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Erratum to Donaldson–Thomas invariants and flops (J. reine angew. Math. 716 (2016), 103–145)

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Veröffentlicht/Copyright: 18. Juli 2015

This is an erratum for [6] (which essentially coincides with [4]). The main result [6, Corollary 3.27] is correct. Indeed, if one assumes throughout to be working in [6, Situation 3.24] (namely, if only cares about flops) then the whole paper is fine as is. However, the key [6, Theorem 3.23] is incorrect as stated in its full generality. To reflect this, the arXiv version of the paper has been updated to [5].

This erratum is divided in three sections. The first provides an explanation as to why some statements in [6] need to be modified. The second goes through the differences between [6] and [5]. The third is an appendix to [6], which is parallel to [5, Section 4].

1 Explanation

The paper [6] is concerned with proving a comparison formula for Donaldson–Thomas (DT) invariants. Let us recall the main strategy. One starts with a flopping contraction YX and a flop Y+X. The main goal is to prove the formula

(*)DTexc(Y)DT(Y)=DTexc(Y+)DT(Y+).

The proof goes via the fact that Y and Y+ are derived equivalent. The respective categories of perverse coherent sheaves are mapped to each other under Bridgeland’s equivalence, hence the perverse Hilbert schemes are isomorphic. Up to some additional details, this formally implies that the perverse DT numbers of Y and Y+ are the same [6, Theorem 3.26].

The main focus of the paper actually lies in proving [6, Theorem 3.23], which compares the perverse DT invariants with the ordinary ones. In this sense, all the action happens on just one side of the flop.

Let us go back to our flopping contraction YX. Readers solely interested in flops can assume that the singular locus of X is zero-dimensional. In this case, the statements and proofs of [6] can be left untouched and one can safely ignore the present text.

Nonetheless, the actual perverse/ordinary comparison formula is of interest beyond the context of flops (for example in the setting of the crepant resolution conjecture for Donaldson–Thomas invariants [2, 3]).

If we allow the singular locus of X to be a curve then [6, Theorem 3.23] needs to be modified into [5, Theorem 3.23]. The latter statement, however, contains the symbol DT which we now explain.

The proof of [6, Proposition 3.5] contains a mistake, the root of which can be traced back to the following fact. Inside the category of perverse coherent sheaves 𝒜p we find 𝒜1p, consisting of those complexes having support of dimension at most one (recall that the support of a complex is the union of the supports of the cohomology sheaves).

The subcategory 𝒜1p𝒜p is not closed under subobjects nor quotients.

Let us illustrate this with an example, for which we thank the referee. For simplicity, let us assume p=-1. Suppose f:YX is contracting a divisor D1×1 to a 1, via projection to the second factor. Let C be a horizontal curve, i.e. C{l}×1 for some l1, so that we have f(C)=1. Take the following short exact sequence:

0𝒪D(-C)𝒪D𝒪C0

As f*𝒪D(-C)=0 we see that 𝒪D(-C)p. As 𝒪D and 𝒪C are quotients of 𝒪Y they both lie in 𝒯p. Therefore,

0𝒪D𝒪C𝒪D(-C)[1]0

is a short exact sequence in 𝒜p where the middle term lies in 𝒜1p while the outer terms do not.

To fix the mistake, one needs (among other things) to change the main identity (3.4) of [6]. The element 1 needs to be replaced by 𝒦1, which corresponds to the subscheme Hilb1(Y)Hilb1(Y) parameterizing those surjections 𝒪Y𝒪Z in Coh(Y) whose perverse cokernel lies in 1p[1]. This is explained in [5, Remark 3.5]. We remark that the perverse cokernel of any surjection 𝒪Y𝒪Z lies in p[1].

When X happens to have singular locus of dimension zero, 1p=p and thus Hilb1(Y)=Hilb1(Y). However, in general the two are different. Let us illustrate this by means of an example. Suppose p=-1 and assume again f:YX is contracting a divisor D1×1 to a 1. Let as before C be a horizontal curve and let IC be its ideal sheaf in Y, so that we have a short exact sequence

0IC𝒪Y𝒪C0

in Coh(Y). Let now

0TICF0

be the unique exact sequence with respect to the torsion pair (𝒯p,p). It follows that F[1] is the perverse cokernel of 𝒪Y𝒪C.

We also have a short exact sequence

0𝒪Y(-D)IC𝒪D(-C)0.

Since we have 𝒪D(-C)p, the surjection IC𝒪D(-C) factors through a surjection F𝒪D(-C). Hence the support of F is two-dimensional.

Similarly, we have two perverse Hilbert schemes: Hilbch1p and Hilb1p. The first parameterizes perverse quotients 𝒪YE with ch0(E)=0=ch1(E), while the second parameterizes quotients 𝒪YE where the dimension of the support of E is at most one. As a consequence, we introduce partial invariants DT by integrating 𝒦1 or, equivalently, by taking the weighted Euler characteristic of Hilb1(Y).

2 Differences

We proceed here by detailing how [6] was modified to obtain [5] (we will omit a few minor changes which have no impact on the mathematical content).

  1. For organization purposes, we moved Lemma 3.2 to [5, Lemma 1.4] and added [5, Lemma 1.5]. The latter makes it clear that the subcategory 1p[1]𝒜1p is closed under quotients and extensions.

  2. Section 2 can be left untouched.

  3. In [5], we added Remark 3.5 to explain why the element 𝒦1 is necessary.

  4. In the identity (3.4), 1 should be replaced by 𝒦1, cf. [5, (3.6)].

  5. The definitions of the stacks 𝔐R and 𝔑 need to be changed: one must require in both cases the morphism 𝒪YT in the displayed diagram to have perverse cokernel in 1p[1].

  6. The proof of Proposition 3.5 needs to be modified slightly (by including an application of the snake lemma, cf. [5, Proposition 3.10]).

  7. In the identity prior to Section 3.6, one should replace 1 by 𝒦1.

  8. In the statement of Proposition 3.15, 1 should be replaced by 𝒦1. Similarly, in its proof Hilb should be replaced by Hilb, cf. [5, Proposition 3.21].

  9. Similarly, in the first identity of Section 3.7, 1 should be replaced by 𝒦1.

  10. Remark 3.21 should be extended to point out that it holds ditto for DT(Y).

From here on out, we should introduce the notation DT(Y/X) for consistency with DT(Y) and DT(Y), cf. [5, Remark 3.28]. Namely, DT(Y/X) comes from integrating Hilbch1p(Y/X) while DT(Y/X) comes from Hilb1p(Y/X). From [6, Remark 3.21] onwards, one should replace DT(Y/X) with DT(Y/X). Similarly, 𝒦1 should replace 1 in all Hall algebra identities.

Finally, [5] contains a new section where we investigate what happens when we restrict to curve classes contracted by f.

3 One-dimensional singular locus

Recall our general setup.

Situation 3.1

Fix a smooth and projective variety Y of dimension three, over , with trivial canonical bundle ωY𝒪Y and satisfying H1(Y,𝒪Y)=0. Fix a map f:YX satisfying the following properties:

  1. f is birational and its fibres are at most one-dimensional;

  2. X is projective and Gorenstein;

  3. Rf*𝒪Y=𝒪X.

As we have remarked earlier the category 𝒜1p, consisting of those E𝒜p with dimsuppE1, is not closed under quotients. This fact is the core reason why we had to replace with 𝒦 and is what causes the appearance of the “partial” DT numbers.

It is not clear whether there is a compact formula in the Hall algebra relating p with . Any approach seems to involve dealing with surface classes contracted by f. To complicate matters further, the basic identity (in H) 1𝒜p𝒪=1p[1]𝒪*1𝒯p𝒪 does not even hold in the full Hall algebra: given E𝒜p, together with its torsion and torsion-free parts F[1] and T, there is an exact sequence

0Hom(𝒪Y,F[1])Hom(𝒪Y,E)Hom(𝒪Y,T)Hom(𝒪Y,F[2])

where the last group is equal to H2(Y,F)=H1(X,R1f*F). This group vanishes when F1p (this assumption, in conjunction with f*F=0, forces the support of F to be a union of curves contracted to points, hence the support of R1f* is zero-dimensional), but in general it may not be the case.

This being said, let us come to the good news. If we restrict to the subcategory 𝒜excp then we can work around these obstacles.

Lemma 3.2

Let EAp be such that ch0(E)=ch1(E)=0 and dimsuppRf*E=0. Then dimsuppE1, in other words EA1p.

In other words, given EAp with Rf*E a skyscraper, EA1p if and only if ch0(E)=ch1(E)=0 (i.e. for these complexes, being supported in dimension at most one is a condition on their Chern characters).

Before we prove this lemma, we recall the key technical result of Van den Bergh [1, Lemmas 3.1.3, 3.1.5].

Lemma 3.3

Lemma 3.3 (Van den Bergh)

Consider the counit morphism f*f*TT. The objects in T-1 are precisely those TCoh(Y) such that f*f*TT is surjective.

Given FCoh(Y), there is a canonical map ϕF:FH-1(f!R1f*F). The objects in F0 are precisely those FCoh(Y) such that ϕF is injective.

Proof of Lemma 3.2.

Let us now prove that a perverse coherent sheaf E satisfying our assumptions is actually supported on a curve. Let T=H0(E) and F=H-1(E). As Rf*E is a skyscraper sheaf, it follows that both f*T and R1f*F are skyscraper sheaves as well.

As [E]=[T]-[F] in K0(Y) and ch0(E)=ch1(E)=0, it follows that T is supported in dimension at most one if and only if F is. When the perversity is p=-1, we have that f-1(suppf*T)=suppf*f*TsuppT. But, as f*T is a skyscraper sheaf and the fibres of f are at most one-dimensional, we have dimsuppf*f*T1 and we can conclude.

When the perversity is p=0, we have

suppFsuppH-1(f!R1f*F)suppf!R1f*Ff-1(suppR1f*F).

Again, as R1f*F is a skyscraper sheaf, we are done. ∎

What truly makes the category 𝒜excp robust is the following lemma.

Lemma 3.4

The category Aexcp is closed under extensions, quotients and subobjects.

Proof.

Let ABC be a short exact sequence in 𝒜p. First of all, Rf*B is a skyscraper if and only if both Rf*A and Rf*C are skyscraper sheaves. As [B]=[A]+[C] in K0(𝒜p), it follows from Lemma 3.2 that 𝒜excp is closed under extensions.

Thus we are left to show that if B𝒜excp then A,C𝒜excp. Consider the long exact sequence of cohomology sheaves.

0H-1(A)H-1(B)H-1(C)H0(A)H0(B)H0(C)0.

As B𝒜excp it follows that H-1(A) and H0(C) are both supported in dimension at most one. Thus the only obstruction to concluding is the support of either H-1(C) or H0(A). However, we know that both R1f*H-1(C) and f*H0(A) are skyscraper sheaves. Using Van den Bergh’s lemma, we conclude that at least one is (and hence both are) supported in dimension at most one. ∎

Consequently, Section 3 of [6] can be adapted to the category 𝒜excp without needing any “partial” invariants.

Theorem 3.5

Assume Situation 3.1. Then

DT¯excp(Y/X)=DT¯excDT¯exc(Y)DT0(Y)

holds, where

DT¯excp(Y/X)=β,nf*β=0DT¯Y/X(β,n)q(β,n),DT¯Y/X(β,n)=χμ(HilbY/Xp(β,n)).

Acknowledgements

We would like to thank Jørgen Rennemo for spotting the mistake in [6] and an anonymous referee for very useful comments.

References

[1] Van den Bergh M., Three-dimensional flops and noncommutative rings, Duke Math. J. 122 (2004), 423–455. 10.1215/S0012-7094-04-12231-6Suche in Google Scholar

[2] Bryan J., Cadman C. and Young B., The orbifold topological vertex, Adv. Math. 229 (2012), 531–595. 10.1016/j.aim.2011.09.008Suche in Google Scholar

[3] Calabrese J., On the crepant resolution conjecture for Donaldson–Thomas invariants, preprint 2012, http://arxiv.org/abs/1206.6524. 10.1090/jag/660Suche in Google Scholar

[4] Calabrese J., Donaldson–Thomas invariants and flops, preprint 2014, http://arxiv.org/abs/1111.1670v4. 10.1515/crelle-2014-0017Suche in Google Scholar

[5] Calabrese J., Donaldson–Thomas invariants and flops, preprint 2014, http://arxiv.org/abs/1111.1670v5. 10.1515/crelle-2014-0017Suche in Google Scholar

[6] Calabrese J., Donaldson–Thomas invariants and flops, J. reine angew. Math. 716 (2016), 103–145. 10.1515/crelle-2014-0017Suche in Google Scholar

Received: 2014-12-14
Revised: 2015-3-13
Published Online: 2015-7-18
Published in Print: 2017-3-1

© 2017 by De Gruyter

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