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Exceptional collections on Σ2\Sigma_{2}

Akira Ishii Graduate School of Mathematics, Nagoya University, Furocho, Chikusa-ku, Nagoya, 464-8602, Japan [email protected] Shinnosuke Okawa Department of Mathematics, Graduate School of Science, Osaka University
1-1, Machikaneyamacho, Toyonaka, Osaka 560-0043, Japan
[email protected]
 and  Hokuto Uehara Department of Mathematical Sciences, Graduate School of Science, Tokyo Metropolitan University, 1-1 Minamiohsawa, Hachioji-shi, Tokyo, 192-0397, Japan [email protected]
Abstract.

Structure theorems for exceptional objects and exceptional collections of the bounded derived category of coherent sheaves on del Pezzo surfaces are established by Kuleshov and Orlov in [MR1286839]. In this paper we propose conjectures which generalize these results to weak del Pezzo surfaces. Unlike del Pezzo surfaces, an exceptional object on a weak del Pezzo surface is not necessarily a shift of a sheaf and is not determined by its class in the Grothendieck group. Our conjectures explain how these complications are taken care of by spherical twists, the categorification of (2)(-2)-reflections acting on the derived category.

This paper is devoted to solving the conjectures for the prototypical weak del Pezzo surface Σ2\Sigma_{2}, the Hirzebruch surface of degree 22. Specifically, we prove the following results: Any exceptional object is sent to the shift of the uniquely determined exceptional vector bundle by a product of spherical twists which acts trivially on the Grothendieck group of the derived category. Any exceptional collection on Σ2\Sigma_{2} is part of a full exceptional collection. We moreover prove that the braid group on 4 strands acts transitively on the set of exceptional collections of length 44 (up to shifts).

1. Introduction

Semiorthogonal decomposition is among the most fundamental notions of triangulated categories. The finest ones, i.e., semiorthogonal decompositions whose components are equivalent to the bounded derived category of a point, are identified with (full) exceptional collections of the triangulated category. If there is an exceptional collection in a triangulated category, then virtually always there are infinitely many of them because of the group action explained below. Hence the classification of exceptional collections is not obvious at all.

Let XX be a smooth projective variety and 𝐃(X)\mathbf{D}(X) be the bounded derived category of coherent sheaves on XX. Concerning the classification of the exceptional collections of 𝐃(X)\mathbf{D}(X), the prototypical results are given in [Gorodentsev_1987, Section 5] for X=2X=\mathbb{P}^{2}. The similar results for X=1×1X=\mathbb{P}^{1}\times\mathbb{P}^{1} are given in [MR966985]. Based on these works, Kuleshov and Orlov established in [MR1286839] the similar results for arbitrary del Pezzo surfaces (see also [MR2108443, Corollary 4.3.2, Theorem 4.3.3, Theorem 4.6.1]). They are summarized as follows.

Theorem 1.1 ([MR1286839]).

Let XX be a del Pezzo surface over an algebraically closed field 𝐤\mathbf{k}.

  1. (1)

    Any exceptional object 𝐃(X)\mathcal{E}\in\mathbf{D}(X) is either a vector bundle or a line bundle on a (1)(-1)-curve, up to shifts.

  2. (2)

    The isomorphism class of an exceptional object 𝐃(X)\mathcal{E}\in\mathbf{D}(X) is determined by its class []K0(X)[\mathcal{E}]\in\operatorname{K_{0}}\left(X\right), up to shifts by 22\mathbb{Z}.

  3. (3)

    Any exceptional collection of 𝐃(X)\mathbf{D}(X) can be extended to a full exceptional collection.

  4. (4)

    Conjecture 1.2 below is true for XX; i.e., the action Gr𝖤𝖢r(X)G_{r}\curvearrowright\mathsf{EC}_{r}(X) is transitive.

The symbol K0(X)\operatorname{K_{0}}\left(X\right) denotes the Grothendieck group of the triangulated category 𝐃(X)\mathbf{D}(X). We briefly explain (4). Let 𝖤𝖢r(X)\mathsf{EC}_{r}(X) denote the set of isomorphism classes of exceptional collections of length rr of 𝐃(X)\mathbf{D}(X), where r=rankK0(X)r=\operatorname{rank}\operatorname{K_{0}}\left(X\right). An important fact relevant to the classification is that there is a standard action of the group GrrBrrG_{r}\coloneqq\mathbb{Z}^{r}\rtimes\operatorname{Br}_{r} on 𝖤𝖢r(X)\mathsf{EC}_{r}(X) by shifts and mutations, where Brr\operatorname{Br}_{r} is the braid group on rr strands (see Section LABEL:sc:Deformation_and_mutation_of_exceptional_collections for details).

Inspired by the earlier works mentioned above, Bondal and Polishchuk gave the following conjecture.

Conjecture 1.2 (==[MR1230966, Conjecture 2.2]).

Suppose that XX is a smooth projective variety such that 𝐃(X)\mathbf{D}(X) admits a full exceptional collection of length rr. Then the action Gr𝖤𝖢r(𝐃(X))G_{r}\curvearrowright\mathsf{EC}_{r}(\mathbf{D}(X)) is transitive.

In dimensions greater than 22, the classification of exceptional collections is widely open. Even for 3\mathbb{P}^{3}, only partial results seem to be known ([1995alg.geom..7014P]) and Conjecture 1.2 is still open.

The aim of this paper is to investigate the generalization of Theorem 1.1 to weak del Pezzo surfaces; i.e., smooth projective surfaces XX whose anti-canonical bundle ωX1\omega_{X}^{-1} is nef and big. As it turns out, the generalization is not straightforward at all.

A weak del Pezzo surface XX which is not a del Pezzo surface admits at least one (and only finitely many) (2)(-2)-curve(s); i.e., a smooth curve CXC\subset X with C2=2C^{2}=-2 and C1C\simeq\mathbb{P}^{1}. Line bundles on CC, as objects of 𝐃(X)\mathbf{D}(X), are 22-spherical objects and hence yield non-trivial autoequivalences of 𝐃(X)\mathbf{D}(X) called spherical twists due to Seidel and Thomas [Seidel-Thomas]. For a 22-spherical object α𝐃(X)\alpha\in\mathbf{D}(X), the corresponding spherical twist TαT_{\alpha} acts as a reflection on K0(X)\operatorname{K_{0}}\left(X\right) whereas it always satisfies Tα2id𝐃(X)T_{\alpha}^{2}\not\simeq\operatorname{id}_{\mathbf{D}(X)}. For example, the exceptional object T𝒪C2(𝒪X)T_{\mathcal{O}_{C}}^{2}(\mathcal{O}_{X}) has the same class as 𝒪X\mathcal{O}_{X} in K0(X)\operatorname{K_{0}}\left(X\right) but is not isomorphic to 𝒪X\mathcal{O}_{X}. In fact, by direct computation one can confirm the following.

i(T𝒪C2(𝒪X)){𝒪Xi=0𝒪Ci=1,20otherwise\displaystyle\mathcal{H}^{i}\left(T_{\mathcal{O}_{C}}^{2}(\mathcal{O}_{X})\right)\simeq\begin{cases}\mathcal{O}_{X}&i=0\\ \mathcal{O}_{C}&i=1,2\\ 0&\text{otherwise}\end{cases} (1.1)

Moreover, by applying T𝒪C2T_{\mathcal{O}_{C}}^{2} repeatedly, we obtain a collection of infinitely many exceptional objects of unbounded cohomological amplitudes which share the same class in K0(X)\operatorname{K_{0}}\left(X\right). Hence Theorem 1.1 (1) (2) are not true for XX at all.

Conjecture 1.3, which is the main conjecture of this paper, generalizes Theorem 1.1 to weak del Pezzo surfaces while taking into account all the complications mentioned in the previous paragraph. In a word, it asserts that the failure of Theorem 1.1 (1) (2) on weak del Pezzo surfaces is remedied by spherical twists and that Theorem 1.1 (3) (4) should hold for weak del Pezzo surfaces too. The main theorem of this paper is that Conjecture 1.3 is true for Σ2=1(𝒪𝒪(2))\Sigma_{2}=\mathbb{P}_{\mathbb{P}^{1}}(\mathcal{O}\oplus\mathcal{O}(2)); namely, the Hirzebruch surface of degree 22, a paradigm of weak del Pezzo surfaces. In fact we formulated Conjecture 1.3 by generalizing the results we obtained for Σ2\Sigma_{2}, Theorem 1.1, and [MR3758518, Theorem 1.2] simultaneously.

Conjecture 1.3.

Let XX be a weak del Pezzo surface over an algebraically closed field 𝐤\mathbf{k}.

  1. (1)

    For any exceptional object 𝐃(X)\mathcal{E}\in\mathbf{D}(X), there exists a sheaf \mathcal{F} on XX which is either an exceptional vector bundle or a line bundle on a (1)(-1)-curve, a sequence of line bundles on (2)(-2)-curves 1,,n\mathcal{L}_{1},\dots,\mathcal{L}_{n}, and an integer mm\in\mathbb{Z} such that

    (TnT1)()[m].\displaystyle\mathcal{E}\simeq(T_{\mathcal{L}_{n}}\circ\cdots\circ T_{\mathcal{L}_{1}})(\mathcal{F})[m]. (1.2)
  2. (2)

    For any pair of exceptional objects ,𝐃(X)\mathcal{E},\mathcal{E}^{\prime}\in\mathbf{D}(X) such that []=[]K0(X)[\mathcal{E}]=[\mathcal{E}^{\prime}]\in\operatorname{K_{0}}\left(X\right), there are a product bb of spherical twists and inverse spherical twists which acts trivially on K0(X)\operatorname{K_{0}}\left(X\right) and m2m\in 2\mathbb{Z} such that b()[m]\mathcal{E}^{\prime}\simeq b(\mathcal{E})[m]. Moreover, for each exceptional object 𝐃(X)\mathcal{E}\in\mathbf{D}(X), there is a unique exceptional vector bundle \mathcal{F} such that either []=[][\mathcal{E}]=[\mathcal{F}] or []=[][\mathcal{E}]=-[\mathcal{F}] holds.

  3. (3)

    Any exceptional collection on XX can be extended to a full exceptional collection.

  4. (4)

    Conjecture 1.2 is true for XX.

As it is more or less visible, (1), (2), (3), and (4) of Conjecture 1.3 generalizes (1), (2), (3), and (4) of Theorem 1.1, respectively.

To avoid repetition, let us simply state the main result of this paper as follows.

Theorem 1.4 (MAIN THEOREM).

Conjecture 1.3 is true for X=Σ2X=\Sigma_{2}.

More specifically, for X=Σ2X=\Sigma_{2}

  • Conjecture 1.3 (1) is solved affirmatively in Section LABEL:sc:Twisting_exceptional_objects_down_to_exceptional_vector_bundles as Theorem LABEL:th:exceptional_objects_are_equivalent_to_vector_bundles.

  • Conjecture 1.3 (2) is solved affirmatively in Section LABEL:sc:Exceptional_objects_sharing_the_same_class as Corollary LABEL:cr:exceptional_objects_in_the_same_numerical_class.

  • Conjecture 1.3 (3) is solved affirmatively in Section LABEL:sc:Constructibility_of_exceptional_collections as Corollary LABEL:cr:constructibility.

  • Conjecture 1.3 (4) is solved affirmatively in Section LABEL:sc:Braid_group_acts_transitively_on_the_set_of_full_exceptional_collections as Theorem LABEL:th:transitivity.

Remark 1.5.

We give some comments on the preceding works which are related to Conjecture 1.3 and Theorem 1.4, and one important consequence of Conjecture 1.3 (4) on the fullness of exceptional collections of maximal length.

  • This paper is a continuation of [MR3431636] by the 2nd and the 3rd authors and almost completely supersedes it. Conjecture 1.3 (1) for Σ2\Sigma_{2} is stated as [MR3431636, Conjecture 1.3], and is solved for exceptional sheaves in [MR3431636, Theorem 1.4].

  • Conjecture 1.3 (1) for torsion exceptional sheaves is partially solved in [MR3758518, Theorem 1.2]. A weaker version of Conjecture 1.3 (1) is stated as [MR3758518, Conjecture 1.1].

  • Exceptional objects and exceptional collections of vector bundles on weak del Pezzo surfaces is systematically studied in [MR1604186]. In fact we use some results of this work in this paper.

  • It follows from the definition of mutations that the triangulated subcategory generated by an exceptional collection is invariant under mutation. In particular, the fullness of an exceptional collection is preserved by mutations. On the other hand, any XX as in Conjecture 1.3 admits a full exceptional collection. Hence Conjecture 1.3 (4) would imply that any exceptional collection of length equal to rankK0(X)=rankPic(X)+2\operatorname{rank}\operatorname{K_{0}}\left(X\right)=\operatorname{rank}\operatorname{Pic}(X)+2 of 𝐃(X)\mathbf{D}(X) is full, though it would also follow from Conjecture 1.3 (3).

1.1. Summary of each section and structure of the paper

Section 2 is a preliminary section. We recall the rudiments of mutations and the group BB of autoequivalences generated by spherical twists from [Ishii-Uehara_ADC]. Among others, we prove in Corollary LABEL:cr:btriv_is_generated_by_squares that BK0𝗍𝗋𝗂𝗏B^{K_{0}-\mathsf{triv}}, the subgroup of BB acting trivially on K0(Σ2)\operatorname{K_{0}}\left(\Sigma_{2}\right), is generated by squares of spherical twists by line bundles on CC.

From Section LABEL:sc:Twisting_exceptional_objects_down_to_exceptional_vector_bundles till the end of the paper, we restrict ourselves to the proof of Theorem 1.4 and in particular discuss the case of Σ2\Sigma_{2} only.

Section LABEL:sc:Twisting_exceptional_objects_down_to_exceptional_vector_bundles is the main component of the paper and devoted to the proof of Theorem LABEL:th:exceptional_objects_are_equivalent_to_vector_bundles. Namely, in this section, we prove that for each exceptional object 𝐃(Σ2)\mathcal{E}\in\mathbf{D}(\Sigma_{2}) there is a sequence of integers a1,,ana_{1},\dots,a_{n} such that (TanTa1)()\left(T_{a_{n}}\circ\cdots\circ T_{a_{1}}\right)(\mathcal{E}) is isomorphic to a shift of a vector bundle. In accordance with the steps of the proof, Section LABEL:sc:Twisting_exceptional_objects_down_to_exceptional_vector_bundles is divided into six subsections.

In Section LABEL:sc:First_properties we prove some properties of the cohomology sheaf ()=ii()\mathcal{H}^{\bullet}(\mathcal{E})=\bigoplus_{i\in\mathbb{Z}}\mathcal{H}^{i}(\mathcal{E}). Among others we show that there is the index i0i_{0}\in\mathbb{Z} such that Suppi0()=Σ2\operatorname{Supp}\mathcal{H}^{i_{0}}(\mathcal{E})=\Sigma_{2} and for any ii0i\neq i_{0} the cohomology sheaf i()\mathcal{H}^{i}(\mathcal{E}), if not 0, is a pure sheaf whose reduced support is CC. Then in Section LABEL:sc:Properties_of_the_schematic_support, we prove that actually the schematic support of i()\mathcal{H}^{i}(\mathcal{E}) for ii0i\neq i_{0} is CC. This is the most technical part of the paper, and actually this had been the main obstacle for the whole work. Fortunately one can use the result of this subsection as a black box to read the rest of the paper.

In Section LABEL:sc:More_on_the_structure we prove that there is a decomposition i0()TE\mathcal{H}^{i_{0}}(\mathcal{E})\simeq T\oplus E, where E=E()E=E(\mathcal{E}) is an exceptional sheaf and TT is a torsion sheaf. We moreover show that if torsE0\operatorname{tors}E\neq 0, then TT is a direct sum of copies of 𝒪C(a)\mathcal{O}_{C}(a) for some aa\in\mathbb{Z} and that tors()\operatorname{tors}\mathcal{H}^{\bullet}(\mathcal{E}) is a direct sum of copies of 𝒪C(a)\mathcal{O}_{C}(a) and 𝒪C(a+1)\mathcal{O}_{C}(a+1). This integer a=a()a=a(\mathcal{E}) plays a central role throughout the paper.

In Section LABEL:sc:Derived_dual_of_exceptional_objects we investigate the relationship between the cohomology sheaves of \mathcal{E} and those of \mathcal{E}^{\vee}, the derived dual of \mathcal{E}. We in particular show in Corollary LABEL:cr:E(cE_vee)_has_non-trivial_torsion that if \mathcal{E} is not isomorphic to a shift of a vector bundle and torsE()=0\operatorname{tors}E(\mathcal{E})=0, then torsE()0\operatorname{tors}E(\mathcal{E}^{\vee})\neq 0. In this paper we mainly discuss the case torsE()0\operatorname{tors}E(\mathcal{E})\neq 0, and by this result we can settle the case where torsE()=0\operatorname{tors}E(\mathcal{E})=0 by passing to \mathcal{E}^{\vee}.

In Section LABEL:sc:Length_of_the_torsion_part we introduce the notion of the length of the “torsion part” of an object at the generic point γ\gamma of CC. Formally speaking, for \mathcal{E} it is defined as ()=ilength𝒪Σ2,γtorsi()γ\ell(\mathcal{E})=\sum_{i\in\mathbb{Z}}\operatorname{length}_{\mathcal{O}_{\Sigma_{2},\gamma}}\operatorname{tors}\mathcal{H}^{i}(\mathcal{E})_{\gamma}. It follows that \mathcal{E} is isomorphic to a shift of a vector bundle if and only if ()=0\ell(\mathcal{E})=0, and hence it suffices to show that (Tc())<()\ell(T_{c}(\mathcal{E}))<\ell(\mathcal{E}) for some c=c()c=c(\mathcal{E})\in\mathbb{Z} if ()>0\ell(\mathcal{E})>0. This is exactly what we achieve in Section LABEL:sc:Proof_of_Theorem_3.1. We show in Theorem LABEL:th:decrease_the_length_by_appropriate_twist that c=a()c=a(\mathcal{E}) works if torsE()0\operatorname{tors}E(\mathcal{E})\neq 0 and otherwise c=a()3c=-a(\mathcal{E}^{\vee})-3 does.

Spherical objects on the minimal resolution of type AA singularity is classified in [Ishii-Uehara_ADC]. More specifically, the proof of Theorem LABEL:th:exceptional_objects_are_equivalent_to_vector_bundles is an adaptation of the proof of [Ishii-Uehara_ADC, Proposition 5.1]. It is, however, much more involved than that of [Ishii-Uehara_ADC, Proposition 5.1]. This is due to the fact that the support of an exceptional object on Σ2\Sigma_{2} is never concentrated in the (2)(-2)-curve CC. On the contrary the reduced support of a spherical object on Σ2\Sigma_{2} is concentrated in CC, and it immediately implies that the schematic supports of the cohomology sheaves of the spherical object coincide with CC.

Section LABEL:sc:Exceptional_objects_sharing_the_same_class is devoted to the proof of Theorem LABEL:th:exceptional_object_is_K0-trivial_equivalent_to_vector_bundle. It is almost immediately obtained by combining Theorem LABEL:th:exceptional_objects_are_equivalent_to_vector_bundles with a small trick on squares of spherical twists (Proposition LABEL:pr:TaTb_as_product_of_O_(m_C_)_and_squares_of_twists) and the fact that an exceptional vector bundle is uniquely determined by its class in K0(Σ2)\operatorname{K_{0}}\left(\Sigma_{2}\right) (Lemma LABEL:lm:exceptional_vb_is_determined_by_K0).

Section LABEL:sc:Constructibility_of_exceptional_collections is devoted to the proof of Corollary LABEL:cr:constructibility. Take an exceptional collection ¯\underline{\mathcal{E}}. We first show in Theorem LABEL:th:twisting_exceptional_collection_to_vector_bundles that there is a product of spherical twists bb such that b(¯)b(\underline{\mathcal{E}}) consists of vector bundles up to shifts. This is achieved in a one-by-one manner. The key is that if (,)(\mathcal{B},\mathcal{E}) is an exceptional pair such that \mathcal{B} is a vector bundle and ()>0\ell(\mathcal{E})>0, then, surprisingly enough, Tc()()T_{c(\mathcal{E})}(\mathcal{B}) remains to be a vector bundle (though it may not be isomorphic to \mathcal{B}). Recall that c()c(\mathcal{E})\in\mathbb{Z} depends only on \mathcal{E} and that Tc()T_{c(\mathcal{E})} strictly decreases the length of \mathcal{E}.

Corollary LABEL:cr:constructibility is known for exceptional collections of vector bundles by a slight generalization Theorem LABEL:th:Constructibility_for_bundle_collections of a result by Kuleshov in [MR1604186]. Applying it to b(¯)b(\underline{\mathcal{E}}), we immediately obtain the proof of Corollary LABEL:cr:constructibility for ¯\underline{\mathcal{E}}.

Section LABEL:sc:Braid_group_acts_transitively_on_the_set_of_full_exceptional_collections is devoted to the proof of Theorem LABEL:th:transitivity. We use the deformation of Σ2\Sigma_{2} to 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}. The difficulty is that there are infinitely many exceptional objects on Σ2\Sigma_{2} which deform to the same exceptional object on 1×1\mathbb{P}^{1}\times\mathbb{P}^{1} (non-uniqueness of the specialization, which is translated into the non-separatedness of the moduli space of semiorthogonal decompositions introduced in [2020arXiv200203303B]). Actually, two exceptional objects have the same deformation to 1×1\mathbb{P}^{1}\times\mathbb{P}^{1} if and only if they have the same class in K0(Σ2)\operatorname{K_{0}}\left(\Sigma_{2}\right) (up to shifts by 22\mathbb{Z}).

In Step LABEL:st:reduction_to_numerically_standard_collection of the proof, we use the fact that the corresponding result is already known by Theorem 1.1 (4) for the del Pezzo surface 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}. Since deformation of exceptional collections commutes with mutations, the result for 1×1\mathbb{P}^{1}\times\mathbb{P}^{1} immediately implies that for any exceptional collection of length 44 on Σ2\Sigma_{2} there is a sequence of mutations which brings it to a collection which is numerically equivalent to the standard collection 𝗌𝗍𝖽\mathcal{E}^{\mathsf{std}} (i.e., having the same classes as 𝗌𝗍𝖽\mathcal{E}^{\mathsf{std}} in K0(Σ2)\operatorname{K_{0}}\left(\Sigma_{2}\right). See (LABEL:eq:standard_collection) for the definition of 𝗌𝗍𝖽\mathcal{E}^{\mathsf{std}}).

It remains to show that an exceptional collection ¯\underline{\mathcal{E}} on Σ2\Sigma_{2} which is numerically equivalent to 𝗌𝗍𝖽\mathcal{E}^{\mathsf{std}} can be sent to 𝗌𝗍𝖽\mathcal{E}^{\mathsf{std}} by mutations. In Step LABEL:st:from_numerically_standard_to_standard, as an intermediate step, we find bBb\in B such that ¯=b(𝗌𝗍𝖽)\underline{\mathcal{E}}=b(\mathcal{E}^{\mathsf{std}}). We construct such bb again in one-by-one manner.

In Step LABEL:st:replace_b_with_mutations we prove that bb can be replaced by a sequence of mutations. Thanks to the fact that mutations commute with autoequivalences, it is enough to show the assertion only for b{T0,T1}b\in\{T_{0},T_{-1}\}. Recall that T0,T1T_{0},T_{-1} generate BB. At this point the problem is concrete enough to be settled by hand.

1.2. Some words on future directions

Though Conjecture 1.3 is stated for arbitrary weak del Pezzo surfaces, in this paper we restrict ourselves to the study of the case of Σ2\Sigma_{2}. This is partly because the proof is rather involved already in this case. We nevertheless think that the case of Σ2\Sigma_{2} should serve as a paradigm for the further investigations of Conjecture 1.3.

The proof of Theorem 1.4 is based on the classification of rigid sheaves on the (2)(-2)-curve; i.e., the fundamental cycle of the minimal resolution of the A1A_{1}-singularity. So far such classification is achieved only for the minimal resolution of type AA singularities by [Ishii-Uehara_ADC]. If one wants to push the strategy of this paper, it seems inevitable to establish the similar classification for the minimal resolution of type DD and type EE singularities. See [MR3983387] for results in this direction.

A weak del Pezzo surface over an algebraically closed field 𝐤\mathbf{k} is isomorphic to either 1×1,Σ2\mathbb{P}^{1}\times\mathbb{P}^{1},\Sigma_{2}, or a blowup of 2\mathbb{P}^{2} in at most eight points in almost general positions (see, say, [MR2964027, Theorem 8.1.15, Corollary 8.1.24]). Hence our strategy based on the deformation to del Pezzo surfaces, in principle, is applicable to all weak del Pezzo surfaces.

Structure theorems for exceptional collections on 2\mathbb{P}^{2} play an important role in showing the contractibility of (the main component of) the space of Bridgeland stability conditions Stab(2)\operatorname{Stab}(\mathbb{P}^{2}) in [MR3703470]. Our results should be similarly useful for studying Stab(Σ2)\operatorname{Stab}(\Sigma_{2}). More specifically, they should be very closely related to the relationship between Stab(Σ2)\operatorname{Stab}(\Sigma_{2}) and Stab(1×1)\operatorname{Stab}(\mathbb{P}^{1}\times\mathbb{P}^{1}); see Remark LABEL:rm:stability_conditions for details.

1.3. Notation and convention

We work over an algebraically closed field 𝐤\mathbf{k}, unless otherwise stated. To ease notation, we will write exti=dim𝐤Exti,hi=dim𝐤Hi,ep,q2=dim𝐤E2p,q,\operatorname{ext}^{i}=\dim_{\mathbf{k}}\operatorname{Ext}^{i},h^{i}=\dim_{\mathbf{k}}H^{i},e^{p,q}_{2}=\dim_{\mathbf{k}}E_{2}^{p,q}, and so on. Below is a list of frequently used symbols.

Σd\Sigma_{d} the Hirzebruch surface of degree dd (2.1)
CC the (2)(-2)-curve of Σ2\Sigma_{2}
ff the divisor class of a fiber of the morphism Σ21\Sigma_{2}\to\mathbb{P}^{1} (2.4)
\ast^{\vee} the derived dual of 𝐃(Σ2)\ast\in\mathbf{D}(\Sigma_{2}) (2.6)
Ta(resp. Ta)Auteq(Σ2)T_{a}\ (\text{resp. }T^{\prime}_{a})\in\operatorname{Auteq}(\Sigma_{2}) the (inverse) spherical twist by 𝒪C(a)\mathcal{O}_{C}(a) (2.15)
B<Auteq(Σ2)B<\operatorname{Auteq}(\Sigma_{2}) the group of autoequivalences generated by spherical twists (Definition LABEL:df:subgroup_of_spherical_twists)
𝖤𝖢N,𝖤𝖢𝖵𝖡N,𝖥𝖤𝖢,𝖥𝖤𝖢𝖵𝖡\mathsf{EC}_{N},\mathsf{ECVB}_{N},\mathsf{FEC},\mathsf{FECVB} various sets of exceptional collections (Definition LABEL:df:sets_of_exceptional_collections)
BrN\operatorname{Br}_{N} (resp. GNG_{N}) the braid group on NN strands (LABEL:eq:braid_group) (resp. the extension of BrN\operatorname{Br}_{N} by N\mathbb{Z}^{N} (LABEL:equation:GN))
𝗀𝖾𝗇\operatorname{\mathsf{gen}} the generalization map for exceptional collections from the central fiber to the generic fiber (LABEL:eq:generalization_map)
𝗇𝗎𝗆𝖤𝖢N,𝗇𝗎𝗆𝖥𝖤𝖢\mathsf{numEC}_{N},\mathsf{numFEC} various sets of numerical exceptional collections (Definition LABEL:df:numerical_exceptional_collection)
𝗌𝗍𝖽𝖥𝖤𝖢𝖵𝖡(Σ2)\mathcal{E}^{\mathsf{std}}\in\mathsf{FECVB}(\Sigma_{2}) the standard full exceptional collection of 𝐃(Σ2)\mathbf{D}(\Sigma_{2}) (Definition LABEL:df:the_standard_exceptional_collection_on_Sigma2)
𝗌𝗍𝖽ξ𝖥𝖤𝖢𝖵𝖡(𝒳𝗀𝖾𝗇)\mathcal{E}^{\mathsf{std}}_{\xi}\in\mathsf{FECVB}(\mathcal{X}_{\operatorname{\mathsf{gen}}}) the standard full exceptional collection of 𝐃(𝒳𝗀𝖾𝗇)\mathbf{D}(\mathcal{X}_{\operatorname{\mathsf{gen}}}) (LABEL:eq:standard_collection_generic)
()(resp. i())\mathcal{H}^{\bullet}(\mathcal{E})\ (\text{resp. }\mathcal{H}^{i}(\mathcal{E})) the total (resp. ii-th) cohomology of 𝐃(X)\mathcal{E}\in\mathbf{D}(X) with respect to the standard t-structure (LABEL:eq:cohomology_object)
i0=i0()i_{0}=i_{0}(\mathcal{E}) the unique index such that Suppi0()=Σ2\operatorname{Supp}\mathcal{H}^{i_{0}}(\mathcal{E})=\Sigma_{2} (Definition LABEL:df:i0)
(R,𝔪)(R,\mathfrak{m}) the complete local ring of the A1A_{1}-singularity (Notation LABEL:nt:A1_singularity)
(0:I)MM(0:I)_{M}\subseteq M the maximal submodule of MM annihilated by the ideal IRI\subseteq R (LABEL:eq:annihilator)
C𝒪Σ2\mathcal{I}_{C}\subset\mathcal{O}_{\Sigma_{2}} the ideal sheaf of CΣ2C\subset\Sigma_{2} (LABEL:equation:cIC)
D()D(\ast) the dual 𝐤\mathbf{k}-vector space of \ast (LABEL:equation:k-dual)
i0()E()T()\mathcal{H}^{i_{0}}(\mathcal{E})\simeq E(\mathcal{E})\oplus T(\mathcal{E}) the canonical decomposition into an exceptional sheaf and a torsion sheaf (Lemma LABEL:lm:exceptional_sheaf_is_a_direct_summand)
𝒯(),()\mathcal{T}(\mathcal{E}),\ \mathcal{F}(\mathcal{E}) the torsion (resp. the torsion free) part of i0()\mathcal{H}^{i_{0}}(\mathcal{E}) (Definition LABEL:df:E_and_cF)
a,s,ta,s,t\in\mathbb{Z} integers specified by the irreducible decomposition of 𝒯\mathcal{T} (LABEL:eq:decomposition_of_cT) (see also Lemma LABEL:lm:exceptional_sheaf_is_a_direct_summand)
()\ell(\ast) “length of the torsion part of \ast” at the generic point γ\gamma of CC (Definition LABEL:df:length)
b,r,sb,r,s\in\mathbb{Z} integers specified by the irreducible decomposition of an exceptional vector bundle restricted to CC (Lemma LABEL:lm:exceptional_vector_bundle_restricted_to_C)

Acknowledgements

During the preparation of this paper, A.I. was partially supported by JSPS Grants-in-Aid for Scientific Research (19K03444). S.O. was partially supported by JSPS Grants-in-Aid for Scientific Research (16H05994, 16H02141, 16H06337, 18H01120, 20H01797, 20H01794). H.U. was partially supported by JSPS Grants-in-Aid for Scientific Research (18K03249).

2. Preliminaries

2.1. The Hirzebruch surfaces

The Hirzebruch surface of degree d0d\in\mathbb{Z}_{\geq 0} is the ruled surface

p:Σd1(𝒪1𝒪1(d))1.\displaystyle p\colon\Sigma_{d}\coloneqq\mathbb{P}_{\mathbb{P}^{1}}\left(\mathcal{O}_{\mathbb{P}^{1}}\oplus\mathcal{O}_{\mathbb{P}^{1}}(d)\right)\to\mathbb{P}^{1}. (2.1)

The history of Hirzebruch surfaces goes back, at least, to the first paper by Hirzebruch [MR45384]. An explicit isotrivial degeneration of Σd\Sigma_{d} to Σd\Sigma_{d^{\prime}} for d>dd>d^{\prime} and dd2d-d^{\prime}\in 2\mathbb{Z} is constructed in [MR153033, p.86 Example]. As a special case, there exists a smooth projective morphism (defined over Spec\operatorname{Spec}\mathbb{Z})

𝒳𝔸1t\displaystyle\mathcal{X}\to\mathbb{A}^{1}_{t} (2.2)

such that the fiber over t=0t=0 is isomorphic to Σ2\Sigma_{2} and the restriction of the family over the open subscheme 𝔾m𝔸1\mathbb{G}_{m}\hookrightarrow\mathbb{A}^{1} is isomorphic to the trivial family (1×1)×𝔾mpr2𝔾m\left(\mathbb{P}^{1}\times\mathbb{P}^{1}\right)\times\mathbb{G}_{m}\stackrel{{\scriptstyle\mathrm{pr}_{2}}}{{\to}}\mathbb{G}_{m}.

In this paper we investigate the bounded derived category of coherent sheaves on Σ2\Sigma_{2}, which is the most basic example of weak del Pezzo surfaces. We let CΣ2C\subset\Sigma_{2} denote the unique negative curve, and ff the (linear equivalence class of) the fiber of pp. Recall that

PicΣ2=Cf,\displaystyle\operatorname{Pic}\Sigma_{2}=\mathbb{Z}C\oplus\mathbb{Z}f, (2.3)

where

C2=2,f2=0,C.f=1.\displaystyle C^{2}=-2,f^{2}=0,C.f=1. (2.4)

The anti-canonical bundle is given by

KΣ2=2C+4f.\displaystyle-K_{\Sigma_{2}}=2C+4f. (2.5)

2.2. Derived category, spherical twist, and the autoequivalence group of Σ2\Sigma_{2}

Definition 2.1.

For a quasi-compact scheme YY, we let PerfY\operatorname{Perf}Y denote the perfect derived category of YY with the standard structure of a triangulated category. When YY is equipped with a morphism to Spec𝐤\operatorname{Spec}\mathbf{k}, we think of PerfY\operatorname{Perf}Y as a triangulated 𝐤\mathbf{k}-linear category. It comes with the natural symmetric monoidal structure given by the tensor product over 𝒪Y\mathcal{O}_{Y}, but we do not take it into account unless otherwise stated.

When YY is a smooth and projective variety over a field 𝐤\mathbf{k}, we identify PerfY\operatorname{Perf}Y with the bounded derived category 𝐃(Y)\mathbf{D}(Y) of coherent sheaves on YY.

The following equivalence of tensor triangulated categories

:(PerfY)opPerfY;omY(,𝒪Y)\displaystyle{}^{\vee}\colon\left(\operatorname{Perf}Y\right)^{\mathrm{op}}\xrightarrow{\sim}\operatorname{Perf}Y;\quad\mathcal{E}\mapsto\mathcal{E}^{\vee}\coloneqq\mathbb{R}\mathop{{\mathcal{H}}om}\nolimits_{Y}(\mathcal{E},\mathcal{O}_{Y}) (2.6)

will be called the derived dual.

One can easily verify that there exits a canonical natural isomorphism

id.\displaystyle\operatorname{id}\stackrel{{\scriptstyle\sim}}{{\Rightarrow}}{}^{\vee\vee}. (2.7)
Definition 2.2.

For smooth projective varieties X,YX,Y over Spec𝐤\operatorname{Spec}\mathbf{k} and an object K𝐃(X×𝐤Y)K\in\mathbf{D}(X\times_{\mathbf{k}}Y), the integral transform by the kernel KK will be denoted and defined as follows.

ΦKΦKXY:𝐃(X)𝐃(Y);EpY(pXEX×𝐤Y𝕃K)\displaystyle\Phi_{K}\coloneqq\Phi_{K}^{X\to Y}\colon\mathbf{D}(X)\to\mathbf{D}(Y);\quad E\mapsto\mathbb{R}p_{Y\ast}\left(p_{X}^{\ast}E\otimes_{X\times_{\mathbf{k}}Y}^{\mathbb{L}}K\right) (2.8)

Let XX be a smooth projective variety over a field 𝐤\mathbf{k}. Recall that an object α𝐃(X)\alpha\in\mathbf{D}(X) is spherical if α𝒪XωXα\alpha\otimes_{\mathcal{O}_{X}}\omega_{X}\simeq\alpha and HomX(α,α)𝐤𝐤[dimX]\mathop{\mathbb{R}\mathrm{Hom}}\nolimits_{X}(\alpha,\alpha)\simeq\mathbf{k}\oplus\mathbf{k}[-\dim X]. The spherical twist by α\alpha is the endofunctor

TαΦKα\displaystyle T_{\alpha}\coloneqq\Phi_{K_{\alpha}} (2.9)

defined by the kernel Kαcone(ααev𝒪ΔX)K_{\alpha}\coloneqq\operatorname{cone}\left(\alpha^{\vee}\boxtimes\alpha\xrightarrow{\operatorname{ev}}\mathcal{O}_{\Delta_{X}}\right).

Consider the exchange automorphism

𝗌𝗐𝖺𝗉:X×XX×X;(x,y)(y,x).\displaystyle\operatorname{\mathsf{swap}}\colon X\times X\to X\times X;\,(x,y)\mapsto(y,x). (2.10)

Recall that

(𝗌𝗐𝖺𝗉Kα)p1ωX[dimX]\displaystyle\left(\operatorname{\mathsf{swap}}^{*}K_{\alpha}\right)^{\vee}\otimes p_{1}^{\ast}\omega_{X}[\dim X] (2.11)

is called the right adjoint kernel of KαK_{\alpha} and it enjoys the following adjoint property (see, say, [MR2244106, Definition 5.7]).

Tα=ΦKαΦ(𝗌𝗐𝖺𝗉Kα)p1ωX[dimX]Tα\displaystyle T_{\alpha}=\Phi_{K_{\alpha}}\dashv\Phi_{\left(\operatorname{\mathsf{swap}}^{*}K_{\alpha}\right)^{\vee}\otimes p_{1}^{\ast}\omega_{X}[\dim X]}\eqqcolon T^{\prime}_{\alpha} (2.12)

It follows that TαT_{\alpha} is an autoequivalence, so that TαTα1T^{\prime}_{\alpha}\simeq T_{\alpha}^{-1}. Note that there exists the obvious isomorphism

𝗌𝗐𝖺𝗉KαKα,\displaystyle\operatorname{\mathsf{swap}}^{\ast}K_{\alpha}\simeq K_{\alpha^{\vee}}, (2.13)

so that

TαΦKαp1ωX[dimX].\displaystyle T^{\prime}_{\alpha^{\vee}}\simeq\Phi_{K_{\alpha}^{\vee}\otimes p_{1}^{\ast}\omega_{X}[\dim X]}. (2.14)

A typical example of a spherical object on Σ2\Sigma_{2} is 𝒪C(a)\mathcal{O}_{C}(a) for aa\in\mathbb{Z}. The corresponding (inverse) spherical twist will be denoted as follows, for short.

TaT𝒪C(a),TaT𝒪C(a)1\displaystyle T_{a}\coloneqq T_{\mathcal{O}_{C}(a)},\quad T^{\prime}_{a}\coloneqq T_{\mathcal{O}_{C}(a)}^{-1} (2.15)

By definition, for each spherical object α\alpha and any object E𝐃(X)E\in\mathbf{D}(X), there are standard triangles as follows. To ease notation, we simply let 𝒪X\otimes_{\mathcal{O}_{X}} denote the derived tensor product. The morphisms ε\varepsilon and η\eta are the evaluation and the coevaluation maps respectively, both of which are obtained from the standard adjoint pair of functors 𝒪XHomX(,)-\otimes_{\mathcal{O}_{X}}\ast\dashv\mathop{\mathbb{R}\mathrm{Hom}}\nolimits_{X}(\ast,-).

HomX(α,E)𝐤αεETα(E)+1\displaystyle\mathop{\mathbb{R}\mathrm{Hom}}\nolimits_{X}\left(\alpha,E\right)\otimes_{\mathbf{k}}\alpha\xrightarrow{\varepsilon}E\to T_{\alpha}(E)\xrightarrow{+1} (2.16)
Tα(E)EηHomX(E,α)𝐤α+1\displaystyle T^{\prime}_{\alpha}(E)\to E\xrightarrow{\eta}\mathop{\mathbb{R}\mathrm{Hom}}\nolimits_{X}\left(E,\alpha\right)^{\vee}\otimes_{\mathbf{k}}\alpha\xrightarrow{+1} (2.17)
Lemma 2.3 ([Ishii-Uehara_ADC, Lemma 4.14]).

For each ΦAuteq(X)\Phi\in\operatorname{Auteq}(X), there is an isomorphism of autoequivalences as follows.

ΦTαΦ1TΦ(α)\displaystyle\Phi\circ T_{\alpha}\circ\Phi^{-1}\simeq T_{\Phi(\alpha)} (2.18)

In particular, for any a,ma,m\in\mathbb{Z} it holds that

(2.19)