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Degenerate parameters Qij destroy the faithful polynomial-representation route

Statement refuted

the faithful polynomial-representation route to the PBW basis and the Grothendieck-ring comparison of Faithful polynomial representation of a KLR algebra needs only the hermitian symmetry (Q2) and the degree condition (Q3); the nonvanishing conditions (Q1) and (Q4) can be dropped.

Facts & Assumptions

Given: The two-vertex datum I={i,j}, aij=aji=−1, di=dj=1, the degenerate pair Qij=Qji=0 satisfying (Q2) and (Q3) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum but not (Q1), and the non-hermitian pair Qij(u,v)=u+2v, Qji(u,v)=u+v satisfying (Q1), (Q3) and (Q4) but not (Q2), over a field of characteristic ≠2.

[F1]

Relation list (4) and (6) of The quiver Hecke (KLR) algebra of a symmetrizable Cartan datum: τ12e(ν)=Qν1ν2(x1,x2)e(ν), and τ1xb=xs1(b)τ1 when ν1≠ν2.

[F2]

Spanning (The PBW (monomial) basis theorem for KLR algebras, whose reduction argument uses only the relations): the family {x1ax2bτ1εe(ν)} spans R(αi+αj) for every two-vertex parameter pair, hermitian or not.

[F3]

Faithful-route hypotheses (Faithful polynomial representation of a KLR algebra): the constructed action requires a factorization Qij=Pij(u,v)Pji(v,u) with both Pij and Pji nonzero, and its faithfulness is proved only under that hypothesis.

Counterexample

Counterexample (two vertices). Let I={i,j}, aij=aji=−1, di=dj=1, and take the degenerate parameters Qij=Qji=0, which satisfy (Q2) and (Q3) but not (Q1). Then: (a) The algebra R(αi+αj) has the PBW basis displayed below even for Q=0. Indeed dots slide past crossings and crossing squares vanish, so those monomials span; independence follows from the algebra of the two-idempotent polynomial skew quiver with both length-two crossing paths zero. There is no factorization with both factors nonzero, since k[u,v] is a domain. (b) Taking Pij=0 and Pji=1 gives a well-defined polynomial action: τ1 kills the ij summand and swaps the ji summand into ij. Hence it kills the NONZERO element τ1e(ij), so is not faithful; it need not kill both crossings. For any polynomial-factor action with Q=0 at least one crossing factor vanishes, giving the same nonfaithfulness conclusion in that corner. (c) Dropping the hermitian symmetry (Q2) while keeping (Q1), (Q3) and (Q4) also destroys the basis route: over a field of characteristic different from 2, for aij=−1 and the non-hermitian pair Qij(u,v)=u+2v, Qji(u,v)=u+v (both homogeneous of degree 2 with nonzero extremal coefficients, but Qji(v,u)=v+u≠u+2v), associativity together with relation (4) on the two corners (i,j) and (j,i) and the dot slides of (6) for the pair of distinct residues gives the identity (Qji(x1,x2)−Qij(x2,x1))τ1e(ij)=−x1τ1e(ij)=0, hence τ1x2e(ij)=0; the spanning monomial τ1x2e(ij) of Rouquier's family {x1ax2bτ1εe(ν)} therefore vanishes, so that family is not linearly independent and the graded PBW statement fails. Equivalently, Rouquier's Theorem 3.7 shows that PBW is equivalent to Qij(u,v)=Qji(v,u), the identity violated here. (On (i,j,i) the braid relation reads (τ2τ1τ2−τ1τ2τ1)e(i,j,i)=−e(i,j,i): both sides have degree 0, so the failure is a linear dependence, not a degree mismatch.) Thus (Q1) is necessary for this factorized faithful-action route, and (Q2) is necessary for the PBW family. This example does not establish an independent need for (Q4) in polynomial faithfulness: for any nonzero hermitian Q, the factorization Pij=Qij, Pji=1 already has nonzero factors. The extremal-coefficient condition is used separately in the categorical Serre contraction of The KLR Grothendieck ring satisfies the divided-power quantum Serre relations, step 2.1; the example does not claim that the KLR algebra with Qij=0 fails to be free (PBW independence has its own source proof), only that the faithful polynomial-representation route used in this library collapses.

1.1givenF1F2algebra

(a) Define a k-algebra E with k-basis {x1ax2be(ij),x1ax2be(ji),x1ax2bτe(ij),x1ax2bτe(ji)}a,b≥0 and multiplication determined by: x1,x2 commuting with each other and with the idempotents; τe(ij)=e(ji)τ, τe(ji)=e(ij)τ; τ2=0; and moving a dot across a crossing permutes the two variables. Associativity holds because the dot permutation is an algebra automorphism of k[x1,x2], the idempotents are orthogonal, and every product containing two consecutive crossings or an idempotent mismatch is zero. The presentation of R(αi+αj) with Q=0 is satisfied by this model, so the universal property gives a surjection R(αi+αj)↠E, while the same Coxeter/dot reduction that proves spanning [F2] shows the model basis spans R(αi+αj); a linear dependence among those spanning elements in R would map to a dependence among basis elements of E, hence they are independent and the PBW basis of the statement holds for Q=0. This proves (a) without applying the nondegenerate PBW theorem outside its hypotheses.

2.1step 1.1F3algebra

(b) A product Pij(u,v)Pji(v,u)=0 in the domain k[u,v] forces one factor to be zero, so no factorization has both factors nonzero; taking Pij=0, Pji=1 and applying the formula of Faithful polynomial representation of a KLR algebra defines a legitimate action: on the ij summand the crossing operator vanishes, on the ji summand it is the swap. It kills the element τ1e(ij), which is nonzero by the basis of step 1.1, so this action (and by the same argument every factorized action, since at least one corner factor vanishes) is not faithful; this is exactly the failure of the faithfulness hypothesis [F3].

3.1step 1.1F1F2algebra∎

(c) For the non-hermitian pair, associativity of the word τ1τ1τ1 on e(ij) computed in the two groupings gives, using relation (4) on the ij corner for the right grouping and on the ji corner after passing through τ1 for the left grouping, (Qij(x2,x1)−Qji(x1,x2))τ1e(ij)=0; the dot slides for distinct colours are used to move dots across the crossings in the outer factors. Substituting Qij(u,v)=u+2v and Qji(u,v)=u+v gives (x2+2x1)−(x1+x2)=x1, so x1τ1e(ij)=0; applying the dot slide τ1x2=x1τ1 on the ij corner gives τ1x2e(ij)=x1τ1e(ij)=0. The element x1τ1e(ij) belongs to the spanning family {x1ax2bτ1εe(ν)} and is nonzero in the free algebra of the presentation, so that spanning family is not linearly independent and the graded PBW claim fails; equivalently, Rouquier’s PBW criterion shows that PBW is equivalent to the hermitian symmetry Qij(u,v)=Qji(v,u), which the pair violates, and the failure is a linear dependence rather than a degree mismatch.

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