not isomorphic to a nonzero shift of itself (compare its least and greatest degrees), and the finite-dimensional theorem [F3] gives the same statement for the quotient categories. For a projective cover Pb and simple Sc with their selected shifts, Hom⁡(Pb,Sc)=0 unless b=c at the selected shift, when it equals End⁡(Sb) by the uniqueness of the cover, whose degree-zero endomorphism ring is a division k-algebra by Schur's argument; finite-dimensionality alone does not identify it with k; this is the diagonal-entry computation of the Hom pairing of Projective–module Hom pairing on class generators. The stronger statement that the diagonal scalar rings equal k over every field, and the associated unscaled dual-basis conclusion, are not inferred here from finite-dimensional algebra alone and are proved separately later on this page; nothing above uses them.

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Maximal KLR tails give a unique induction head and absolute simple modules

Statement

Let R be any graded KLR datum in this page over any field k. For a finite-dimensional graded module M of weight β set ϵi(M)=max⁡{r:e(β−rαi,rαi)M≠0}. If S is simple and r=ϵi(S)>0, there is a simple graded R(β−rαi)-module N with ϵi(N)=0 such that ΔirS=N⊠L(ir), where L(ir) is the unique nil-Hecke simple up to shift. Conversely, for any such N, Ind(N⊠L(ir)) has a unique simple graded head S, appearing once as a composition factor, with ϵi(S)=r and ΔirS=N⊠L(ir); every other composition factor has smaller i-tail. The graded simples of every R(β) remain simple without grading and are absolutely simple; all ordinary endomorphisms are k and nonzero homogeneous endomorphisms have degree 0. The classes of normalized simples and their projective covers are therefore unscaled dual shift-orbit bases for the projective/simple Hom pairing. For each β there is a finite family of ordered divided-power words Yb whose normalized projective classes pair triangularly with the simple classes, with diagonal entries 1 after choosing the simple grading shifts. Thus the selected [P(Yb)] form an A-basis of K0(R(β)); arbitrary divided words span, but need not be a basis. The identical statements hold for maximal FIRST-color blocks, with ϵiL(M)=max⁡{r:e(rαi,β−rαi)M≠0}, restriction Δi(L,r) and induction Ind(L(ir)⊠N).

Facts & Assumptions

Given: A graded KLR datum over any field k, the functors Δi=Resβ−rαi,rαi and Ind of Generic KLR induction and restriction adjunctions preserve projectives, the finite-dimensional graded simples of Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules, and the nil-Hecke idempotents and simple L(ir) of Nil-Hecke idempotents and divided-power KLR projectives.

[F1]

With Cr=k[x1,…,xr]Sr, the full nil-Hecke algebra NHr=R(rαi) is the graded endomorphism algebra of the Artin polynomial column, a free Cr-module of rank r!; thus it is a graded matrix algebra over Cr, with the corresponding row and column shifts. Its positive-center augmentation quotient is a graded matrix algebra over k, with its unique graded simple L(ir) absolutely simple up to shift. Every finite-dimensional graded simple over R(μ)⊗kNHr is killed by that positive-center ideal and is, up to shift, uniquely of the form N⊠L(ir) for a graded simple R(μ)-module; the center-annihilation argument is supplied in step 1.1.

[F2]

Exactness, the adjunctions and the Mackey filtration of Generic KLR induction and restriction adjunctions preserve projectives: Ind is left adjoint to Res, both are exact, and a corner restriction has a finite filtration whose subquotients are composites of four-block restrictions, flips and inductions with the displayed shifts.

[F3]

Krull-Schmidt and covers (Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules): finite-dimensional graded modules have finite unique decompositions, simples are finite-dimensional, and the projective/simple Hom pairing has diagonal entries dim⁡kEnd⁡0(Sb).

Proof

technique · direct; identify the nil-Hecke tail by matrix units, compute the maximal restriction through the Mackey filtration, then run the triangular basis argument
1.1givenF1algebra

(Nil-Hecke tail and its matrix units.) The constant-colour block NHr=R(rαi) acts on its polynomial column over Cr=k[x1,…,xr]Sr. The Artin monomial basis and perfect symmetric-variable-linear trace of Nil-Hecke idempotents and divided-power KLR projectives give integral matrix units and identify the full algebra with graded endomorphisms of that free rank-r! column, hence with matrices over Cr carrying the Artin degree shifts. Reducing the positive-degree central elementary symmetric functions to zero gives the graded matrix quotient over k; its column simple L(ir) is absolutely simple, and the divided idempotent cuts out a one-dimensional image. Its full-algebra polynomial-column graded projective cover has degree-zero endomorphism ring k, although its entire endomorphism ring is Cr. If T is a finite-dimensional graded simple over R(μ)⊗kNHr, a positive-degree central operator has graded kernel and image. A nonzero such operator would therefore be invertible by graded simplicity, which is impossible on the finite nonzero degree support of T. Thus the positive tail center annihilates T, and it factors through R(μ)⊗kMat⁡r!(k) with the indicated shifts. Matrix units identify T with N⊠L(ir) for a graded simple R(μ)-module N, unique up to shift. This uses the augmentation matrix quotient for finite simples, not a false identification of the full nil-Hecke algebra with matrices over the ground field.

2.1step 1.1F2algebra

(Maximal restriction.) Let S be a finite-dimensional graded simple with r=ϵi(S)>0 maximal. The finite-dimensional module ΔirS is nonzero by the definition of ϵi and has a simple submodule; by step 1.1 it is of the form N⊠L(ir) for a graded simple R(β−rαi)-module N. If N carried a word ending in i, then concatenating any nonzero nil-Hecke tail word would produce a nonzero vector in S of tail r+1, contradicting maximality, so ϵi(N)=0. By the left adjunction of [F2] the inclusion N⊠L(ir)↪ΔirS corresponds to a nonzero map M:=Ind(N⊠L(ir))→S, which is surjective since S is simple. In the Mackey filtration of ΔirM every shuffle bringing t>0 colours i from the first block into the final tail contains a factor ΔitN and is zero; the only surviving filtration quotient is N⊠L(ir) with zero crossing shift, so ΔirM=N⊠L(ir) exactly. This is a one-surviving-quotient computation, not a semisimplicity assumption.

3.1step 2.1F1F3algebra

(Unique head and simplicity.) Every nonzero quotient Q of M has nonzero defining corner: if eQ=0 with e=e(β−rαi,rαi), then the composite Ae⊗B(N⊠L(ir))→M→Q is zero by the tensor/Res adjunction, hence Q=0. The finite graded semisimple head of M therefore has exactly one simple summand, occurring once, because its exact e-restriction is a quotient of the simple eM=N⊠L(ir); this head is S, and eM→eS is an isomorphism, so exactness gives eker⁡(M→S)=0 and every other composition factor of M has smaller tail. Underlying and absolute simplicity of S: induct on the height of β. For positive height choose i with r>0; by step 2.1 and induction N and L(ir) are absolutely simple, so eS=N⊠L(ir) has endomorphism ring k; if U≤S is any ungraded submodule with eU≠0, then eU=eS and U=S because S is generated by eS; if eU=0 and U≠0, filter S by FdS=⨁j≤dSj and U by FdU=U∩FdS. Every homogeneous algebra element of degree a sends FdU into Fd+aU, so gr⁡U embeds as a nonzero graded submodule of gr⁡S=S. Since e has degree 0 and annihilates U, it annihilates gr⁡U; graded simplicity gives gr⁡U=S, contradicting eS≠0. Thus S is simple as an ungraded module, and every R-endomorphism of S is determined on eS, giving End⁡R(S)=k. The finite-density matrix argument then shows absolute simplicity over every field: any m linearly independent vectors can be sent to arbitrary targets by one algebra element, by induction on m and the commutant k clause, so the action realizes all k-linear matrices and remains simple after field extension.

4.1step 3.1F3algebra

(Triangular divided-string basis.) Choose a cyclic order of the finite colour support and recursively strip maximal i-tails, producing for each simple shift orbit a finite tuple Yb of ordered divided powers; two simples with the same tuple agree by the unique-head recursion of step 3.1. Form P(Yb) from the reversed ordered normalized divided blocks. Its homogeneous Hom to Sc is the corresponding product of divided idempotents acting on Sc; comparing tuples lexicographically, if Yb>Yc at the first differing entry then the required tail exceeds the maximal tail of the successively stripped simple Sc, and the corner is zero. When the tuples agree, every maximal restriction is the simple tensor computed in step 2.1 and each nil-Hecke divided idempotent reduces the tail to one dimension, so by induction the diagonal Hom is a single Laurent monomial with coefficient 1. Shifting each Sb makes the diagonal 1. The finite matrix is triangular over A=Z[q,q−1] with diagonal 1; Krull-Schmidt and the projective-cover/simple Hom pairing (now with End⁡(S)=k from step 3.1) identify it with the matrix expressing the projective classes in the cover basis, and successive integral triangular elimination proves that the selected classes [P(Yb)] are an A-basis of K0(R(β)); the whole family of divided words spans because the recursion covers every simple, while redundancy of non-selected words is allowed. This completes the integral surjectivity argument without a PBW rank or flat-family shortcut.

5.1step 1.1step 3.1step 4.1F2algebra∎

(First-color version.) For maximal FIRST-color blocks use the defining idempotent e(rαi,μ) and M=Ind(L(ir)⊠N) with ϵiL(N)=0; a simple submodule of the maximal first-block restriction Δi(L,r)S has the form L(ir)⊠N by the same nil-Hecke matrix units of step 1.1, and any first-colour support of N would extend the maximal first block, so it vanishes. In the Mackey restriction of Δi(L,r)M every nontrivial shuffle bringing a positive number t of i-colours from N into the first block contains Δi(L,t)N and is zero, so the sole uncrossed quotient is L(ir)⊠N with shift 0; the defining-corner generation and exact-head argument of steps 3.1 and 3.1 are unchanged. Thus the first-block assertions are proved directly, with no unsigned star-crystal preservation assumed.

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The KLR Grothendieck ring satisfies the divided-power quantum Serre relations

Statement

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum and let K0(R):=⨁β∈Q+K0(R(β)) be the split Grothendieck group of finite graded projective modules with the shift action q[P]=[P{1}] (Split Grothendieck group of an additive category, Graded Grothendieck groups, shift action, and Cartan map, Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules). (i) The induction product [P][P′]:=[Indβ,γ(P⊠P′)] for P∈K0(R(β)),P′∈K0(R(γ)) makes K0(R) a unital associative Z[q,q−1]-algebra, and [Res] makes it a coassociative counital Z[q,q−1]-coalgebra; with the twisted multiplication on K0(R)⊗K0(R) defined by (x1⊗x2)(x1′⊗x2′)=q−(∣x2∣∣∣x1′∣)x1x1′⊗x2x2′ on homogeneous elements, [Res] is an algebra homomorphism (Generic KLR induction and restriction adjunctions preserve projectives). (ii) With the divided-power projectives Pi,n of Nil-Hecke idempotents and divided-power KLR projectives, the classes [Pi,n] satisfy, for all i≠j, the divided-power quantum Serre relation ∑a+b=−aij+1(−1)a[Pi,a] [Pj,1] [Pi,b]=0in K0(R), with the convention [Pi,0]=1, and satisfy [Pi,1][Pj,1]=[Pj,1][Pi,1] when aij=0; these are the defining relations of the negative half. (iii) Consequently the assignment θi↦[Pi,1] extends uniquely to an algebra homomorphism γ:Af→K0(R) of the divided-power form of the negative half, with γ(θi(n))=[Pi,n] and γ(θi1(n1)⋯θir(nr))=[Ind(Pi1,n1⊠⋯⊠Pir,nr)]; γ is compatible with the coproducts (r on Af and [Res] on K0(R)) and with the bar involutions, and it is Z[q,q−1]-linear.

Facts & Assumptions

Given: A KLR datum Q, its divided-power projectives Pi,n of Nil-Hecke idempotents and divided-power KLR projectives, the induction and restriction functors with their exactness, adjunction and Mackey filtration of Generic KLR induction and restriction adjunctions preserve projectives, and the negative half Af with divided powers θi(n) of The Lusztig divided-power integral form UA and Quantum integers, factorials, Gaussian binomials and divided powers at qi.

[F1]

Corner filtration (Generic KLR induction and restriction adjunctions preserve projectives): eβ,γR(β+γ)eβ′,γ′ has a finite Mackey filtration indexed by four-block weight matrices whose subquotient is the composite four-block restriction, middle flip and induction bimodule, shifted by the negative pairing of the crossed blocks; Ind is left adjoint to Res and both are exact.

[F2]

Presentation of the negative half (The Lusztig divided-power integral form UA): UA− is the A-subalgebra generated by the divided powers Fi(r), with the Serre relations; the A-form is spanned by ordered divided words, not by an ordinary free algebra on the Fi.

[F3]

The negative half over Q(q) is exactly the algebra presented by the negative Serre relations (Triangular decomposition of a quantized enveloping algebra, clause (ii)); UA− is its A-subalgebra generated by divided powers. No integral shuffle-freeness claim is taken from the formal C⟦ℏ⟧ theorem.

Proof

technique · direct; build the induction algebra and restriction coalgebra, then the contracting homotopy for the Serre relation, then descend $\gamma$
1.1givenF1algebra

(Induction algebra and restriction coalgebra.) The induction product is associative and unital: the balanced identifications of Induction and restriction bimodules for KLR algebras for the two parenthesizations of three blocks are inverse degree-zero isomorphisms, and the unit is [R(0)]=[k]. For the block algebra B, the positive-center quotient is the tensor product of the two finite-dimensional graded quotients from Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules. Their simples are absolutely simple by Maximal KLR tails give a unique induction head and absolute simple modules, so their graded semisimple quotients are products of split graded matrix algebras. Tensoring these matrix blocks gives all simple shift orbits of B; tensor products of the factor projective covers cover them, by reducing their kernels and using the graded least-degree argument. Uniqueness of covers therefore identifies K0(B) with K0(R(β))⊗AK0(R(γ)). Restriction is coassociative with counit the weight-zero component, because iterated idempotent restriction multiplies the corresponding block idempotents, and the two orders of multiplication agree. To prove that [Res] respects the twisted multiplication, apply the Mackey filtration [F1] to the corner eβ,γReβ′,γ′: PBW partitions its basis by the double cosets of the two block permutation groups, ordered by crossing length, and multiplication across a braid move changes only smaller-length terms; the associated quotient is exactly the four-block restriction/induction bimodule shifted by minus the root pairing of the two crossed middle blocks. Taking classes gives [Res](xy)=∑q−(∣y2∣∣∣x1′∣)x1x1′⊗x2x2′ with the twisted product, so [Res] is an algebra homomorphism; no use of the second adjunction is needed.

2.1step 1.1algebraconstruct

(Explicit Serre contraction.) Fix i≠j, write d=−aij, D=d+1, N=d+2, and t=[ud]Qij≠0. For 0≤r≤D, let Er be the product of the reflected nil-Hecke idempotents on the two i-blocks in irjiD−r, let sr=−di((r2)+(D−r2)), and put Cr=REr{sr}. Use right multiplication by ar=ErτN−1⋯τr+1Er+1 for Cr→Cr+1 and by br=Er+1τ1⋯τr+1Er in the reverse direction. Each string crosses j once and respectively D−r−1 or r equal-color pairs, so its degrees are did−2di(D−r−1) and did−2dir. As sr+1−sr=di(D−2r−1), both maps have degree zero between the shifted columns. The nil-Hecke identities τaEr=0 for equal-color crossings internal to its divided blocks and the braid moves give ar−1ar=0. At corner r, put Lr=arbr, Rr=br−1ar−1, with absent endpoint terms zero. Moving far crossings cancels the common strings in Lr−Rr; the remaining braid correction is the divided difference of Qij. For a monomial uavb its correction is the sum of a monomials of combined outer degree a−1, with the native minus sign. The r−1 left and D−r−1 right equal-color divided differences kill it unless a≥d; homogeneity permits a=d only when b=0, and permits no a>d. For a=d exactly the staircase exponents r−1,D−r−1 survive, each evaluated by the nil-Hecke trace calculation of Nil-Hecke idempotents and divided-power KLR projectives; transporting the variable order on the left block gives Lr−Rr=(−1)rtEr, including endpoints. Thus hr=(−1)rt−1br satisfies arhr+hr−1ar−1=Er on every corner. These degree-zero maps contract the finite complex (Cr,ar) over every field and every (Q1)–(Q4) parameter.

3.1step 2.1algebra

(Alternating classes and the aij=0 case.) A bounded complex with dh+hd=1 is split contractible: choosing the successive splittings gives a contraction with h2=0, and then d+h is an isomorphism from even to odd part; hence the alternating sum of the classes of its terms vanishes, which is exactly ∑a+b=D(−1)a[Pi,a][Pj,1][Pi,b]=0, the displayed Serre relation. If aij=0 then the crossing τ of the two colours is invertible (its square is the nonzero constant Qij), and right multiplication by it gives a degree-zero isomorphism between the two corners, so [Pi,1][Pj,1]=[Pij]=[Pji]=[Pj,1][Pi,1].

4.1step 1.1step 3.1F2F3algebra∎

(Descent of γ.) First define γ over Q(q) from the presentation of the negative Serre half: [F3] identifies the Serre-presented rational negative half with the actual negative subalgebra, and the assignments θi↦[Pi,1], extended multiplicatively and q-linearly, respect all Serre relations by step 3.1 and the commuting relation, so they define an algebra homomorphism γQ on the localization. Since the A-form is the A-subalgebra spanned by ordered divided words [F2], and [Pi,1]n=[n]i![Pi,n] by the nil-Hecke decomposition, so every rational divided power maps to [Pi,n]. These divided-word images lie in K0(R), which embeds in its rational scalar extension because its shift-orbit basis is free, the homomorphism restricts to the stated A-linear γ; the formula γ(θi1(n1)⋯θir(nr))=[Ind(Pi1,n1⊠⋯⊠Pir,nr)] is multiplicativity of γ together with the definition of Pθ. Coproduct compatibility is the Mackey computation of step 1.1, and bar compatibility is the projective # duality of Nil-Hecke idempotents and divided-power KLR projectives, which fixes each normalized Pi,n and hence each word class. No source parameter-specialization is asserted to preserve projective ranks.

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The KLR Cartan (graded Hom) pairing on the projective Grothendieck group

Definition

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum and let ψ be the horizontal-reflection anti-involution of R(β) (reflection of diagrams about a horizontal axis, which reverses the order of crossings); for a finitely generated graded left module P let Pψ be the right module with p⋅r:=ψ(r)p. For β∈Q+ define the Cartan pairing ([P],[Q])β:=gdimk(Pψ⊗R(β)Q)∈Z[q,q−1]⋅(β)q,(β)q:=∏i∏a=1βi11−q2dia, for finitely generated graded projective modules P,Q, where gdimkM=∑m∈Zqmdim⁡kMm; the tensor is over the graded algebra with the total-degree grading (Graded balanced tensor product and homogeneous Hom). Equivalently define the hom pairing ([P],[Q])β′:=gdimkHOM⁡R(β)(P,Q) (Projective–module Hom pairing on class generators, Projective Hom pairing descends and is graded sesquilinear); then ([P],[Q])β′=([P#],[Q])β for the graded left projective P#:=HOM⁡R(β)(P,R(β))ψ. Thus the tensor form is symmetric and bilinear; the Hom form is conjugate-linear in its first variable and linear in its second. For the tensor form ([P],q[Q])=q([P],[Q]) and (q[P],[Q])=q([P],[Q]), while the Hom form obeys h(qr[P],qs[Q])=qs−rh([P],[Q]). Both are additive, vanish on different-weight components, and descend to K0(R)=⨁βK0(R(β)): the tensor form is A-bilinear and the Hom form is A-sesquilinear (first variable conjugate-linear), with values in Q(q), more precisely in the localization adjoining all (1−qi2a)−1; the values lie in Z[q,q−1]⋅(β)q because Pψ⊗R(β)Q is a finite free graded module over the central color-symmetric polynomial subalgebra Cβ of Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules. Normalization: ([Pi],[Pi])=(1−q2di)−1=(1−qi2)−1 and ([Pi],[Pj])=0 for i≠j, where Pi=R(αi).

Remarks

Well-definedness. Pψ⊗R(β)Q is a graded k-vector space of finite dimension in each degree and bounded below, so its graded dimension is a well-defined element of Z((q)); the monic-root tower and PBW calculation in step 1.1 of Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules explicitly prove that R(β) is finite graded free over Cβ, although freeness is not a separate assertion of that lemma's Statement. Write V=Pψ⊗RQ. Taking the split inclusions of P and Q into finite shifted-free R-modules and tensoring their splitting maps exhibits V as a direct summand of a finite sum of shifts of R. Thus V is finite graded projective over Cβ. This upgrades the value to Z[q,q−1]⋅(β)q: lifting a homogeneous k-basis of V/Cβ+V gives a surjection from a finite shifted free Cβ-module with vanishing cokernel, whose projective splitting has kernel K with K=Cβ+K, also vanishing by the least-degree argument; hence the Hilbert series is a finite Laurent polynomial times gdim Cβ=(β)q. Symmetry of the tensor form is commutativity of the balanced tensor Pψ⊗RQ≅Qψ⊗RP under the flip; the comparison form is the evaluation isomorphism HOM⁡R(P,R)⊗RQ→HOM⁡R(P,Q), f⊗v↦(p↦f(p)v), an isomorphism for shifted free P and hence for all finite graded projective summands, twisted by ψ on the first factor.

Shifts and the two normalizations. The total Hom-degree convention is that of Projective Hom pairing descends and is graded sesquilinear, so h(P{r},Q{s})=qs−rh(P,Q); no scalar conjugation of the tensor value is valid, and the rank-one values (R(αi),R(αi))=1/(1−qi2) already show that the Hom form is not the plain scalar extension of the tensor form. The generator values follow from Pi=R(αi)=k[x1], Piψ⊗R(αi)Pi≅k[x1] with deg⁡x1=2di, and ([Pi],[Pj])=0 for i≠j because the two weight components are orthogonal. The cited projective/module Hom suppliers concern finite-dimensional algebras. Here the same shift and additivity formulas follow directly from homogeneous Hom and evaluation on finite shifted-free modules and summands; their finite-dimensional hypotheses are not applied to R(β). The anti-involution ψ is recorded explicitly because it fixes the sign of the shift in the Hom form. No choice principle is used.

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The KLR Cartan pairing is the Lusztig-normalized half form

Statement

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum, let BK be the normalized Lusztig-Kashiwara form on the negative half of The Lusztig-Kashiwara bilinear form on the negative half: the recursion and put BL:=CνBK on the weight component ν, Cν=∏i(1−qi2)−νi, the Lusztig-normalized form of The Lusztig–Kashiwara form, parameter and coproduct dictionary. Then for homogeneous x,y∈Afν the Cartan pairing of The KLR Cartan (graded Hom) pairing on the projective Grothendieck group satisfies (γ(x),γ(y))KLR=BL(x,y)=Cν BK(x,y), where γ:Af→K0(R) is the algebra homomorphism of The KLR Grothendieck ring satisfies the divided-power quantum Serre relations. Equivalently, the two bilinear forms are equal under the identification of divided-power classes; in particular the KLR pairing is Q(q)-nondegenerate on each finite weight component Afν⊗AQ(q) after extending scalars, and (γ(x),γ(y))KLR′=BL(x‾,y), where bar acts on the first input. On generators: ([Pi],[Pj])=δij(1−qi2)−1=BL(θi,θj) and ([Pi,n],[Pi,n])=BL(θi(n),θi(n))=∏a=1n(1−qi2a)−1.

Facts & Assumptions

Given: A KLR datum Q, the Cartan pairing of The KLR Cartan (graded Hom) pairing on the projective Grothendieck group on K0(R), the homomorphism γ of The KLR Grothendieck ring satisfies the divided-power quantum Serre relations, the normalized half form BK of The Lusztig-Kashiwara bilinear form on the negative half: the recursion with skew derivations ei′ of Kashiwara's skew derivations ei′ and ei′′ on the negative half, and the normalization factor Cν=∏i(1−qi2)−νi of The Lusztig–Kashiwara form, parameter and coproduct dictionary.

[F1]

Normalization and adjunction (The KLR Cartan (graded Hom) pairing on the projective Grothendieck group): the tensor form is symmetric and bilinear with ([Pi],[Pi])=(1−qi2)−1 and ([Pi],[Pj])=0 for i≠j, and Ind is left adjoint to Res.

[F2]

Mackey and the coproduct comparison (The KLR Grothendieck ring satisfies the divided-power quantum Serre relations): [Res] is an algebra homomorphism for the twisted product, so the pairing satisfies the adjunction identities (x,yy′)=(r(x),y⊗y′) and (xx′,y)=(x⊗x′,r(y)) with r=[Res].

[F3]

Determination of BK (The Lusztig-Kashiwara bilinear form on the negative half: the recursion): axioms (H), (N), (R): homogeneity, B(1,1)=1 and B(FiP,Q)=B(P,ei′Q) determine B uniquely, and peeling first letters reduces every evaluation to the base case.

[F4]

Normalization dictionary (The Lusztig–Kashiwara form, parameter and coproduct dictionary): with the source-to-library parameter transport φ:Q(v)→Q(q), φ(v)=q−1 the root-colour factor Cν converts the Kashiwara recursion into BL(FiP,Q)=(1−qi2)−1BL(P,ei′Q) and BL has the generator value (1−qi2)−1.

[F5]

Nondegeneracy (The negative-half bilinear form is symmetric, nondegenerate and integral, clause (iii)): for every 0≠x∈Uq− there is y with (x,y)≠0; equivalently the form restricted to each finite-dimensional graded piece is nondegenerate. Its construction uses the Axiom of Choice (The Axiom of Choice).

Proof

technique · direct; compare the two forms on a spanning set by the same recursive characterization, then upgrade with the supplier's nondegeneracy
1.1givenF1F2F4algebra

(Tensor adjunction.) Write A=R(β+γ), B=R(β)⊗R(γ) and e=e(β,γ). Reflection fixes each block and gives (Ae⊗BX)ψ=Xψ⊗BeA, with the same total grading. Thus T(Ind⁡X,Y)=gdim(Xψ⊗BeY)=TB(X,Res⁡Y). For X=P⊠Q, the last tensor factorizes, giving the tensor-product form. Symmetry supplies the adjunction in the other variable. Pull this identity back through γ, using its coproduct compatibility from [F2]. The coefficient of Fi⊗z in r(y) is ei′y: on words this follows by deleting an i and accumulating qi−aij for each preceding letter in the twisted product, exactly the recursion of [F4]. Weight orthogonality therefore gives T(γ(Fix),γ(y))=(1−qi2)−1T(γ(x),γ(ei′y)), with vacuum value 1.

1.2givenF3F4algebra

(Abstract side.) BK is characterized by (H), (N), (R) of [F3], and its normalized multiple BL=CνBK satisfies the generator value BL(θi,θj)=δij(1−qi2)−1 and the recursion BL(FiP,Q)=(1−qi2)−1BL(P,ei′Q) by [F4]; the same recursion with the same base value determines every value on word monomials inductively, since peeling the first letter of the first argument and applying the recursion reduces the positive height by one.

2.1step 1.1step 1.2algebra

(Comparison on monomials.) The KLR pairing and BL satisfy the same recursion and the same value at 1: on the KLR side this is step 1.1 with γ(Fi)=γ(θi)=[Pi,1]=[Pi] and the identification of the restriction class with the coproduct; on the abstract side it is step 1.2. Induction on the height of the weight components therefore gives (γ(x),γ(y))KLR=BL(x,y) on all divided-power monomials and hence on all of Af by bilinearity, using that γ is onto the classes of the divided words by The KLR Grothendieck ring satisfies the divided-power quantum Serre relations. Injectivity of γ is not used: the equality is checked on the spanning monomials.

3.1step 2.1F4F5algebra∎

(Nondegeneracy and generator values.) By [F5] the form BK, hence the unit multiple BL, is nondegenerate on each finite weight component, so the KLR tensor pairing is nondegenerate there as well; the Axiom of Choice enters only through this supplier, and the categorical comparison of steps 1.1, 1.2 and 2.1 is choice-free. The Hom-form identity (γ(x),γ(y))′=BL(x‾,y) follows from h(P,Q)=T(P#,Q) of The KLR Cartan (graded Hom) pairing on the projective Grothendieck group and γ(x‾)=γ(x)# from The KLR Grothendieck ring satisfies the divided-power quantum Serre relations, clause (iii). For the rank-one divided power, γ(θi(n))=[Pi,n] gives ([Pi,n],[Pi,n])=∏a=1n(1−qi2a)−1, matching BL(θi(n),θi(n)) by the recursion of step 1.2; for n=1 this is the generator value already recorded.

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The KLR category categorifies the negative quantum half

Statement

Let Q be a KLR datum as in The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum over any field k. Then the homomorphism γ:Af→K0(R) of The KLR Grothendieck ring satisfies the divided-power quantum Serre relations is an isomorphism of Z[q,q−1]-algebras and of N[I]-graded twisted bialgebras: (i) Surjectivity. Every class in K0(R(β)) is a Z[q,q−1]-linear combination of classes of divided-power projectives [Pθ], θ a sequence of divided powers of weight β; hence γ is onto. (ii) Injectivity. γ is injective, because it preserves the forms by The KLR Cartan pairing is the Lusztig-normalized half form and the source form BL (equivalently BK) is nondegenerate on each finite weight component. (iii) Compatibility. γ intertwines the multiplications ([Ind] against the product in Af), the comultiplications ([Res] against r), the bar involutions and the forms; the free A-rank of K0(R(β)) equals the free A-rank of Afβ; no rank or dimension comparison of the infinite-dimensional algebra R(β) itself with fβ is asserted. Equivalently, K0(R) is a free A-module with the classes of the indecomposable graded projective R-modules as a shift-orbit basis (Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules), and the divided-power classes span; the triangularly selected classes [P(Yb)] form an A-basis, whereas the family of all divided-power words is generally redundant.

Facts & Assumptions

Given: A KLR datum Q over any field k, the algebra Af of the divided-power form of the negative half with its generators θi(n) of The Lusztig divided-power integral form UA, the homomorphism γ of The KLR Grothendieck ring satisfies the divided-power quantum Serre relations, and the Cartan form comparison of The KLR Cartan pairing is the Lusztig-normalized half form.

[F1]

Triangular basis and simplicity (Maximal KLR tails give a unique induction head and absolute simple modules): for each β there is a finite family of ordered divided-power words Yb with [P(Yb)] a triangular A-basis of K0(R(β)) with diagonal 1, and the graded simples are absolutely simple with all nonzero homogeneous endomorphisms of degree 0.

[F2]

Form comparison (The KLR Cartan pairing is the Lusztig-normalized half form): (γ(x),γ(y))KLR=BL(x,y) on each weight component, and BL is a unit multiple of the nondegenerate normalized form BK.

[F3]

Nondegeneracy (The negative-half bilinear form is symmetric, nondegenerate and integral): BK is nondegenerate on each finite weight component; this uses the Axiom of Choice (The Axiom of Choice).

[F4]

Proof

technique · direct; surjectivity by the triangular divided-string basis, injectivity by the preserved nondegenerate form, then compatibility
1.1givenF1algebra

(Surjectivity.) By [F1] the classes [P(Yb)] form an A-basis of K0(R(β)) for a finite family of ordered divided-power words; each Yb is a word in divided powers of single colours, so its class equals γ(θi1(n1)⋯θir(nr)) by multiplicativity of γ and the definition of Pθ. Hence every class in K0(R(β)) is an A-linear combination of classes [Pθ] of divided-power projectives, and γ is onto.

2.1step 1.1F2F3algebra

(Injectivity.) Suppose γ(x)=0 for some x∈Afν. By [F2] and [F3], for every y in the same weight component one has BL(x,y)=(γ(x),γ(y))=0; since BL is a unit multiple of the nondegenerate form BK on the finite-dimensional Q(q)-space Afν⊗AQ(q), this forces x=0. The categorical and form-comparison steps of [F2] are choice-free; the Axiom of Choice is inherited only through the nondegeneracy supplier [F3].

3.1step 1.1step 2.1F1F4algebra∎

(Compatibility and ranks.) The intertwining of multiplications is multiplicativity of γ together with the induction formula of The KLR Grothendieck ring satisfies the divided-power quantum Serre relations; the intertwining of comultiplications is the Mackey comparison of Generic KLR induction and restriction adjunctions preserve projectives against the coproduct r of the negative half; the bar compatibility is Pi,n#=Pi,n for the normalized divided projectives of Nil-Hecke idempotents and divided-power KLR projectives, and form preservation is [F2]. Since γ is an isomorphism of A-modules by steps 1.1 and 2.1, the free A-rank of K0(R(β)) equals that of Afβ; the finite free basis supplied by [F1] transfers through γ to a finite free basis of Afβ, and the infinite-dimensional algebra R(β) itself is not compared with fβ.

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Self-dual KLR projectives have positive first-block divided-string leading terms

Statement

For any graded KLR datum in this page and any field k, each finite-dimensional graded simple shift orbit has a unique representative Sb self-dual for D(M)d=Hom⁡k(M−d,k) with action (af)(m)=f(ψ(a)m). Its projective cover Pb, normalized by Hom⁡0(Pb,Sb)=k, satisfies Pb#=Pb for P#=HOM⁡R(P,R)ψ. These are unique normalizations. Induction of two self-dual finite projectives is self-dual. If ϵiL(Sb)=r>0 and Δi(L,r)Sb=L(ir)⊠Sa with ϵiL(Sa)=0, normalized as above, then [Pi,r][Pa]=[Pb]+∑ϵiL(Sc)>rmc(q)[Pc], with mc∈N[q,q−1] each invariant under q↦q−1. Under γ the integral LEFT divided-string ideal I(i,≥n)=∑r≥nFi(r)UA− is the A-span of [Pb] with ϵiL(Sb)≥n. Consequently, if the normalized projective classes are known to be a SIGNED lower-global set, this leading coefficient 1 identifies them with the POSITIVE lower-global set using the general adapted LEFT-string recursion; no finite-ADE canonical-comparison theorem is needed. For the conclusions compared with the quantum half and the conditional lower-global/LEFT-string recursion, carry the inherited Axiom of Choice of those quantum suppliers; the generic finite module duality/parity/Frobenius arguments themselves are choice-free.

Facts & Assumptions

Given: A graded KLR datum over any field k, the graded simple modules and projective covers of Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules with the maximal-tail triangular basis and absolute simplicity of Maximal KLR tails give a unique induction head and absolute simple modules, the duality P# and pairing of The KLR Cartan (graded Hom) pairing on the projective Grothendieck group, and the isomorphism γ of The KLR category categorifies the negative quantum half.

[F1]

Maximal-tail basis (Maximal KLR tails give a unique induction head and absolute simple modules): there is a finite triangular A-matrix of divided-idempotent Homs against simples with diagonal 1, the simples are absolutely simple, and the selected divided words Yb give a triangular A-basis of K0(R(β)); the identical assertions holds for maximal FIRST-colour blocks.

[F2]

Divided powers (Nil-Hecke idempotents and divided-power KLR projectives): Pi,n is the unique indecomposable projective summand of R(nαi) up to shift and Pi,n#=Pi,n; [Pi,n]=γ(θi(n)).

[F3]

Categorification (The KLR category categorifies the negative quantum half): γ is an isomorphism of A-algebras intertwining induction products with the algebra product, restriction with the coproduct, and the bar involutions, with both sides free over A componentwise.

[F4]

Global suppliers (Bar invariance, congruence and uniqueness of the lower global basis, The highest weight and negative half integral crystal triples are balanced): the lower global basis of the negative half and its integral balanced globalization, and the adapted LEFT-string ideal decomposition and normalized transition of clause (v) of the balanced theorem: if e~ia=0, then Fi(r)G(a)−G(f~ira)∈I(i,≥r+1), are available under the stated hypotheses.

Proof

technique · direct; normalize dualities by word characters, compute the first-block expansion, then compare with the integral string ideals and the global recursion
1.1givenF1algebra

(Self-dual simples.) The maximal-tail supplier [F1] gives a triangular divided-idempotent/simple Hom matrix with diagonal 1 over A=Z[q,q−1], which remains invertible at q=1. Ordinary dimensions of divided-word corners are determined by ordinary word dimensions: in each constant-colour block the nil-Hecke matrix presentation makes the polynomial column simple of rank r! and the divided idempotent a rank-one matrix projection, so dim⁡(edivM)=dim⁡(eexpandedM)/∏rr! for every finite module M, including nonsemisimple central quotients. Hence ordinary word characters separate simple shift orbits. The vector duality D(M)d=Hom⁡k(M−d,k) preserves simple modules and fixes ordinary word dimensions because ψ fixes the word idempotents, so DS≅S{s} for some integer s.

2.1step 1.1algebra

(Evenness and normalization.) Choose a total colour order and set p(ν)=∑a<b, νa>νbbνaνb mod 2. Each adjacent unequal swap changes p by its crossing degree modulo 2, and equal crossings and dots have even degree, so the PBW basis puts e(η)Re(ν) in degrees congruent to p(η)−p(ν); a graded module therefore splits into the two submodules on which d−p(ν) is fixed modulo 2 on e(ν)Md, and a simple uses one of them. Since −d−p(ν)≡d−p(ν)(mod2), DS has the same sector as S, so the shift s above is even; replacing S by S{s/2} gives DS=S, and uniqueness follows because a nonzero finite-dimensional graded module is not isomorphic to a nonzero shift of itself (compare its finite least and greatest degrees).

3.1step 2.1F2algebra

(Self-dual covers and induction.) For a finite projective P and finite module M, evaluation gives Hom⁡(P#,DM)=DHom⁡(P,M) with ordinary homogeneous degrees: verify on P=Re(ν){a}, where both sides are the dual of the finite-dimensional space e(ν)M{−a} (Nil-Hecke idempotents and divided-power KLR projectives), and restrict to a finite summand. The duality # is an involution on finite projectives, so Pb# is the same normalized indecomposable projective cover of DSb=Sb, giving Pb#=Pb; a nonzero projective is bounded below, so the normalization is unique. If M is a finite projective over the separated block algebra B, then Hom⁡R(Re⊗BM,R)=Hom⁡B(M,eR)=Hom⁡B(M,B)⊗BeR by evaluation on finite free modules and summands, and twisting by ψ identifies this with Re⊗BM# without reversing the horizontal block order; for M=Pa⊠Pi,r this proves that IndM is self-dual. Restriction commutes with D because ψ fixes the defining block idempotent, so the maximal FIRST-block restriction of the normalized Sb is exactly the normalized L(ir)⊠Sa with no residual shift: that tensor is D-self-dual and any extra shift would contradict finite support.

4.1step 3.1F1F2algebra

(Leading coefficient 1.) Use the exact tensor/Res adjunction of Generic KLR induction and restriction adjunctions preserve projectives and the maximal-tail lemma [F1] to compute Hom⁡(Ind(Pi,r⊠Pa),Sc): it vanishes if ϵiL(Sc)<r; if ϵiL(Sc)=r, the maximal restriction is L(ir)⊠Sa′ and the Hom is zero unless a′=a, when it is exactly k in degree 0; the unique-head lemma makes c=b in that case. Since Hom from a projective detects the multiplicity polynomial of each summand in the decomposition, the induced projective has exactly [Pb] with coefficient 1 at tail r and all other summands at strictly higher tail, giving the displayed expansion. Self-duality of the induction and of each normalized projective forces every multiplicity polynomial to be bar invariant, and finite decompositions give nonnegative coefficients.

5.1step 4.1F3algebra

(Integral string ideals.) For every n, induction with a divided block of length r≥n has no summands of tail <n by the same Hom computation of step 4.1, so γ(I(i,≥n)) is contained in the span of the corresponding covers. Conversely descend on the finite possible tail r (bounded by βi): the coefficient-1 expansion expresses every [Pb] of tail r as [Pi,r][Pa] minus classes of strictly higher tail, which lie in I(i,≥r) already; this proves the reverse inclusion integrally, using the sum of all divided images and not a Gaussian-unit identification with a single ordinary power ideal.

6.1step 5.1F3F4algebra∎

(Signs.) Suppose [Pb]=γ(signb G(b′)) has been established by a separate norm/geometric argument. The ideal equality of step 5.1 and the adapted LEFT-string lower-global basis [F4] identify the tail partitions of these signed vectors with the LEFT string partitions; at the exact LEFT-string quotient the lower-global recursion has coefficient +1 for Fi(r)G(a′) when a′ has LEFT string 0. Induction on root height fixes signa=+1, and comparing the projective coefficient-1 expansion with this quotient fixes signb=+1; the unit/vacuum starts the induction. The reversal supplier used elsewhere promises only signed star preservation, so an unsigned right recursion is deliberately not inferred here. The Axiom of Choice enters only through the inherited quantum-half/global suppliers [F4] and The KLR category categorifies the negative quantum half (The Axiom of Choice); no additional simultaneous module-basis choice is used, and the finite duality, parity, Frobenius and first-block multiplicity arguments above are choice-free.

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Self-dual indecomposable KLR projectives give the lower global basis (symmetric type)

Statement

Assume the Cartan datum of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum has symmetric Cartan matrix aij=aji and uses the quiver normalization di=1 for every i, the field k has characteristic 0, and the KLR parameters are the quiver-geometric ones (the specialization attached to a finite quiver without loops, with arbitrary arrow multiplicities hij and aij=−(hij+hji): Qij(u,v)=(−1)hij(u−v)hij+hji for i≠j, in the fixed native crossing-sign convention; arbitrary parameter changes, including a global replacement by u+v, require their own proved gauge equivalence). Then, normalizing each indecomposable finitely generated graded projective R(β)-module to be self-dual for the contravariant graded projective duality P#=HOM⁡R(β)(P,R(β))ψ (P≅P# after the unique normalizing shift), the map b↦[Pb] is a bijection between the lower global basis B(∞) of the negative half (The lower global basis of Uq− and of a highest weight module, Bar invariance, congruence and uniqueness of the lower global basis) and the shift-orbit basis of K0(R) by self-dual indecomposable projectives; under the isomorphism γ of The KLR category categorifies the negative quantum half one has γ(G(b))=[Pb] for the lower global lift G(b), and the identification is compatible with the based quotient of The based quotient: projection of the lower global basis to a highest weight module. No extension to arbitrary KLR parameters or to non-symmetric Cartan data is asserted here; any such extension requires its own parameter-change invariance theorem.

Facts & Assumptions

Choice. Assume the inherited Axiom of Choice of the geometric and quantum suppliers; the finite presented-algebra comparison and finite graded Yoneda argument below introduce no additional choice.

[F1]

Categorical input (The KLR category categorifies the negative quantum half, The KLR Cartan (graded Hom) pairing on the projective Grothendieck group): γ:Af→K0(R) is an isomorphism of A-algebras and twisted bialgebras intertwining the forms, and every indecomposable finite graded projective shift orbit has a unique normalized self-dual representative by Self-dual KLR projectives have positive first-block divided-string leading terms, with the pairing of The KLR Cartan (graded Hom) pairing on the projective Grothendieck group.

[F2]

Positive first-string supplier (Self-dual KLR projectives have positive first-block divided-string leading terms): normalized self-dual projective covers satisfy the coefficient-1 FIRST-block expansion, the integral LEFT divided-string ideal equality, and the positive FIRST/LEFT global comparison; its inherited Axiom of Choice (The Axiom of Choice) is carried here.

[F3]

Actual geometric realization (Quiver full-flag incidence varieties and signed geometric KLR generators, Signed KLR algebra is the equivariant Ext algebra of quiver-flag complexes, Quiver-flag convolution generators satisfy the signed KLR relations, Relative-position incidence strata give a faithful geometric PBW basis): the intrinsic presentation has the full distinct-color adjacent dot slides, native equal-color mixed and braid signs, and a faithful action generated by the native polynomial operators on summands with unit degree −dν; the Ext product is a∗b=b[n]∘a for a of degree n, with source-first corner eηReν=Ext⁡G(Lη,Lν).

[F4]

Actual semisimplicity (Full quiver-flag pushforwards are semisimple in characteristic zero): for every finite loopless quiver with arbitrary finite arrow multiplicities and every characteristic-zero field, Lν=Rπν!k[dν] and their finite sum are finite direct sums of shifts of simple objects in the actual equivariant perverse heart of Middle perverse t structure glues and has simple intersection complexes. That bounded heart gives Hom⁡(T,T[n])=0 for n<0 and division End⁡(T) for simple T.

[F5]

Projective covers (Graded Krull-Schmidt and shift-orbit bases for finitely generated KLR modules, Maximal KLR tails give a unique induction head and absolute simple modules): graded indecomposable finite projectives are projective covers of finite-dimensional graded simples, and those simples are absolutely simple over k.

[F6]

Actual splitting (Cartesian simplicial sheaves model actual equivariant derived Hom): the bounded equivariant constructible category is triangulated and idempotent complete.

Proof

technique · direct; build the geometric realization, run the graded-Yoneda argument, then globalize and fix the signs with the positive first-string supplier
1.1givenF3algebra

(The graded algebra comparison.) Set Pij(u,v)=(v−u)hij for i≠j. These are nonzero, including when hij=0, and Pij(u,v)Pji(v,u)=(−1)hij(u−v)hij+hji=Qij(u,v). Thus Faithful polynomial representation of a KLR algebra gives a faithful action of R(β;Q) by projections, dots and unequal crossings (xr−xr+1)hijsr, with equal crossings (1−sr)/(xr−xr+1). The actual geometric action of [F3] uses exactly those operators. In both actions give the unit of the ν polynomial summand degree −dν: the incidence formula dν=∑iβi(βi−1)/2+∑a>bhνaνb gives dsrν−dν=hij−hji, so the unequal crossing has degree 2hij+dν−dsrν=hij+hji; equal crossings have degree −2 and dots degree 2. Both faithful images are therefore the identical graded subalgebra generated by these operators, yielding R(β;Q)≅SΓ(β)≅Ext⁡G∙(L,L) for L=⨁νLν. This is also the direct comparison of the identical specialized presentations: all adjacent unequal dot slides and the native mixed and braid signs are present in [F3]. The equal geometric crossing is minus its standard complex Borel–Moore class, so no sign change is implicit.

2.1F4step 1.1

(The actual normalized complex.) By [F4], the same L=⨁νRπν!k[dν] of step 1.1 is a finite direct sum of shifts of simple actual equivariant perverse objects. The normalization [dν] has already been included in Lν; no further shift of L is made. This uses the proved semisimplicity clause in the complete loopless multiedge scope, with no semismallness or finite-ADE restriction.

2.2F3F6step 1.1algebra

(Graded Yoneda.) Use the shifted opposite-composition product of [F3] and define YT=Ext⁡G∙(L,T) as a graded left R-module: for homogeneous a:L→L[n] and y:L→T[m], set a⋅y=y[n]∘a, so (a∗b)⋅y=a⋅(b⋅y). On T=L this is the regular left module. A homogeneous map f:T→U[t] acts by postcomposition y↦f[m]∘y of degree t. For T=U=L every graded R-linear map R→R is right multiplication by its value at 1, hence is induced uniquely by the corresponding f; extend this identification to finite sums and shifts and then to idempotent summands. Since the actual category is idempotent complete and all finite graded projectives are summands of finite sums of shifts of R, this gives a fully faithful equivalence from the additive category generated by shifts of L onto finite graded projectives, with End⁡R∙(YT)≅Ext⁡G∙(T,T) using ordinary categorical composition on both endomorphism rings.

3.1F4F5step 2.1step 2.2algebra

(Indecomposables and scalar degree zero.) Each simple perverse summand T in step 2.1 belongs to that additive category up to shift. By [F4] and step 2.2 its projective YT has no negative-degree endomorphisms and its degree-zero endomorphism ring is a division algebra, hence it is graded indecomposable. These exhaust the indecomposable projective shift orbits: every projective is a summand of a finite sum of the YT and their shifts, and [F5] gives the finite graded Krull–Schmidt decomposition. Distinct simple perverse objects yield distinct orbits, since full faithfulness would otherwise give T≅U[t], and perverse concentration forces t=0. Finally the simple head S of YT has End⁡R0(S)=k by [F5]. Every degree-zero endomorphism preserves the unique maximal graded submodule, so descent to the head is a unital k-algebra homomorphism End⁡R0(YT)→k; its kernel is zero because its source is a division algebra, and its image contains all scalars, so End⁡R0(YT)=k.

4.1step 3.1F1F2algebra

(Self-dual normalization, norm one and signed globalization.) By [F1] every indecomposable projective shift orbit has a unique # self-dual representative Pb; put xb=γ−1[Pb], which is integral and bar fixed. The exact Hom/tensor comparison for a self-dual P gives BL(xb,xb)=h(Pb,Pb), a nonnegative integer power series in q congruent to 1 modulo q, since the geometric nonnegative-End property is unchanged by grading shifts. Dividing by Cβ (which is 1 modulo q) gives a value BK(xb,xb) congruent to 1 modulo q with integer coefficients, so the general half norm criterion places xb in the q0 crystal lattice; being bar fixed, it also lies in the actual bar chart, and the integral balanced globalization writes xb as a finite Z-linear combination of lower global vectors. Their residue Gram matrix is the identity, so norm residue 1 forces the sum of coefficient squares to be 1: xb is exactly plus or minus one lower global vector. Distinct projective shift orbits are independent and have the same finite weight cardinality as the global basis by the integral K0 isomorphism, so they exhaust this signed set.

5.1step 4.1F2algebra∎

(Positivity and the based quotient.) The positive divided-string leading-term supplier [F2] removes every minus sign using its integral LEFT-string ideal equality, its coefficient-1 projective adjunction expansion, and the general adapted LEFT global recursion (carried with its inherited Axiom of Choice, The Axiom of Choice); batch 8's finite-ADE canonical-comparison item is not used. Consequently the sign in step 4.1 is +1, giving γ(G(b))=[Pb] for every lower global vector G(b) and establishing the bijection of the statement. The compatibility with the based quotient is the general zero/survival projection theorem of the QG-5 machinery.

5 · Examples, counterexamples and false statements

None yet.

Sources