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Classifying sections of del Pezzo fibrations, II

Brian Lehmann Department of Mathematics
Boston College
Chestnut Hill, MA     02467
[email protected]
 and  Sho Tanimoto Graduate School of Mathematics, Nagoya University, Furocho Chikusa-ku, Nagoya, 464-8602, Japan [email protected]
Abstract.

Let XX be a del Pezzo surface over the function field of a complex curve. We study the behavior of rational points on XX leading to bounds on the counting function in Geometric Manin’s Conjecture. A key tool is the Movable Bend and Break Lemma which yields an inductive approach to classifying relatively free sections for a del Pezzo fibration over a curve. Using this lemma we prove Geometric Manin’s Conjecture for certain split del Pezzo surfaces of degree 2\geq 2 admitting a birational morphism to 2\mathbb{P}^{2} over the ground field.

1. Introduction

In an unpublished note ([Bat88]), Batyrev developed a heuristic argument for Manin’s Conjecture for a trivial family of Fano varieties over an 𝔽q\mathbb{F}_{q}-curve. His heuristic relies on several assumptions about the geometry of sections of a Fano fibration over an 𝔽q\mathbb{F}_{q}-curve as well as some point counting estimates. If we focus on the geometry of sections, the collection of analogous conjectures over the function field of a complex curve is known as Geometric Manin’s Conjecture. In this paper we study Geometric Manin’s Conjecture for del Pezzo surfaces over the function field of a complex curve.

Let BB be a smooth projective curve over an algebraically closed field of characteristic 0. A del Pezzo fibration over BB is an algebraic fiber space π:𝒳B\pi:\mathcal{X}\to B such that 𝒳\mathcal{X} is projective, 𝒳\mathcal{X} has only Gorenstein terminal singularities, and the general fiber of π\pi is a smooth del Pezzo surface. Let Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) denote the parameter space of sections of π\pi. Our main results describe the relationship between irreducible components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) and the geometric invariants used in Geometric Manin’s Conjecture.

In the companion paper [LT19a], we studied the analogous problem for del Pezzo fibrations over 1\mathbb{P}^{1}. The conceptual approach in this paper is similar (particularly in Theorem 5.3 and in Section 7): we systematically use Bend-and-Break to reduce questions about sections to properties of rational curves in the fibers. [LT19a] explains how our main results can be applied to study the Abel-Jacobi map for components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) and the enumerativity of certain Gromov-Witten invariants; we will not explain these applications in this paper but refer the reader to [LT19a] for details.

1.1. Main results

The following definition identifies the “well-behaved” sections of a del Pezzo fibration.

Definition 1.1.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. We say that a section CC is relatively free if CC is contained in the smooth locus of 𝒳\mathcal{X}, H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0, and NC/𝒳N_{C/\mathcal{X}} is generically globally generated.

Remark 1.2.

[GHS03] shows that every del Pezzo fibration π:𝒳B\pi:\mathcal{X}\to B admits a section. Since a Gorenstein terminal threefold has only lci singularities, starting from any given section we can construct a relatively free section by gluing on sufficiently many free rational curves contained in the fibers of π\pi and smoothing (see Remark 10.8). Thus every del Pezzo fibration admits many families of relatively free sections.

It is natural to separate irreducible components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) into three types:

  1. (1)

    Non-dominant families of sections.

  2. (2)

    Dominant families for which a general section is not relatively free.

  3. (3)

    Dominant families for which a general section is relatively free.

We prove structural theorems for all three types of irreducible components. We first analyze the components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which parametrize a non-dominant family of sections.

Theorem 1.3.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. There is a finite union of surfaces YY whose intersections with a general fiber of π\pi are rational curves of anticanonical degree 2\leq 2 and a constant C(𝒳)C(\mathcal{X}) such that the following holds. Suppose that MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is a component parametrizing a non-dominant family of sections of height C(𝒳)\geq C(\mathcal{X}). Then the sections parametrized by MM sweep out one of these surfaces YY.

Here C(𝒳)C(\mathcal{X}) is an explicit constant determined by the behavior of low degree sections.

Remark 1.4.

[Cor96, 3.3 Theorem] shows that any del Pezzo surface over the function field of BB admits an integral model with Gorenstein terminal singularities such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. Thus every del Pezzo fibration admits a birational model where Theorem 1.3 applies.

Remark 1.5.

Theorem 1.3 can be used to show that there is a proper closed set V𝒳V\subsetneq\mathcal{X} which contains all sections which do not deform to dominate 𝒳\mathcal{X}.

Our second main result addresses dominant families of sections which are not relatively free. It shows that the existence of sections of this type is controlled by a bounded family of surfaces.

Theorem 1.6.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. There is a bounded family of surfaces YY whose intersections with a general fiber of π\pi are rational curves of anticanonical degree 22 and a constant D(𝒳)D(\mathcal{X}) such that the following holds. Suppose that MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is a component parametrizing a dominant family of sections of height D(𝒳)\geq D(\mathcal{X}) which are not relatively free. Then the general section parametrized by MM is contained in some surface in our family.

Here D(𝒳)D(\mathcal{X}) is an explicit constant determined by the behavior of low degree sections.

Our final main result shows that any component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) that parametrizes relatively free sections of large height will contain in its closure a union of a π\pi-vertical rational free curve and a relatively free section of smaller height. As in [HRS04], this allows us to study families of relatively free sections of large height via induction by appealing to the gluing-and-smoothing structure of stable maps.

Theorem 1.7 (Movable Bend-and-Break for relatively free sections).

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. There is a constant Q(𝒳)Q(\mathcal{X}) satisfying the following property. Suppose that MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is a component that parametrizes a dominant family of relatively free sections CC satisfying K𝒳/BCQ(𝒳)-K_{\mathcal{X}/B}\cdot C\geq Q(\mathcal{X}). Then the closure of MM in M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) contains a point representing a stable map whose domain has two components; one maps birationally to a relatively free section and the other maps birationally to a free π\pi-vertical rational curve.

Here Q(𝒳)Q(\mathcal{X}) is an explicit constant determined by the behavior of low degree sections.

Remark 1.8.

[Cor96, 1.10 Theorem] shows that any del Pezzo fibration whose generic fiber has degree 3\geq 3 will admit a birational model which has Gorenstein terminal singularities and a relatively ample anticanonical divisor.

1.2. Geometric Manin’s Conjecture

Inspired by the thin set version of Manin’s conjecture and the conjectural description of the exceptional set in [LST18], the authors proposed the first version of Geometric Manin’s Conjecture in [LT19b]. The statement relies on the following invariant from the Minimal Model Program.

Definition 1.9.

Let XX be a smooth projective variety over a field of characteristic 0. Let LL be a big and nef \mathbb{Q}-Cartier divisor on XX. We define the Fujita invariant, or the aa-invariant, to be

a(X,L)=min{tKX+tLEff¯1(X)}.a(X,L)=\min\{t\in\mathbb{R}\mid K_{X}+tL\in\overline{\mathrm{Eff}}^{1}(X)\}. (1.1)

When LL is nef but not big, we formally set a(X,L)=+a(X,L)=+\infty.

When XX is singular, we define the Fujita invariant as the Fujita invariant of the pullback of LL to any smooth model. This is well-defined because of [HTT15, Proposition 2.7].

Roughly speaking Geometric Manin’s Conjecture predicts two things. First, the conjecture predicts that there should be a “thin exceptional set” which can be described using the Fujita invariant as in [LST18].

Principle 1.10.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration over a smooth projective curve. All “pathological” irreducible components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) will parametrize sections which are contained in a bounded family of subvarieties 𝒴𝒳\mathcal{Y}\subset\mathcal{X} such that the Fujita invariant of 𝒴η\mathcal{Y}_{\eta} with respect to K𝒳/B-K_{\mathcal{X}/B} is at least as large as the Fujita invariant of 𝒳η\mathcal{X}_{\eta}.

Here the notion of “pathological” is flexible. If we interpret patholgical to mean “not relatively free”, then Principle 1.10 for del Pezzo fibrations is established by Theorem 1.3 and Theorem 1.6. We can also interpret pathological more narrowly to mean “components which grow too quickly” and we give a precise accounting of Principle 1.10 for del Pezzo fibrations in this setting in Section 10.

Second, Geometric Manin’s Conjecture predicts that the number of relatively free families representing a given numerical class is bounded above.

Principle 1.11.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration over a smooth projective curve. After removing all components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which factor through the exceptional set constructed by [LST18], there should be exactly |Br(X)||\mathrm{Br}(X)| irreducible components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) representing each sufficiently positive nef curve class which admits a relatively free section.

We do not know how to establish Principle 1.11 for del Pezzo fibrations in general. However, the inductive structure given by Theorem 1.7 allows us to prove a weaker bound on the number of components. The following result shows that the number of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) only grows polynomially in the degree as predicted by Batyrev.

Theorem 1.12.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Then there is a polynomial P(d)P(d) such that the number of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing sections of height d\leq d is bounded above by P(d)P(d).

One can rephrase Geometric Manin’s Conjecture to emphasize the analogy with the number theoretic version. Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. For simplicity, we assume that ρ(𝒳η)2\rho(\mathcal{X}_{\eta})\geq 2 where ρ(𝒳η)\rho(\mathcal{X}_{\eta}) is the Picard rank of 𝒳η\mathcal{X}_{\eta}. We say that a component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is an accumulating component if MM parametrizes sections contained in a surface whose generic fiber is a union of K𝒳η-K_{\mathcal{X}_{\eta}}-lines. We say that a component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is a Manin component if it is not accumulating.

Let Manini\mathrm{Manin}_{i} be the set of Manin components parametrizing sections CC with K𝒳/B.C=i-K_{\mathcal{X}/B}.C=i. For q>1q>1 and any positive integer dd we define the counting function by

N(𝒳,K𝒳/B,q,d):=i=1dMManiniqdimM.N(\mathcal{X},-K_{\mathcal{X}/B},q,d):=\sum_{i=1}^{d}\sum_{M\in\mathrm{Manin}_{i}}q^{\dim M}.

This counting function is inspired by Batyrev’s heuristic for Manin’s Conjecture for 𝔽q\mathbb{F}_{q}-curves on a smooth Fano variety; the term qdimMq^{\dim M} represents the “expected” number of 𝔽q\mathbb{F}_{q}-points on MM. The “expected” asymptotic growth rate of the counting function is

N(𝒳,K𝒳/B,q,d)dcqddρ(𝒳η)1.N(\mathcal{X},-K_{\mathcal{X}/B},q,d)\mathrel{\mathop{\sim}_{d\to\infty}}cq^{d}d^{\rho(\mathcal{X}_{\eta})-1}.

Theorem 1.12 implies a weaker upper bound on the counting function. For simplicity we assume that the general fiber of π\pi contains a (1)(-1)-curve.

Theorem 1.13.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that 𝒳\mathcal{X} is smooth, K𝒳/B-K_{\mathcal{X}/B} is relatively ample, and the general fiber is a del Pezzo surface that is not 2\mathbb{P}^{2} or 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}. Then there is some non-negative integer rr such that

N(𝒳,K𝒳/B,q,d)=O(qddr).N(\mathcal{X},-K_{\mathcal{X}/B},q,d)=O(q^{d}d^{r}).
Remark 1.14.

Suppose we fix a del Pezzo surface 𝒳η\mathcal{X}_{\eta} over the function field of BB. Geometric Manin’s Conjecture for 𝒳η\mathcal{X}_{\eta} implicitly relies on the choice of an integral model of 𝒳η\mathcal{X}_{\eta} over BB. (Analogously, in the number field setting Manin’s Conjecture depends upon a choice of metrization.)

Just as in the number field setting, if 𝒳η\mathcal{X}_{\eta} has an integral model where Theorem 1.13 applies then one should be able to deduce the analogous bound for every integral model of 𝒳η\mathcal{X}_{\eta}. (In contrast, although we expect Theorem 1.3 and Theorem 1.7 to hold for any integral model of 𝒳η\mathcal{X}_{\eta} we do not see an easy way to pass the statements between different integral models.)

1.3. Classifying components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B)

Suppose that π:𝒳B\pi:\mathcal{X}\to B is a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Furthermore, suppose that we can classify all sections of low height by hand. Then the components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) of large height can be described inductively using Theorem 1.3, Theorem 1.6, and Theorem 1.7. This technique is illustrated in several examples in [LT19a, Section 8]. In particular, this type of argument should allow us to fully prove Geometric Manin’s Conjecture for specific examples. However it is challenging to prove a general statement. We are able to prove this strong version in a somewhat restrictive situation.

Theorem 1.15.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that every fiber of π\pi is a del Pezzo surface with canonical singularities of degree 2\geq 2. Suppose that 𝒳\mathcal{X} is \mathbb{Q}-factorial and that the generic fiber 𝒳η\mathcal{X}_{\eta} is the blow-up of k(B)2\mathbb{P}^{2}_{k(B)} at a finite number of points defined over k(B)k(B). Then there is some section CC such that for every integral numerical class α\alpha in C+Nef1(𝒳η)C+\mathrm{Nef}_{1}(\mathcal{X}_{\eta}) there is exactly one component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which parametrizes relatively free sections and represents α\alpha.

Example 1.16.

Suppose we fix a smooth del Pezzo surface SS of degree 2\geq 2 and a curve BB. Applying Theorem 1.15 to π:S×BB\pi:S\times B\to B we see there is a translate of Nef1(S)\mathrm{Nef}_{1}(S) in N1(S)N_{1}(S) such that every curve class in this translate is represented by a unique component of Mor(B,S)\mathrm{Mor}(B,S).

Theorem 1.15 verifies the strong version of Geometric Manin’s Conjecture for this type of del Pezzo fibration. Note that in this situation 𝒳η\mathcal{X}_{\eta} is rational so that Br(𝒳)\mathrm{Br}(\mathcal{X}) is trivial. For the del Pezzo fibrations addressed by Theorem 1.15 we obtain the expected growth rate

N(𝒳,K𝒳/B,q,d)dcqddρ(𝒳η)1.N(\mathcal{X},-K_{\mathcal{X}/B},q,d)\mathrel{\mathop{\sim}_{d\to\infty}}cq^{d}d^{\rho(\mathcal{X}_{\eta})-1}.

where the leading constant cc is described by Theorem 10.10.

A key new feature of Theorem 1.15 is that the proof does not rely on induction. In particular, we do not need any ad hoc arguments to analyze base cases. Instead, we define a monoid structure on the set \mathcal{R} of components of nef curve classes on a del Pezzo surface given by gluing and smoothing. This monoid acts on the set of components of relatively free sections of sufficiently large height by gluing and smoothing and Movable Bend and Break tells us that this set is finitely generated by \mathcal{R}. By exhibiting many relations among components of relatively free sections, we show that every nef class in a translate of the cone is represented by one irreducible relatively free component.

1.4. Comparison to previous works

Batyrev developed a heuristic for Manin’s Conjecture over global function fields in the unpublished notes [Bat88]. (This heuristic is explained in [Tsc09, Section 4.7] and [Bou11, Section 1.2].) This perspective motivated the formulation of the Batyrev-Manin Conjecture developed in [BM90]. This theme was also revisited in [Man95] which proves an exponential bound on the number of components of Mor(1,X)\mathrm{Mor}({\mathbb{P}}^{1},X) and discusses the analogy with rational point counts.

Suppose that XX is a Fano variety and BB is a smooth projective curve over a finite field. Batyrev’s heuristic for sections of π:X×BB\pi:X\times B\to B is based on the following three assumptions:

  1. (1)

    For each nef class αNef1(X)\alpha\in\mathrm{Nef}_{1}(X)_{\mathbb{Z}}, every irreducible component of the moduli space Mor(B,X,α)\mathrm{Mor}(B,X,\alpha) has the expected dimension KXB+dim(X)(1g(B))-K_{X}\cdot B+\dim(X)(1-g(B));

  2. (2)

    For each nef class αNef1(X)\alpha\in\mathrm{Nef}_{1}(X)_{\mathbb{Z}}, Mor(B,X,α)\mathrm{Mor}(B,X,\alpha) is irreducible;

  3. (3)

    If we use the naive estimate |Mor(B,X,α)(𝔽q)|qdimMor(B,X,α)|\mathrm{Mor}(B,X,\alpha)(\mathbb{F}_{q})|\approx q^{\dim\mathrm{Mor}(B,X,\alpha)} then we do not affect the asymptotic growth rate of the number of rational points.

As stated the assumptions (1) and (2) are not valid even for large degree curves. This failure is related to the properties of the exceptional set in Manin’s Conjecture for rational points. (Ellenberg and Venkatesh suggest that (3) may be approached using homological stability – see [EV05] – but as of now we do not have many examples. [BS20] proves a statement in this direction for low degree Fano hypersurfaces.)

The classification of components of Mor(1,X)\mathrm{Mor}(\mathbb{P}^{1},X) for a Fano variety XX has a long and rich history. For 1\mathbb{P}^{1} the predictions (1),(2) implicit in Batyrev’s heuristics have been verified in the following cases (and in many other special cases):

In contrast, there has not been much progress toward the classification of irreducible components of Mor(B,X)\mathrm{Mor}(B,X) when BB has genus 1\geq 1. Aside from Bourqui’s pioneering results for toric varieties, to the best of our knowledge there are only a few examples of homogeneous varieties XX where the irreducible components of Mor(B,X)\mathrm{Mor}(B,X) have been fully classified (and primarily when BB is an elliptic curve – [Bru87], [Bal89], [Per12], [PP13]).

More generally, one would like to classify the irreducible components of the space of sections of a Fano fibration. While there are many powerful theorems describing the qualitative nature of sections of Fano fibrations, there are fewer quantitative results. [LT19a] develops Geometric Manin’s Conjecture for sections of Fano fibrations over 1\mathbb{P}^{1} and proves some results for del Pezzo fibrations. In this paper we address del Pezzo fibrations over curves of higher genus. The key contributions of this paper are:

  • This is the first paper which uses the inductive strategy of [HRS04] to classify curves of high genus on a Fano variety. The framework and perspective we develop should be applicable in other situations. When working with higher genus curves, there are many new technical obstacles – in particular, the most difficult part of the argument concerns dominant families of sections which are not relatively free.

  • For a special class of del Pezzo fibrations, we give a conceptual proof of Geometric Manin’s Conjecture using a gluing-and-smoothing monoid structure (Theorem 1.15). Previous techniques have tended to be somewhat ad hoc.


Acknowledgements: The authors would like to thank Yuri Tschinkel for answering our question regarding del Pezzo surfaces over non-closed fields. The authors would also like to thank the anonymous referees for carefully reading our manuscript and significantly improving the exposition of the paper.

Brian Lehmann was supported by NSF grant 1600875. Sho Tanimoto was partially supported by Inamori Foundation, by JSPS KAKENHI Early-Career Scientists Grant number 19K14512, by JSPS Bilateral Joint Research Projects Grant number JPJSBP120219935, and by MEXT Japan, Leading Initiative for Excellent Young Researchers (LEADER).

2. Preliminaries

Let kk be an algebraically closed field of characteristic 0. Let BB be a smooth projective curve defined over kk. In this paper our ground fields will be kk and k(B)k(B). A variety is a reduced irreducible separated scheme which has finite type over the ground field. In this paper a component of a scheme means an irreducible component unless otherwise specified. When we take a component of a scheme, we always endow it with its reduced structure.

2.1. Positive cycles

We will use rat\sim_{rat} to denote rational equivalence of cycles, alg\sim_{alg} to denote algebraic equivalence of cycles, and \equiv to denote numerical equivalence of cycles.

Let XX be a projective variety. We will let N1(X)N^{1}(X) denote the space of \mathbb{R}-Cartier divisors up to numerical equivalence and let Eff¯1(X)\overline{\mathrm{Eff}}^{1}(X) and Nef1(X)\mathrm{Nef}^{1}(X) denote respectively the pseudo-effective and nef cones of divisors. Dually, N1(X)N_{1}(X) denotes the space of real 11-cycles up to numerical equivalence and Eff¯1(X)\overline{\mathrm{Eff}}_{1}(X) and Nef1(X)\mathrm{Nef}_{1}(X) denote respectively the pseudo-effective and nef cones of curves. We will denote by N1(X)N_{1}(X)_{\mathbb{Z}} the lattice of integral curve classes inside of N1(X)N_{1}(X) and by N1(X)N^{1}(X)_{\mathbb{Z}} the lattice of integral divisors inside of N1(X)N^{1}(X).

We say that a reduced irreducible curve CC on XX is movable if CC is a member of a family of curves which dominates XX.

2.2. Height functions

Definition 2.1.

A Fano fibration π:𝒳B\pi:\mathcal{X}\to B is a surjective morphism with connected fibers from a Gorenstein terminal projective variety 𝒳\mathcal{X} to a smooth projective curve BB such that a general fiber is a smooth Fano variety.

We will always denote the generic point of BB by η\eta and the generic fiber of π\pi by 𝒳η\mathcal{X}_{\eta}.

Given a section CC of π\pi and a divisor LL on 𝒳\mathcal{X}, the height of CC with respect to LL is defined to be LCL\cdot C. The following statement is the Northcott property for Fano fibrations over BB.

Lemma 2.2.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration. Fix a \mathbb{Q}-Cartier divisor LL on 𝒳\mathcal{X} whose restriction to the generic fiber of π\pi is ample. For any constant γ\gamma, the sections whose height with respect to LL is γ\leq\gamma form a bounded family.

One consequence is that there is a lower bound on the possible values of LCL\cdot C as we vary CC over all sections.

Definition 2.3.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration and let LL be a \mathbb{Q}-Cartier divisor on 𝒳\mathcal{X} such that the restriction of LL to the generic fiber is ample. We define neg(𝒳,L)\mathrm{neg}(\mathcal{X},L) to be the smallest value of LCL\cdot C as we vary CC over all sections of π:𝒳B\pi:\mathcal{X}\to B.

Another consequence is captured by the following observation:

Observation 2.4.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration. Fix an irreducible component MM of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B). We let M[m]M^{[m]} denote the family of sections parametrized by MM with mm marked points and we denote the evaluation map by evm:M[m]𝒳m\mathrm{ev}_{m}:M^{[m]}\to\mathcal{X}^{m}.

Fix an integer dd and a relatively ample divisor LL. Suppose that we vary MM over all components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) of LL-degree d\leq d for which the evaluation map evm\mathrm{ev}_{m} does not map dominantly to 𝒳×m\mathcal{X}^{\times m}. By Lemma 2.2 the union of closures of the images of these maps will be a proper closed subset of 𝒳×m\mathcal{X}^{\times m}. In particular, if we fix mm general points of 𝒳\mathcal{X}, then any irreducible component MM of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) of degree d\leq d which parametrizes a section through these points will yield a dominant map onto 𝒳×m\mathcal{X}^{\times m}.

Remark 2.5.

From now on, when we say that an irreducible component MM of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizes sections through mm general points, we will mean “general” in the sense of Observation 2.4. Note that implicitly the meaning of “general” will depend upon the relative anticanonical degree of the curves parametrized by MM even when this degree is not explicitly mentioned.

2.3. Generic Fujita invariants

Let us recall the definition of the Fujita invariant from the introduction.

Definition 2.6.

Let XX be a smooth projective variety over a field of characteristic 0. Let LL be a big and nef \mathbb{Q}-Cartier divisor on XX. We define the Fujita invariant, or the aa-invariant, to be

a(X,L)=min{tKX+tLEff¯1(X)}.a(X,L)=\min\{t\in\mathbb{R}\mid K_{X}+tL\in\overline{\mathrm{Eff}}^{1}(X)\}. (2.1)

When LL is nef but not big, we formally set a(X,L)=+a(X,L)=+\infty.

When XX is singular, we define the Fujita invariant as the Fujita invariant of the pullback of LL to any smooth model. This is well-defined because of [HTT15, Proposition 2.7].

Note that the aa-invariant is geometric: it does not change under field extension. We will be interested in how the Fujita invariant behaves over k(B)k(B).

Lemma 2.7 ([LT19a] Lemma 3.3).

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration and let LL be a \mathbb{Q}-Cartier divisor on 𝒳\mathcal{X} such that the restriction of LL to the generic fiber 𝒳η\mathcal{X}_{\eta} is big and nef. Then for any smooth Fano fiber FF of π\pi we have

a(Xη,L|Xη)=a(F,L|F).a(X_{\eta},L|_{X_{\eta}})=a(F,L|_{F}).

As in [LT19a] we will call this quantity the generic aa-invariant of 𝒳\mathcal{X} with respect to LL. For del Pezzo surfaces, it is easy to work out the behavior of the aa-invariant of the anticanonical divisor when restricted to subvarieties. This leads to the following description:

Lemma 2.8 ([LT19a] Lemma 3.4).

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Then:

  • A subvariety YY will have a(Yη,K𝒳/B)>1a(Y_{\eta},-K_{\mathcal{X}/B})>1 if and only if its intersection with a general fiber FF is a union of curves of the following types: (1)(-1)-curves, or rational curves in |KF||-K_{F}| when FF has degree 11.

  • A subvariety YY will have a(Yη,K𝒳/B)=1a(Y_{\eta},-K_{\mathcal{X}/B})=1 if and only if its intersection with a general fiber FF is a union of curves of the following types: irreducible fibers of a conic fibration on FF, the rational curves in |KF||-K_{F}| if FF has degree 22, and the rational curves which lie in |2KF||-2K_{F}| or the pullback of the anticanonical linear series on a degree 22 del Pezzo surface if FF has degree 11.

Corollary 2.9.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. The union of all subvarieties YY with a(Yη,K𝒳/B)>1a(Y_{\eta},-K_{\mathcal{X}/B})>1 is a closed subset of 𝒳\mathcal{X}.

The subvarieties YY with generic aa-invariant equal to 11 are a little more complicated; note that they need not form a bounded family on 𝒳\mathcal{X} (even though the corresponding subvarieties of 𝒳η\mathcal{X}_{\eta} do form a bounded family). However, we do have a weaker boundedness statement.

Proposition 2.10.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Fix a bounded family of sections of π\pi. The family of surfaces Y𝒳Y\subset\mathcal{X} which contain a section in our family and satisfy a(Yη,K𝒳/B)=1a(Y_{\eta},-K_{\mathcal{X}/B})=1 is bounded.

Proof.

Lemma 2.8 (2) describes the possible types of a general fiber of π|Y\pi|_{Y}: they are rational curves of anticanonical degree 22. Note that if we fix a point in a del Pezzo surface there are only finitely many curves of these types through that point.

Suppose we fix a section CC of π\pi. The observation above shows that there are only finitely many surfaces which contain this section and satisfy a(Yη,K𝒳/B)=1a(Y_{\eta},-K_{\mathcal{X}/B})=1. Constructing an incidence correspondence we obtain the boundedness of the surfaces YY as in the statement of the proposition. ∎

2.4. Bend-and-Break

We will need the following result controlling the behavior of Bend-and-Break for sections.

Lemma 2.11.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration. Fix a set of nn general points {xi}i=1n\{x_{i}\}_{i=1}^{n} of 𝒳\mathcal{X} where n2n\geq 2. Suppose there is a one-dimensional family of sections which contain all nn points. Then the closure of this family in M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) contains a stable map f:C𝒳f:C\to\mathcal{X} such that CC has at least two components C1,C2C_{1},C_{2} which are not contracted by ff and such that f(C1)f(C_{1}) and f(C2)f(C_{2}) each contain one of the xix_{i}.

Proof.

When B1B\cong\mathbb{P}^{1} this statement is proved in [LT19a, Lemma 4.1]. Suppose that g(B)1g(B)\geq 1. The statement of Bend-and-Break shows that the family of sections deforms to a stable map f:C𝒳f:C\to\mathcal{X} such that

  • f(C)f(C) contains all nn general points, and

  • there is some component C1C_{1} of CC which is rational, is not contracted by ff, and whose ff-image contains one of the general points.

Since C1C_{1} is rational and g(B)1g(B)\geq 1 the image of C1C_{1} must be π\pi-vertical, so f(C1)f(C_{1}) can contain at most one general point. Thus the other general points will be contained in other components of f(C)f(C), proving the statement. ∎

2.5. Vector bundles on curves

In this section we quickly review some facts about rank 22 vector bundles on curves.

Lemma 2.12 ([Har77] V.2.12.(b), [Nag70] Theorem 1).

Let \mathcal{E} be a rank 22 vector bundle on the smooth curve BB.

  1. (1)

    Suppose that \mathcal{E} is unstable. Consider the destabilizing exact sequence

    02100\to\mathcal{L}_{2}\to\mathcal{E}\to\mathcal{L}_{1}\to 0

    given by the maximal slope subbundle 2\mathcal{L}_{2}. If \mathcal{E} is indecomposable then

    0<deg(2)deg(1)2g(B)2.0<\deg(\mathcal{L}_{2})-\deg(\mathcal{L}_{1})\leq 2g(B)-2.
  2. (2)

    Suppose that \mathcal{E} is semistable. Consider the exact sequence

    01200\to\mathcal{L}_{1}\to\mathcal{E}\to\mathcal{L}_{2}\to 0

    given by a maximal slope rank 11 subbundle 1\mathcal{L}_{1}. Then we have

    0deg(2)deg(1)g(B).0\leq\deg(\mathcal{L}_{2})-\deg(\mathcal{L}_{1})\leq g(B).

Using Kodaira vanishing and the exact sequences above, one obtains:

Corollary 2.13.

Let \mathcal{E} be a rank 22 vector bundle on the smooth curve BB.

  1. (1)

    If \mathcal{E} is unstable, indecomposable, and deg()6g(B)4\deg(\mathcal{E})\geq 6g(B)-4 then h1(B,)=0h^{1}(B,\mathcal{E})=0.

  2. (2)

    If \mathcal{E} is semistable and deg()5g(B)2\deg(\mathcal{E})\geq 5g(B)-2 then h1(B,)=0h^{1}(B,\mathcal{E})=0.

We will also need the following fact about the variation of the Harder-Narasimhan filtration in families.

Theorem 2.14 ([HL97] Theorem 2.3.2).

Let TT be a variety and let \mathcal{E} be a vector bundle of rank 22 on T×BT\times B. We can think of TT as the parameter space for a family of rank 22 vector bundles on BB. Then there exists a non-empty Zariski open subset TTT^{\prime}\subset T such that either

  • for each tTt\in T^{\prime}, |{t}×B\mathcal{E}|_{\{t\}\times B} is semistable, or;

  • there exists a line subbundle |T×B\mathcal{L}\subset\mathcal{E}|_{T^{\prime}\times B} on T×BT^{\prime}\times B such that for each tTt\in T^{\prime}, |{t}×B\mathcal{L}|_{\{t\}\times B} is the maximal destabilizing subsheaf of |{t}×B\mathcal{E}|_{\{t\}\times B}.

2.6. Conics on del Pezzo surfaces

Finally we record the following lemma for later applications:

Lemma 2.15.

Let SS be a smooth del Pezzo surface of degree dd over an algebraically closed field kk of characteristic 0. Let CC be an anticanonical conic on SS, i.e. CC is rational and KSC=2-K_{S}\cdot C=2. Then CC satisfies one of the following conditions:

  1. (1)

    C2=0C^{2}=0 and CC is a member of a conic fibration ρ:S1\rho:S\to\mathbb{P}^{1};

  2. (2)

    d=2d=2 and CC is a rational member of |KS||-K_{S}|;

  3. (3)

    d=1d=1 and CC is a rational member of |L||L| where LL is the pullback of the anticanonical divisor via a blow down SSS\to S^{\prime} to a degree 22 del Pezzo surface, or;

  4. (4)

    d=1d=1 and CC is a rational member of |2KS||-2K_{S}|.

Moreover a general member of each family has at worst nodal singularities.

Proof.

First of all it follows from adjunction that C20C^{2}\geq 0 and C2C^{2} is even. On the other hand, by the Hodge index theorem we have dC240dC^{2}-4\leq 0. Thus when d3d\geq 3, we conclude that C2=0C^{2}=0 and the linear series |C||C| defines a conic fibration. When d=2d=2, we have two possibilities: C2=0C^{2}=0 or 22. When C2=0C^{2}=0, |C||C| defines a conic fibration. When C2=2C^{2}=2, CC is linearly equivalent to KS-K_{S}. Thus CC is a rational member of |KS||-K_{S}|. When d=1d=1, there are three possibilities: C2=0,2C^{2}=0,2, or 44. Again when C2=0C^{2}=0 the linear series |C||C| defines a conic fibration. When C2=2C^{2}=2, we claim that C+KSC+K_{S} is linearly equivalent to a (1)(-1)-curve. Indeed, using the exact sequence

0H0(S,𝒪S(C+KS))H0(S,𝒪S(C))H0(C,𝒪C)0\to H^{0}(S,\mathcal{O}_{S}(C+K_{S}))\to H^{0}(S,\mathcal{O}_{S}(C))\to H^{0}(C,\mathcal{O}_{C})

one sees that H0(S,C+KS)>0H^{0}(S,C+K_{S})>0 and then the intersection-theoretic properties of C+KSC+K_{S} show that it is linearly equivalent to a (1)(-1)-curve. Thus CC is a member of a family in (3). When C2=4C^{2}=4, CC is linearly equivalent to 2KS-2K_{S}. Thus our assertion follows.

Finally for the last claim, any general member of a conic fibration is smooth. For a degree 22 del Pezzo surface SS, |KS||-K_{S}| defines a double cover S2S\to\mathbb{P}^{2} ramified along a smooth quartic curve DD and any rational member of |KS||-K_{S}| is the pullback of a tangent line to DD. A generic tangent line has only one tangency point so that a general rational curve in |KS||-K_{S}| has only one node. This proves the claim for families in (2) and (3). Finally for a degree 11 del Pezzo surface SS, |2KS||-2K_{S}| defines a double cover SQS\to Q to a singular quadric cone ramified along a smooth complete intersection of QQ and a cubic surface. A general rational member of |2KS||-2K_{S}| corresponds to a hyperplane section bitangent to the branch divisor, thus a general rational curve in |2KS||-2K_{S}| has two nodes. Thus our assertion follows. ∎

3. Families of sections

3.1. Moduli spaces of sections

Let π:𝒳B\pi:\mathcal{X}\rightarrow B be a Fano fibration with dim𝒳3\dim\mathcal{X}\leq 3. By definition 𝒳\mathcal{X} has only Gorenstein terminal singularities. When dim(𝒳)=3\dim(\mathcal{X})=3, this is equivalent to saying that 𝒳\mathcal{X} has cDV singularities ([KM98, Corollary 5.38]). Such singularities are analytically isomorphic to hypersurface singularities, and in particular 𝒳\mathcal{X} is locally complete intersection in the Zariski topology.

We let Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) denote the open subset of Hilb(𝒳)\mathrm{Hilb}(\mathcal{X}) parametrizing sections of π\pi and let Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} denote the sublocus parametrizing sections of height dd. Suppose that CC is a general curve parametrized by a component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B). The expected dimension of MM is

K𝒳/BC+(dim𝒳1)(1g(B)).-K_{\mathcal{X}/B}\cdot C+(\dim\mathcal{X}-1)(1-g(B)).

The expected dimension is a lower bound for the dimension of MM by [Kol96, Chapter I.2 Theorem I.2.15.2]. Indeed, let C𝒪𝒳\mathcal{I}_{C}\subset\mathcal{O}_{\mathcal{X}} be the ideal sheaf of CC. Using the fact that 𝒳\mathcal{X} is lci, one can conclude that we have the exact sequence

0C/C2Ω𝒳1|CΩC10.0\to\mathcal{I}_{C}/\mathcal{I}_{C}^{2}\to\Omega^{1}_{\mathcal{X}}|_{C}\to\Omega^{1}_{C}\to 0.

Our claim follows by combining this with [Kol96, Chapter I.2 Theorem 2.15.2].

When CC avoids the singular locus of 𝒳\mathcal{X} and H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0, then the expected dimension coincides with the actual dimension and CC represents a smooth point of MM. The quantity H0(C,NC/𝒳)H^{0}(C,N_{C/\mathcal{X}}) is an upper bound for the dimension of MM assuming that CC avoids the singularities of 𝒳\mathcal{X}.

3.1.1. Compactifications

Using the functor defining the Hilbert scheme, we see that each component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) admits a natural embedding into the stack g(B),0(𝒳)\mathcal{M}_{g(B),0}(\mathcal{X}). Since every stable map parametrized by MM is birational onto its image these curves have trivial automorphism group over 𝒳\mathcal{X}, so that MM also admits a natural embedding into a component M¯\overline{M} of the coarse moduli space M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}). Note that the domain of any stable map parametrized by M¯\overline{M} will be the union of a section with a finite collection of trees of π\pi-vertical rational curves.

3.1.2. Fixed points

We will also need parameter spaces for sections containing a set of fixed points. When the base has genus 0 we can appeal to [She12] which constructs a moduli space for rational curves through fixed points. We will briefly discuss the situation for curves of higher genus.

Let q1,,qrq_{1},\ldots,q_{r} be rr points on 𝒳\mathcal{X} whose images pi:=π(qi)p_{i}:=\pi(q_{i}) are distinct. Recall that [Kol96, Section I.1] constructs the moduli space Mor(B,𝒳,piqi)\mathrm{Mor}(B,\mathcal{X},p_{i}\mapsto q_{i}) of morphisms f:B𝒳f:B\to\mathcal{X} sending piqip_{i}\mapsto q_{i}. This space admits a map to Aut(B,pi)\mathrm{Aut}(B,p_{i}). Since the genus of BB is at least 11 and r1r\geq 1, this automorphism group is finite. Using the universal properties, we see that the component of Mor(B,𝒳,piqi)\mathrm{Mor}(B,\mathcal{X},p_{i}\mapsto q_{i}) lying above the trivial automorphism is isomorphic to the sublocus Sec(𝒳/B,q1,,qr)\mathrm{Sec}(\mathcal{X}/B,q_{1},\ldots,q_{r}) in Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing sections containing the points {qi}\{q_{i}\}. It is clear from the construction that we have natural inclusions Sec(𝒳/B,q1,,qr)Sec(𝒳/B,q1,,qr1)\mathrm{Sec}(\mathcal{X}/B,q_{1},\ldots,q_{r})\to\mathrm{Sec}(\mathcal{X}/B,q_{1},\ldots,q_{r-1}). The expected dimension of Sec(𝒳/B,q1,,qr)\mathrm{Sec}(\mathcal{X}/B,q_{1},\ldots,q_{r}) is

K𝒳/BC+(dim𝒳1)(1g(B)r)-K_{\mathcal{X}/B}\cdot C+(\dim\mathcal{X}-1)(1-g(B)-r)

and every component has at least the expected dimension. If CC avoids the singular locus of 𝒳\mathcal{X} and H1(C,NC/𝒳(q1qr))=0H^{1}(C,N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{r}))=0 then the expected dimension coincides with the actual dimension and CC represents a smooth point of MM. If CC is in the smooth locus of 𝒳\mathcal{X} the quantity H0(C,NC/𝒳(q1qr))H^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{r})) is an upper bound for the dimension of MM.

3.2. Dominant families

Suppose that MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) parametrizes a dominant family of sections. Let CC be a general section parametrized by MM; we will study the properties of the normal bundle.

Definition 3.1.

We say that a section CC is relatively free if CC avoids the singular locus of 𝒳\mathcal{X}, H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0, and NC/𝒳N_{C/\mathcal{X}} is generically globally generated, in the sense that the evaluation map

H0(C,NC/𝒳)𝒪CNC/𝒳H^{0}(C,N_{C/\mathcal{X}})\otimes\mathcal{O}_{C}\to N_{C/\mathcal{X}}

is surjective at the generic point of CC.

Remark 3.2.

According to [Kol96, II.3 Definition 3.1] a curve f:CXf:C\to X is free if CC avoids the singular locus of XX, H1(C,fTX)=0H^{1}(C,f^{*}T_{X})=0, and fTXf^{*}T_{X} is globally generated. Note that our notion of relatively free is not quite a “relative version” of the notion of freeness, since we only require the normal bundle to be generically globally generated. Our decision to use a weaker notion is motivated by Corollary 3.4.

The following proposition connects the existence of deformations of CC through general points with the generically globally generated condition of NC/𝒳N_{C/\mathcal{X}}.

Proposition 3.3.

Let π:𝒳B\pi:\mathcal{X}\rightarrow B be a Fano fibration. Fix different points q1,,qmq_{1},\ldots,q_{m} of 𝒳\mathcal{X} and let MM denote a component of Sec(𝒳/B,q1,,qm)\mathrm{Sec}(\mathcal{X}/B,q_{1},\ldots,q_{m}). Suppose that the sections parametrized by MM dominate 𝒳\mathcal{X} and the general such section avoids the singular locus of 𝒳\mathcal{X}. Then for a general section CC parametrized by MM and for a general point pBp\in B we have that H0(C,NC/𝒳(q1qm))NC/𝒳|pH^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m}))\to N_{C/\mathcal{X}}|_{p} is surjective.

Conversely, suppose we fix a section f:B𝒳f:B\rightarrow\mathcal{X} whose image CC avoids the singularities of 𝒳\mathcal{X}. Suppose that q1,,qmq_{1},\ldots,q_{m} are distinct points of CC such that H1(C,NC/𝒳(q1qm))=0H^{1}(C,N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m}))=0. Let MSec(𝒳/B,q1,,qm)M\subset\mathrm{Sec}(\mathcal{X}/B,q_{1},\ldots,q_{m}) denote the unique component containing ff. If for a general point pCp\in C we have that H0(C,NC/𝒳(q1qm))NC/𝒳|pH^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m}))\to N_{C/\mathcal{X}}|_{p} is surjective, then MM parametrizes a dominant family of curves on 𝒳\mathcal{X}.

Proof.

This is proved by [She12, Section 2] when the genus is 0. Let p1,,pmp_{1},\cdots,p_{m} be the images of q1,,qmq_{1},\cdots,q_{m} on BB. In the situations where Sec(𝒳/B,q1,,qm)\mathrm{Sec}(\mathcal{X}/B,q_{1},\ldots,q_{m}) can be identified with a component of Mor(B,𝒳,piqi)\mathrm{Mor}(B,\mathcal{X},p_{i}\mapsto q_{i}), this follows from the deformation theory for morphisms described by [Kol96, Section II.3]. The only remaining case is when g(B)=1g(B)=1 and m=0m=0, and it follows from similar arguments. ∎

In particular, we obtain an alternative description of relative free sections.

Corollary 3.4.

Let CC be a section that is general in its family. Then CC is relatively free if and only if CC avoids the singularities of 𝒳\mathcal{X}, H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0, and CC is movable.

We next give two statements relating the space of sections of NC/𝒳N_{C/\mathcal{X}} with the existence of deformations of CC through general points.

Proposition 3.5.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration of relative dimension 11. Let CC be a section of π\pi. If H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0 and for some positive integer mm we have h0(C,NC/𝒳)mh^{0}(C,N_{C/\mathcal{X}})\geq m then deformations of CC go through mm general points of 𝒳\mathcal{X}.

Conversely, if deformations of CC go through mm general points of 𝒳\mathcal{X} then

h0(C,NC/𝒳)m.h^{0}(C,N_{C/\mathcal{X}})\geq m.
Proposition 3.6.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration.

  1. (1)

    Let CC be a section of π\pi contained in the smooth locus of 𝒳\mathcal{X} whose normal bundle is unstable with the maximal destabilizing exact sequence

    02NC/𝒳10.0\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0.

    Suppose that K𝒳/BC4g(B)4-K_{\mathcal{X}/B}\cdot C\geq 4g(B)-4 and H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0. Suppose mm is a positive integer such that

    h0(C,1)m.h^{0}(C,\mathcal{L}_{1})\geq m.

    Then CC is relatively free and deformations of CC go through at least mm general points of 𝒳\mathcal{X}.

    Conversely, suppose that CC is general in moduli. Fix a positive integer mm. If CC goes through at least mm general points of 𝒳\mathcal{X} then we have

    h0(C,1)m.h^{0}(C,\mathcal{L}_{1})\geq m.
  2. (2)

    Let CC be a section of π\pi contained in the smooth locus of 𝒳\mathcal{X} whose normal bundle is semistable.

    Suppose that K𝒳/BC6g(B)2-K_{\mathcal{X}/B}\cdot C\geq 6g(B)-2 and H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0. Suppose mm is a positive integer such that

    h0(C,NC/𝒳)2m.h^{0}(C,N_{C/\mathcal{X}})\geq 2m.

    Then CC is relatively free and deformations of CC go through at least mm general points of 𝒳\mathcal{X}.

    Conversely, fix a positive integer mm. If deformations of CC go through at least mm general points of 𝒳\mathcal{X} then we have

    h0(C,NC/𝒳)2m.h^{0}(C,N_{C/\mathcal{X}})\geq 2m.

We will only prove Proposition 3.6, since the proof of Proposition 3.5 is similar but easier.

Proof.

Case (1): We start by proving the reverse implication. Suppose that CC is general in moduli and goes through mm general points. By Proposition 3.3, if q1,,qmq_{1},\cdots,q_{m} are general points on CC then for any j=1,2,,mj=1,2,\ldots,m we have a surjection

H0(C,NC/𝒳(q1qj1))NC/𝒳(q1qj1)|qj.H^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{j-1}))\to N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{j-1})|_{q_{j}}.

Using the exact sequence

02(q1qm1)NC/𝒳(q1qm1)1(q1qm1)00\to\mathcal{L}_{2}(-q_{1}-\ldots-q_{m-1})\to N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m-1})\to\mathcal{L}_{1}(-q_{1}-\ldots-q_{m-1})\to 0

we see that we must have h0(C,1(q1qm1))>0h^{0}(C,\mathcal{L}_{1}(-q_{1}-\ldots-q_{m-1}))>0. Indeed, there are at least two sections of H0(C,NC/𝒳(q1qm1))H^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m-1})) which generate NC/𝒳(q1qm1)|qmN_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m-1})|_{q_{m}}. Then one of these sections must generate 1(q1qm1)|qm\mathcal{L}_{1}(-q_{1}-\ldots-q_{m-1})|_{q_{m}}. Thus our claim follows. Since the points qiq_{i} were generic, we deduce that h0(C,1)mh^{0}(C,\mathcal{L}_{1})\geq m.

Next we prove the forward implication. Suppose that K𝒳/BC4g(B)4-K_{\mathcal{X}/B}\cdot C\geq 4g(B)-4, H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0, and for some positive integer mm we have

h0(C,1)m.h^{0}(C,\mathcal{L}_{1})\geq m.

Since h1(C,NC/𝒳)=0h^{1}(C,N_{C/\mathcal{X}})=0 we have h1(C,1)=0h^{1}(C,\mathcal{L}_{1})=0. Moreover since deg(2)>12K𝒳/BC2g(B)2\deg(\mathcal{L}_{2})>-\frac{1}{2}K_{\mathcal{X}/B}\cdot C\geq 2g(B)-2 we have h1(C,2)=0h^{1}(C,\mathcal{L}_{2})=0. Since we have deg(2)>deg(1)\deg(\mathcal{L}_{2})>\deg(\mathcal{L}_{1}), we must have

h0(C,2)m.h^{0}(C,\mathcal{L}_{2})\geq m.

If we fix m1m-1 general points q1,,qm1q_{1},\ldots,q_{m-1} in CC then for i=1,2i=1,2

h0(C,i(q1qm1))=h0(C,i)(m1).h^{0}(C,\mathcal{L}_{i}(-q_{1}-\ldots-q_{m-1}))=h^{0}(C,\mathcal{L}_{i})-(m-1).

Thus h1(C,i(q1qm1))=0h^{1}(C,\mathcal{L}_{i}(-q_{1}-\ldots-q_{m-1}))=0 and h0(C,i(q1qm1))1h^{0}(C,\mathcal{L}_{i}(-q_{1}-\ldots-q_{m-1}))\geq 1. Since for i=1,2i=1,2 we have a surjection

i(q1qm1)i(q1qm1)|p\mathcal{L}_{i}(-q_{1}-\ldots-q_{m-1})\to\mathcal{L}_{i}(-q_{1}-\ldots-q_{m-1})|_{p}

for a general point pp, the Snake Lemma shows that NC/𝒳(q1qm1)N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m-1}) surjects onto NC/𝒳(q1qm1)|pN_{C/\mathcal{X}}(-q_{1}-\ldots-q_{m-1})|_{p} for a general point pp. Applying Proposition 3.3 we obtain the desired statement.

Case (2): We first prove the reverse implication. Let CC^{\prime} be a general section in our family. Fix mm general points q1,,qmq_{1},\ldots,q_{m} on CC^{\prime}. By Proposition 3.3

H0(C,NC/𝒳(q1qj1))NC/𝒳(q1qj1)|qjH^{0}(C^{\prime},N_{C^{\prime}/\mathcal{X}}(-q_{1}-\ldots-q_{j-1}))\to N_{C^{\prime}/\mathcal{X}}(-q_{1}-\ldots-q_{j-1})|_{q_{j}}

is surjective for any j=1,2,,mj=1,2,\ldots,m. Thus for jj in this range

h0(C,NC/𝒳(q1qj))=h0(C,NC/𝒳(q1qj1))2h^{0}(C^{\prime},N_{C^{\prime}/\mathcal{X}}(-q_{1}-\ldots-q_{j}))=h^{0}(C^{\prime},N_{C^{\prime}/\mathcal{X}}(-q_{1}-\ldots-q_{j-1}))-2

and we conclude h0(C,NC/𝒳)2mh^{0}(C^{\prime},N_{C^{\prime}/\mathcal{X}})\geq 2m. Then our assertion follows from upper semicontinuity of h0h^{0}.

We next prove the forward implication. Suppose that h=K𝒳/BC6g(B)2h=-K_{\mathcal{X}/B}\cdot C\geq 6g(B)-2 and H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0. We let k0k\geq 0 denote the maximal number of general points contained in deformations of CC. Assume for a contradiction that h+22g(B)>2k+1h+2-2g(B)>2k+1. We fix kk general points q1,,qkq_{1},\cdots,q_{k} on CC and set D=q1++qkD=q_{1}+\ldots+q_{k}. Using Proposition 3.3 inductively as we twist down by general points, we see that h1(C,NC/𝒳(D))=0h^{1}(C,N_{C/\mathcal{X}}(-D))=0. Since kk is the maximal number of general points, Proposition 3.3 shows that NC/𝒳(D)N_{C/\mathcal{X}}(-D) is not generically globally generated. Thus the image of the evaluation map

H0(C,NC/𝒳(D))𝒪CNC/𝒳(D)H^{0}(C,N_{C/\mathcal{X}}(-D))\otimes\mathcal{O}_{C}\to N_{C/\mathcal{X}}(-D)

is a rank 11 subsheaf. We let D\mathcal{L}_{D} denote the saturation of this subsheaf. Note that by our assumption on kk we have

h0(C,D)=h0(C,NC/𝒳(D))>1.h^{0}(C,\mathcal{L}_{D})=h^{0}(C,N_{C/\mathcal{X}}(-D))>1.

We next study how D\mathcal{L}_{D} varies as we change DD. Choose a different general point qk+1q_{k+1} and set D=q1++qk1+qk+1D^{\prime}=q_{1}+\ldots+q_{k-1}+q_{k+1}. Just as above we obtain a saturated subsheaf D\mathcal{L}_{D^{\prime}} of NC/𝒳(D)N_{C/\mathcal{X}}(-D^{\prime}). Note that we have

h0(C,D(qk+1))=h0(C,NC/𝒳(q1qk+1))=h0(C,D(qk))h^{0}(C,\mathcal{L}_{D}(-q_{k+1}))=h^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\cdots-q_{k+1}))=h^{0}(C,\mathcal{L}_{D^{\prime}}(-q_{k}))

and that all of these spaces of sections have dimension at least 11. This implies that both D(qk+1)\mathcal{L}_{D}(-q_{k+1}) and D(qk)\mathcal{L}_{D^{\prime}}(-q_{k}) agree with the saturation of the subsheaf of NC/𝒳(q1qk+1)N_{C/\mathcal{X}}(-q_{1}-\ldots-q_{k+1}) generated by global sections. In particular D=D(qkqk+1)\mathcal{L}_{D^{\prime}}=\mathcal{L}_{D}(q_{k}-q_{k+1}).

Define =D(D)\mathcal{L}=\mathcal{L}_{D}(D). Note that by our argument above \mathcal{L} does not depend on the choice of the sum of kk general points. Consider the exact sequence

0NC/𝒳𝒦0.0\to\mathcal{L}\to N_{C/\mathcal{X}}\to\mathcal{K}\to 0.

Then 𝒦\mathcal{K} is invertible because \mathcal{L} is saturated. Since we have

h0(C,NC/𝒳)=h0(C,NC/𝒳(q1qk))+2k,h^{0}(C,N_{C/\mathcal{X}})=h^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\cdots-q_{k}))+2k,

we must have

h0(C,)=h0(C,(q1qk))+\displaystyle h^{0}(C,\mathcal{L})=h^{0}(C,\mathcal{L}(-q_{1}-\cdots-q_{k}))+\ell
h0(C,𝒦)=h0(C,𝒦(q1qk))+k,\displaystyle h^{0}(C,\mathcal{K})=h^{0}(C,\mathcal{K}(-q_{1}-\cdots-q_{k}))+k,

for some k\ell\leq k. Since the sections of NC/𝒳(q1qk)N_{C/\mathcal{X}}(-q_{1}-\cdots-q_{k}) generate (q1qk)\mathcal{L}(-q_{1}-\cdots-q_{k}) we also must have

h0(C,𝒦(q1qk))=h1(C,(q1qk))=h1(C,)+k.h^{0}(C,\mathcal{K}(-q_{1}-\cdots-q_{k}))=h^{1}(C,\mathcal{L}(-q_{1}-\cdots-q_{k}))=h^{1}(C,\mathcal{L})+k-\ell.

Since h0(C,(q1qk))>1h^{0}(C,\mathcal{L}(-q_{1}-\cdots-q_{k}))>1 we see that g(B)h1(C,(q1qk))=k+h1(C,)g(B)\geq h^{1}(C,\mathcal{L}(-q_{1}-\cdots-q_{k}))=k-\ell+h^{1}(C,\mathcal{L}). Thus

deg(𝒦)\displaystyle\deg(\mathcal{K}) h0(C,𝒦)+g(B)1\displaystyle\leq h^{0}(C,\mathcal{K})+g(B)-1
(g(B)+k)+g(B)1\displaystyle\leq(g(B)+k)+g(B)-1
+3g(B)1\displaystyle\leq\ell+3g(B)-1
<h0(C,)+3g(B)1.\displaystyle<h^{0}(C,\mathcal{L})+3g(B)-1.

If h0(C,)g(B)h^{0}(C,\mathcal{L})\leq g(B), then we conclude that deg(𝒦)<4g(B)1\deg(\mathcal{K})<4g(B)-1. This would also imply that deg()2g(B)1\deg(\mathcal{L})\leq 2g(B)-1. Combining we get h<6g(B)2h<6g(B)-2, contradicting our height bound. Hence we must have h0(C,)g(B)+1h^{0}(C,\mathcal{L})\geq g(B)+1 so that h1(C,)=0h^{1}(C,\mathcal{L})=0.

Since NC/𝒳N_{C/\mathcal{X}} is semistable we see that deg()deg(𝒦)\deg(\mathcal{L})\leq\deg(\mathcal{K}). Since h1(C,)=h1(C,𝒦)=0h^{1}(C,\mathcal{L})=h^{1}(C,\mathcal{K})=0 we deduce that deformations of CC go through at least deg()+1g(B)\deg(\mathcal{L})+1-g(B) general points. Set s=deg()+1g(B)s=\deg(\mathcal{L})+1-g(B). Note in particular that ksk\geq s. For a set of ss general points {qi}\{q_{i}\} we have h0(C,(q1qs))=0h^{0}(C,\mathcal{L}(-q_{1}-\cdots-q_{s}))=0 which contradicts with h0(C,(q1qk))>0h^{0}(C,\mathcal{L}(-q_{1}-\cdots-q_{k}))>0. Thus our assertion follows. ∎

We will frequently use the following two useful corollaries which allow us to easily show that a curve must be relatively free.

Corollary 3.7.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration and let CC be a section.

  1. (1)

    Suppose that CC avoids the singular locus of 𝒳\mathcal{X} and the normal bundle of CC is unstable with the maximal destabilizing exact sequence

    02NC/𝒳10.0\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0.

    If we have

    h0(C,1)g(B)+1h^{0}(C,\mathcal{L}_{1})\geq g(B)+1

    then CC is relatively free.

  2. (2)

    Suppose that CC avoids the singular locus of 𝒳\mathcal{X} and the normal bundle of CC is semistable. If

    h0(C,NC/𝒳)4g(B)+1h^{0}(C,N_{C/\mathcal{X}})\geq 4g(B)+1

    then CC is relatively free.

  3. (3)

    In particular, if CC is a section containing 2g(B)+12g(B)+1 general points of 𝒳\mathcal{X} then a general deformation of CC avoids the singular locus of 𝒳\mathcal{X} and is relatively free.

Proof.

In case (1), since h0(C,1)>g(B)h^{0}(C,\mathcal{L}_{1})>g(B) we must have deg(1)2g(B)1\deg(\mathcal{L}_{1})\geq 2g(B)-1. Since deg(2)>deg(1)\deg(\mathcal{L}_{2})>\deg(\mathcal{L}_{1}) this implies that K𝒳/BC4g(B)1-K_{\mathcal{X}/B}\cdot C\geq 4g(B)-1 and H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0. Then the statement follows from Proposition 3.6.

In case (2), write 01NC/𝒳200\to\mathcal{L}_{1}\to N_{C/\mathcal{X}}\to\mathcal{L}_{2}\to 0 as in Lemma 2.12. We have

h0(C,1)+h0(C,2)h0(C,NC/𝒳)4g(B)+1.h^{0}(C,\mathcal{L}_{1})+h^{0}(C,\mathcal{L}_{2})\geq h^{0}(C,N_{C/\mathcal{X}})\geq 4g(B)+1.

If h0(C,1)>g(B)h^{0}(C,\mathcal{L}_{1})>g(B) then h1(C,1)=0h^{1}(C,\mathcal{L}_{1})=0. In this case deg(2)deg(1)2g(B)1\deg(\mathcal{L}_{2})\geq\deg(\mathcal{L}_{1})\geq 2g(B)-1 and H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0. If h0(C,1)g(B)h^{0}(C,\mathcal{L}_{1})\leq g(B) then h0(C,2)3g(B)+1h^{0}(C,\mathcal{L}_{2})\geq 3g(B)+1. However, in this case we have deg(2)deg(1)>g(B)\deg(\mathcal{L}_{2})-\deg(\mathcal{L}_{1})>g(B), a contradiction to Lemma 2.12.

Thus we conclude that H1(C,NC/𝒳)=0H^{1}(C,N_{C/\mathcal{X}})=0. By Riemann-Roch this implies that deg(NC/𝒳)6g(B)1\deg(N_{C/\mathcal{X}})\geq 6g(B)-1. We conclude the relative freeness condition using Proposition 3.6.

Finally we prove (3). If a general deformation of CC avoids the singularities of 𝒳\mathcal{X} then relative freeness follows from Proposition 3.6 and (1), (2) above, so we only need to prove that a general deformation of CC is contained in the smooth locus. Let MM denote the component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) containing CC and suppose that all sections parametrized by MM meet with the singular locus of 𝒳\mathcal{X}. Let CC^{\prime} be a general member of MM. We choose a resolution β:𝒴𝒳\beta:\mathcal{Y}\to\mathcal{X} and let C~\widetilde{C}^{\prime} be the strict transform of CC^{\prime}. Since 𝒳\mathcal{X} has terminal singularities

K𝒴/BC~<K𝒳/BC.-K_{\mathcal{Y}/B}\cdot\widetilde{C}^{\prime}<-K_{\mathcal{X}/B}\cdot C^{\prime}.

On the other hand since C~\widetilde{C}^{\prime} contains 2g(B)+12g(B)+1 general points of 𝒴\mathcal{Y} it must be relatively free. This means that the dimension of the component containing C~\widetilde{C}^{\prime} is equal to K𝒴/BC+2(1g(B))-K_{\mathcal{Y}/B}\cdot C+2(1-g(B)). This contradicts with

dimMK𝒳/BC+2(1g(B))\dim M\geq-K_{\mathcal{X}/B}\cdot C+2(1-g(B))

and our assertion follows. ∎

The analogue of Corollary 3.7 in the relative dimension 11 case is:

Corollary 3.8.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration of relative dimension 11. Let CC be a section of π\pi. If either

  1. (1)

    deformations of CC go through g(B)+1g(B)+1 general points of 𝒳\mathcal{X}, or

  2. (2)

    K𝒳/BC2g(B)-K_{\mathcal{X}/B}\cdot C\geq 2g(B)

then a general deformation of CC is relatively free.

Finally, we will need the following observation.

Lemma 3.9.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration of relative dimension 11. Let CC be a section of π\pi. If K𝒳/BC2g(B)-K_{\mathcal{X}/B}\cdot C\geq 2g(B) then for any codimension 22 subset ZZ of 𝒳\mathcal{X} there is a deformation of CC that avoids ZZ.

Lemma 3.10.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Let CC be a relatively free section of π\pi that is general in its family (and thus avoids the singular locus of 𝒳\mathcal{X}). Suppose that either:

  1. (1)

    the normal bundle of CC is semistable and K𝒳/BC5g(B)-K_{\mathcal{X}/B}\cdot C\geq 5g(B), or

  2. (2)

    the normal bundle of CC is unstable and indecomposable and K𝒳/BC6g(B)2-K_{\mathcal{X}/B}\cdot C\geq 6g(B)-2, or

  3. (3)

    the normal bundle of CC is split and the two summands 1,2\mathcal{L}_{1},\mathcal{L}_{2} satisfy deg(i)2g(B)\deg(\mathcal{L}_{i})\geq 2g(B) for i=1,2i=1,2.

Then for any codimension 22 subset ZZ of 𝒳\mathcal{X} there is a deformation of CC that avoids ZZ. In particular, this statement holds for any section CC whose deformations go through 2g(B)+1\geq 2g(B)+1 general points of 𝒳\mathcal{X}.

We will only prove Lemma 3.10, since the proof of Lemma 3.9 is similar but easier.

Proof.

In each of the three circumstances above we have h1(C,NC/𝒳(p))=0h^{1}(C,N_{C/\mathcal{X}}(-p))=0 for every point pp in CC. Thus the space Sec(𝒳/B,p)\mathrm{Sec}(\mathcal{X}/B,p) has the expected dimension, and the first statement follows easily. The second statement follows from Corollary 3.7 and Riemann-Roch. ∎

3.3. Gluing criterion

We will need the following lemma allowing us to glue relatively free sections to free vertical curves.

Lemma 3.11.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration. Suppose that f:C𝒳f:C\to\mathcal{X} is a stable map satisfying the following conditions:

  1. (1)

    The domain of CC is a genus g(B)g(B) curve which consists of a single curve C0C_{0} isomorphic to BB attached to several trees of rational curves, and these trees of rational curves are contracted by πf\pi\circ f.

  2. (2)

    The image of ff is contained in the smooth locus of 𝒳\mathcal{X}.

  3. (3)

    The restriction of ff to C0C_{0} is an isomorphism from C0C_{0} to a relatively free section of π\pi.

  4. (4)

    For each rational component TiT_{i} of CC, fT𝒳|Tif^{*}T_{\mathcal{X}}|_{T_{i}} is globally generated.

Then ff is a smooth point of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}). Furthermore assume that ff is an immersion on a neighborhood of every node on C0C_{0}. Then a general point of the corresponding component of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) parametrizes a relatively free section of π\pi.

The proof is a combination of well-known techniques in deformation theory; see for example [Tes09, Section 1] and [GHS03, Lemma 2.6].

3.4. Shen’s work on curves with unstable normal bundles

Suppose that a section CC has unbalanced normal bundle. If we look at all deformations of CC which contain a suitable number of general points then the resulting sections sweep out a surface Σ\Sigma in 𝒳\mathcal{X}. In [She12] Shen studied the geometry of this surface Σ\Sigma in the setting of rational curves on 33-folds with unbalanced normal bundles. In this section, we will make a few modifications to develop a similar story for sections of higher genus. The goal is Proposition 3.14 which we later use to produce rational curves in Σ\Sigma by applying Bend-and-Break to a large family of sections.

Suppose that we have a del Pezzo fibration π:𝒳B\pi:\mathcal{X}\rightarrow B. Let MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) be a component generically parametrizing relatively free sections. Let CC be a general section parametrized by MM. We assume that NC/𝒳N_{C/\mathcal{X}} is unstable so that it fits into the maximal destabilizing exact sequence

02NC/𝒳10.0\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0.

We define h=K𝒳/BCh=-K_{\mathcal{X}/B}\cdot C and assume that h5g(B)2h\geq 5g(B)-2. As the general section parametrized by MM is relatively free, by definition we have h1(C,NC/𝒳)=0h^{1}(C,N_{C/\mathcal{X}})=0. This implies that h1(C,1)=0h^{1}(C,\mathcal{L}_{1})=0, and since deg(2)>deg(NC/𝒳)/2=h/2\deg(\mathcal{L}_{2})>\deg(N_{C/\mathcal{X}})/2=h/2 we also have h1(C,2)=0h^{1}(C,\mathcal{L}_{2})=0. Define k=deg(1)+1g(B)k=\deg(\mathcal{L}_{1})+1-g(B). Since h1(C,1)=0h^{1}(C,\mathcal{L}_{1})=0 we must have have k1k\geq 1.

Assume that deg(2)>deg(1)+1\deg(\mathcal{L}_{2})>\deg(\mathcal{L}_{1})+1. Fix kk general points q1,,qkq_{1},\ldots,q_{k} on CC so that H1(C,i(q1qk))=0H^{1}(C,\mathcal{L}_{i}(-q_{1}-\ldots-q_{k}))=0. Then the deformation space Sec(𝒳/B;q1,,qk)\mathrm{Sec}(\mathcal{X}/B;q_{1},\cdots,q_{k}) is smooth at CC and at least 22 dimensional. Denote the unique component of Sec(𝒳/B;q1,,qk)\mathrm{Sec}(\mathcal{X}/B;q_{1},\cdots,q_{k}) that contains CC by M(C;q1,,qk)M(C;q_{1},\cdots,q_{k}). As discussed in Section 3.1.2 we have an inclusion M(C;q1,,qk)MM(C;q_{1},\cdots,q_{k})\subset M. Let

𝒰(C;q1,,qk)M(C;q1,,qk)\mathcal{U}(C;q_{1},\cdots,q_{k})\to M(C;q_{1},\cdots,q_{k})

be the universal family with the evaluation map v:𝒰(C;q1,,qk)𝒳v:\mathcal{U}(C;q_{1},\cdots,q_{k})\to\mathcal{X}. Since by Proposition 3.6 deformations of CC can not go through more than kk general points of 𝒳\mathcal{X}, the closure Σ\Sigma of the image v(𝒰(C;q1,,qk))v(\mathcal{U}(C;q_{1},\cdots,q_{k})) is a surface. Let ΣΣ\Sigma^{\prime}\to\Sigma be the normalization. By the universal property of normalizations there is some neighborhood of the curve CC in 𝒰(C;q1,,qk)\mathcal{U}(C;q_{1},\cdots,q_{k}) such that the evaluation map vv restricted to this neighborhood factors through Σ\Sigma^{\prime}. Then we have

Lemma 3.12.

Suppose MM parametrizes a relatively free section CC as above. Then Σ\Sigma^{\prime} is smooth along C{q1,,qk}C\setminus\{q_{1},\cdots,q_{k}\}.

Proof.

We claim that 2(q1qk)\mathcal{L}_{2}(-q_{1}-\cdots-q_{k}) is basepoint free. If deg(2)deg(1)+g(B)12g(B)\deg(\mathcal{L}_{2})-\deg(\mathcal{L}_{1})+g(B)-1\geq 2g(B), then deg(2(q1qk))2g(B)\deg(\mathcal{L}_{2}(-q_{1}-\cdots-q_{k}))\geq 2g(B) and thus this line bundle is basepoint free. Otherwise deg(2)deg(1)g(B)\deg(\mathcal{L}_{2})-\deg(\mathcal{L}_{1})\leq g(B). Since we have 2deg(1)+g(B)deg(1)+deg(2)5g(B)22\deg(\mathcal{L}_{1})+g(B)\geq\deg(\mathcal{L}_{1})+\deg(\mathcal{L}_{2})\geq 5g(B)-2, in this situation

k=deg(1)g(B)+1g(B).k=\deg(\mathcal{L}_{1})-g(B)+1\geq g(B).

Thus the class [2(q1qk)][\mathcal{L}_{2}(-q_{1}-\cdots-q_{k})] in Pic(B)\mathrm{Pic}(B) is generic and has degree g(B)+1\geq g(B)+1 so that it is basepoint free. Now our assertion follows from the argument of [She12, Lemma 2.4]. Indeed, the destabilizing exact sequence shows that for any qC{q1,,qk}q\in C\setminus\{q_{1},\cdots,q_{k}\} the map H0(C,NC/𝒳)NC/𝒳|qH^{0}(C,N_{C/\mathcal{X}})\to N_{C/\mathcal{X}}|_{q} has rank 11. We are thus in a situation where we can apply [She12, Lemma 2.3]. ∎

Then arguing as in [She12, Proposition 2.5], we have

Lemma 3.13.

Suppose MM parametrizes a relatively free section CC as above. Let k=deg(1)g(B)+1k=\deg(\mathcal{L}_{1})-g(B)+1 and choose general points q1,,qkq_{1},\cdots,q_{k} on CC. The surface Σ=Σ(C;q1,,qk)\Sigma=\Sigma(C;q_{1},\cdots,q_{k}) is independent of q1,,qkq_{1},\cdots,q_{k}.

Proof.

We already showed that 2(q1qk)\mathcal{L}_{2}(-q_{1}-\cdots-q_{k}) is basepoint free. Hence for any qC{q1,,qk}q\in C\setminus\{q_{1},\cdots,q_{k}\} we have

h0(C,NC/𝒳(q1qkq))=h0(C,NC/𝒳(q1qk))1.h^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\cdots-q_{k}-q))=h^{0}(C,N_{C/\mathcal{X}}(-q_{1}-\cdots-q_{k}))-1.

Thus the arguments in [She12, Proposition 2.5] yield our assertion. ∎

Finally arguing as in [She12, Corollary 2.7], we obtain

Proposition 3.14.

Suppose MM parametrizes a relatively free section CC as above. Denote the maximal destabilizing exact sequence for the unstable normal bundle as

02NC/𝒳10.0\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0.

Let k=deg(1)g(B)+1k=\deg(\mathcal{L}_{1})-g(B)+1 and choose general points q1,,qkq_{1},\cdots,q_{k} on CC. Let Σ=Σ(C;q1,,qk)\Sigma=\Sigma(C;q_{1},\cdots,q_{k}) and let ΣΣ\Sigma^{\prime}\to\Sigma be the normalization. Then Σ\Sigma^{\prime} is smooth along the strict transform of CC and we have NΣ/𝒳|C=1N_{\Sigma^{\prime}/\mathcal{X}}|_{C}=\mathcal{L}_{1} and NC/Σ=2N_{C/\Sigma^{\prime}}=\mathcal{L}_{2}.

4. Breaking curves on surfaces

The following conjecture is essential for understanding sections of Fano fibrations.

Conjecture 4.1 (Movable Bend-and-Break for sections).

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration. There is a constant Q=Q(𝒳)Q=Q(\mathcal{X}) such that the following holds. Suppose that CC is a relatively free section of π\pi satisfying K𝒳/BC>Q(𝒳)-K_{\mathcal{X}/B}\cdot C>Q(\mathcal{X}). Then CC deforms (as a stable map) to a union of a relatively free section with a π\pi-vertical free curve.

In this section we prove Conjecture 4.1 for sections of surfaces over BB. We first need a couple lemmas about the intersection theory of reducible fibers of a map from a surface to a curve.

Lemma 4.2 ([LT19a] Lemma 4.3).

Let YY be a smooth projective surface with a morphism π:YB\pi:Y\rightarrow B such that a general fiber of π\pi is isomorphic to 1\mathbb{P}^{1}. Let FF be a singular fiber of π\pi with components {Ei}i=1r\{E_{i}\}_{i=1}^{r}. Suppose that E1E_{1} is a (1)(-1)-curve that has multiplicity 11 in the fiber FF. Then there is another (1)(-1)-curve in the fiber FF.

Corollary 4.3.

Let YY be a smooth projective surface with a morphism π:YB\pi:Y\rightarrow B such that a general fiber of π\pi is isomorphic to 1\mathbb{P}^{1}. Let CC be a movable section of π\pi. Then there is a birational morphism ϕ:Y𝔽\phi:Y\to\mathbb{F} to a ruled surface 𝔽\mathbb{F} which is an isomorphism on a neighborhood of CC. This ruled surface satisfies

KY/BCneg(𝔽,K𝔽/B)g(B).K_{Y/B}\cdot C\leq\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq g(B).

(where neg\mathrm{neg} is defined as in Definition 2.3.)

Proof.

Every reducible fiber of π\pi will carry a (1)(-1)-curve. Lemma 4.2 guarantees that if this (1)(-1)-curve intersects CC then there is another π\pi-vertical (1)(-1)-curve in the same fiber that is disjoint from CC. Thus we may inductively contract (1)(-1)-curves that are disjoint from CC to obtain 𝔽\mathbb{F}.

To see the final statement, write ρCC0+kF\rho_{*}C\equiv C^{\prime}_{0}+kF where C0C^{\prime}_{0} is a section of minimal height and FF is a general fiber of the projective bundle. Since ρC\rho_{*}C is movable we have ρCC00\rho_{*}C\cdot C^{\prime}_{0}\geq 0. Thus by applying adjunction to ρC\rho_{*}C we see

KY/BC=K𝔽/BρC=(ρC)2=ρC(C0+kF)k.-K_{Y/B}\cdot C=-K_{\mathbb{F}/B}\cdot\rho_{*}C=(\rho_{*}C)^{2}=\rho_{*}C\cdot(C^{\prime}_{0}+kF)\geq k.

On the other hand

0ρCC0=C02+k.0\leq\rho_{*}C\cdot C^{\prime}_{0}=C^{\prime 2}_{0}+k.

Since K𝔽/BC0=C02-K_{\mathbb{F}/B}\cdot C^{\prime}_{0}=C^{\prime 2}_{0} this yields the first inequality. The second inequality holds true for every ruled surface and is a consequence of Lemma 2.12. ∎

It will be helpful to have a numerical version of Corollary 4.3.

Definition 4.4.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration such that 𝒳\mathcal{X} is smooth. An intersection profile λ\lambda for π\pi is a choice of a component F0F_{0} in each fiber FF of π\pi such that F0F_{0} has multiplicity 11 in FF. We will denote the finite set of intersection profiles for π\pi by Λ\Lambda.

Note that any section CC naturally identifies an intersection profile for π\pi by selecting the components of fibers which meet CC. By repeating the arguments of Corollary 4.3 we obtain:

Lemma 4.5.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration of relative dimension 11. Fix an intersection profile λ\lambda for π\pi. Then there is a birational morphism ϕ:𝒳𝔽\phi:\mathcal{X}\to\mathbb{F} to a ruled surface 𝔽\mathbb{F} over BB such that ϕ\phi contracts every component of every fiber not identified by λ\lambda.

Lemma 4.6.

Let YY be a smooth projective surface with a morphism π:YB\pi:Y\rightarrow B such that a general fiber of π\pi is isomorphic to 1\mathbb{P}^{1}. Let FF be a reducible fiber of π\pi with components {Ei}i=1r\{E_{i}\}_{i=1}^{r}. We assume that E1E_{1} and E2E_{2} have multiplicity 11 in FF. Suppose Q=i=1raiEiQ=\sum_{i=1}^{r}a_{i}E_{i} is an effective \mathbb{Q}-divisor such that

QEj={1 if j=11 if j=20 otherwiseQ\cdot E_{j}=\begin{cases}1&\text{ if }j=1\\ -1&\text{ if }j=2\\ 0&\text{ otherwise}\end{cases}

Then we have

KYQ>0.-K_{Y}\cdot Q>0.
Proof.

We prove this by induction on the number of components rr of FF. When FF consists of two components our assertion is trivial.

Suppose that rr is greater than 22. If some component EjE_{j} with j1,2j\neq 1,2 is a (1)(-1)-curve, then we can contract EjE_{j} via ϕ:YY\phi:Y\to Y^{\prime} and apply the induction hypothesis to deduce that

KYQ=KYϕQ>0.-K_{Y}\cdot Q=-K_{Y^{\prime}}\cdot\phi_{*}Q>0.

So we may assume that there is no (1)(-1)-curve other than E1E_{1} and E2E_{2}. Suppose that E1E_{1} is a (1)(-1)-curve. By Lemma 4.2 FF must contain a different (1)(-1)-curve, and by the argument above we may assume this is E2E_{2}. Similarly, if E2E_{2} is a (1)(-1)-curve then we may assume that E1E_{1} is also. Thus we have reduced to the case when E1E_{1} and E2E_{2} are both (1)(-1)-curves.

Since the multiplicity of E2E_{2} in FF is 11, there is a unique curve E3E_{3} adjacent to E2E_{2}. If we contract E2E_{2} and denote the blow down by ϕ:YY\phi:Y\rightarrow Y^{\prime}, then we have

ϕQϕ(Ej)={1 if j=11 if j=30 otherwise\phi_{*}Q\cdot\phi_{*}(E_{j})=\begin{cases}1&\text{ if }j=1\\ -1&\text{ if }j=3\\ 0&\text{ otherwise}\end{cases}

Then we have

KYQ=KYϕQ+1>0-K_{Y}\cdot Q=-K_{Y^{\prime}}\cdot\phi_{*}Q+1>0

by the induction hypothesis. ∎

The following theorem is the statement of Movable Bend-and-Break for sections of surface fibrations.

Theorem 4.7.

Let π:YB\pi:Y\to B be a Fano fibration of relative dimension 11. Suppose that CC is a section satisfying

KY/BCmax{2,2g(B)+1,4g(B)+1neg(Y,KY/B)}.-K_{Y/B}\cdot C\geq\max\{2,2g(B)+1,4g(B)+1-\mathrm{neg}(Y,-K_{Y/B})\}.

Then there is a relatively free section C0C_{0} and a general fiber FF such that

CalgC0+F.C\sim_{alg}C_{0}+F.

Furthermore CC deforms as a stable map to a morphism whose domain has two components where each component is mapped birationally onto either C0C_{0} or FF.

Proof.

Let n=KY/BC+1g(B)n=-K_{Y/B}\cdot C+1-g(B). By our degree assumption we know that H1(C,NC/Y)=0H^{1}(C,N_{C/Y})=0. Since general points impose codimension 11 conditions on the moduli space of sections, we see that deformations of CC contain nn general points of YY. Thus there is a 11-parameter family of curves through n1n-1 general points of YY. By Lemma 2.11 CC deforms into the union of a section with some π\pi-vertical curves, at least one of which goes through a general point. Thus we can write

CalgC0+mF+TC\sim_{alg}C_{0}+mF+T

where FF denotes a general fiber of π\pi, m1m\geq 1, and TT is an effective π\pi-vertical curve which does not deform.

Fix a fiber F0F_{0} and let T0T_{0} denote the sum of the components of TT contained in F0F_{0}. By [Mat02, Lemma 1-2-10] there are two possibilities: either T0T_{0} is proportional to a multiple of F0F_{0} or T0T_{0} has non-vanishing intersection against some components of F0F_{0}. In the latter case T0T_{0} must have exactly the intersection pattern as in the statement of Lemma 4.6. By applying Lemma 4.6 and summing over all fibers, we conclude that KY/BT>0-K_{Y/B}\cdot T>0 unless T=0T=0. We let bb denote this non-negative constant.

We divide the argument into two cases. First suppose that H1(C0,NC0/Y)=0H^{1}(C_{0},N_{C_{0}/Y})=0. Since KY/BC0+1g(B)=n2mb-K_{Y/B}\cdot C_{0}+1-g(B)=n-2m-b, Proposition 3.5 shows that C0C_{0} can only go through n2mbn-2m-b general points. A fiber FF can go through only 11 general point and TT cannot go through any general points. But the broken curve C0+mF+TC_{0}+mF+T should pass through n1n-1 general points of YY. Thus b=0b=0 and m=1m=1 yielding the desired expression with C=C0C^{\prime}=C_{0}. We see that C0C_{0} is relatively free using Corollary 3.8.

Next suppose that H1(C0,NC0/Y)0H^{1}(C_{0},N_{C_{0}/Y})\neq 0. We will show that this case is impossible using our degree assumption. The maximum number of general points that C0C_{0} can contain is bounded above by H0(C0,NC0/Y)g(B)H^{0}(C_{0},N_{C_{0}/Y})\leq g(B). Thus we must have mng(B)1m\geq n-g(B)-1 so that the entire curve can contain n1n-1 points. But we also know that

neg(Y,KY/B)\displaystyle\mathrm{neg}(Y,-K_{Y/B}) KY/BC0\displaystyle\leq-K_{Y/B}\cdot C_{0}
=n1+g(B)2mb\displaystyle=n-1+g(B)-2m-b
3g(B)+1n\displaystyle\leq 3g(B)+1-n
=4g(B)+KY/BC\displaystyle=4g(B)+K_{Y/B}\cdot C

which contradicts our degree assumption.

To see the final statement, choose a deformation from CC to C0+FC_{0}+F. The generic curve in this deformation family will be a section, yielding a map σ:BY\sigma:B\to Y. Taking a closure in the space of stable maps, we obtain a limit stable map whose image in YY is C0+FC_{0}+F which satisfies the desired properties. ∎

The following example illustrates that the intersection bound in Theorem 4.7 must depend on the choice of surface YY and not just the genus of BB. In particular, this justifies the presence of neg(Y,KY/B)\mathrm{neg}(Y,-K_{Y/B}) in the statement of Theorem 4.7.

Example 4.8.

Let 𝔽e\mathbb{F}_{e} denote the Hirzebruch surface whose rigid section has self-intersection e-e and let π:𝔽e1\pi:\mathbb{F}_{e}\to\mathbb{P}^{1} denote the projective bundle structure. Every movable section CC on 𝔽e\mathbb{F}_{e} satisfies K𝔽e/1Ce-K_{\mathbb{F}_{e}/\mathbb{P}^{1}}\cdot C\geq e. Thus Theorem 4.7 can only apply to a section CC when the height of CC is e+1\geq e+1.

We also prove a breaking statement which deals with numerical equivalence.

Proposition 4.9.

Let π:YB\pi:Y\to B be a Fano fibration of relative dimension 11. Let CC be a general member of a dominant family of sections on YY. Let ρ:Y𝔽\rho:Y\to\mathbb{F} be the birational map to a ruled surface 𝔽\mathbb{F} obtained by applying Corollary 4.3 to YY and CC. Then:

  1. (1)

    We have CC0+T+kFC\equiv C_{0}+T+kF where TT is an effective π\pi-vertical curve, C0C_{0} is a section on YY satisfying KY/BC0neg(𝔽,K𝔽/B)-K_{Y/B}\cdot C_{0}\leq\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}), and k=12(KY/BC)12neg(𝔽,K𝔽/B)k=\frac{1}{2}(-K_{Y/B}\cdot C)-\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}).

  2. (2)

    Define

    s=12(KY/BC)+12neg(𝔽,K𝔽/B)+max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}s=\frac{1}{2}(K_{Y/B}\cdot C)+\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}

    Then for any r0r\geq 0, there is a unique dominant family of relatively free sections C1C_{1} on YY which satisfy

    C1C+(s+r)FC_{1}\equiv C+\left(s+r\right)F

    where FF denotes a general fiber of π\pi. For any 2r+12r+1 general points of YY we can find a deformation of C1C_{1} containing these 2r+12r+1 points.

Proof.

Applying Corollary 4.3 to YY and CC we find a ruled surface 𝔽\mathbb{F} and a birational map ρ:Y𝔽\rho:Y\to\mathbb{F} which is an isomorphism on a neighborhood of CC.

Let C0C^{\prime}_{0} denote a section on 𝔽\mathbb{F} with minimal self intersection, so that K𝔽/BC0=neg(𝔽,K𝔽/B)-K_{\mathbb{F}/B}\cdot C^{\prime}_{0}=\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}). Then we have ρCC0+kF\rho_{*}C\equiv C^{\prime}_{0}+kF where FF denotes a general fiber of the projective bundle map and k=12(KY/BC)12neg(𝔽,K𝔽/B)k=\frac{1}{2}(-K_{Y/B}\cdot C)-\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}). Write ρC0=C0+T\rho^{*}C^{\prime}_{0}=C_{0}+T. Lemma 4.6 implies that KY/BT0K_{Y/B}\cdot T\leq 0, proving (1).

To prove (2), we need to appeal to the geometry of ruled surfaces. Define

m=max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}m=\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}

so that s=k+ms=-k+m. Suppose that \mathcal{E} is a rank 22 bundle such that 𝔽=B()\mathbb{F}=\mathbb{P}_{B}(\mathcal{E}). After twisting \mathcal{E}, we may suppose that the section C0C^{\prime}_{0} constructed above is a section of 𝒪𝔽/B(1)\mathcal{O}_{\mathbb{F}/B}(1).

First suppose that \mathcal{E} is indecomposable. Since \mathcal{E} has a section, by Lemma 2.12 we see that (D)\mathcal{E}(D) is globally generated for any divisor DD on BB of degree at least 4g(B)24g(B)-2. In particular, (D)\mathcal{E}(D) is globally generated for any DD of degree m+rm+r with r0r\geq 0. Then sections of (D)\mathcal{E}(D) yield a basepoint free family of sections C1C^{\prime}_{1} on 𝔽\mathbb{F} with numerical class

ρC+(k+m+r)F.\rho_{*}C+(-k+m+r)F.

Furthermore, the additional twist by rFrF guarantees that we can find deformations of C1C^{\prime}_{1} through any 2r+12r+1 general points of 𝔽\mathbb{F}. Since the same logic applies if we replace DD by any numerically equivalent divisor, we see that the component of Sec(𝔽/B)\mathrm{Sec}(\mathbb{F}/B) containing C1C^{\prime}_{1} is a projective bundle over Jac(B)\mathrm{Jac}(B), and in particular, is irreducible. To construct the desired family of sections on YY, note that when C1C^{\prime}_{1} and FF are general in their respective families they avoid all ρ\rho-exceptional centers by Lemma 3.9. Thus by pulling back we obtain sections of the desired class on YY. Note that pushforward and pullback by ρ\rho induce birational maps on the moduli space of sections of this class, so that sections on YY of the given numerical class also must form an irreducible family.

Second suppose that \mathcal{E} is decomposable. Since C0C^{\prime}_{0} is a minimal section, we can write =1𝒪\mathcal{E}=\mathcal{L}_{1}\oplus\mathcal{O}. Note that we have deg(1)=neg(𝔽,K𝔽/B)\deg(\mathcal{L}_{1})=\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}). Thus, (D)\mathcal{E}(D) is globally generated for any divisor DD on BB of degree 2g(B)neg(𝔽,K𝔽/B)\geq 2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}). We conclude by the same argument as before. ∎

5. Non-dominant families of sections

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. Suppose that MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is a component which defines a non-dominant family of sections. The main goal of this section is to show that if the height of the sections parametrized by MM is sufficiently high then these sections sweep out a surface YY with a(Yη,K𝒳/B|Y)a(Xη,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})\geq a(X_{\eta},-K_{\mathcal{X}/B}). Using this result we show there is a finite set of surfaces which contain all such families of sections.

We start with a couple results concerning surfaces swept out by sections. The first lemma shows that if we have a family NN of surfaces Y𝒳Y\subset\mathcal{X} satisfying a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}) then we can stratify the parameter space NN according to the set of minimal models of YY.

Lemma 5.1.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Suppose that we have a bounded family 𝒮N\mathcal{S}\to N where each fiber is a surface Y𝒳Y\subset\mathcal{X} such that YηY_{\eta} is geometrically irreducible and a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}). Then there is a stratification {Ni}\{N_{i}\} of NN into locally closed subsets with the following properties:

  1. (1)

    There is a family 𝒮Ni\mathcal{S}\to N_{i} such that every fiber is a resolution of the corresponding surface Y𝒳Y\subset\mathcal{X}.

  2. (2)

    There is a base change WiNiW_{i}\to N_{i} such that if we fix a resolution Y~\widetilde{Y} parametrized by NiN_{i} and fix a birational map ϕ:Y~𝔽\phi:\widetilde{Y}\to\mathbb{F} as in Lemma 4.5 then the base change 𝒮Wi\mathcal{S}_{W_{i}} admits a birational morphism over WiW_{i} to a family where every fiber is isomorphic to a ruled surface 𝔽wB\mathbb{F}_{w}\to B and there is a point in WiW_{i} representing Y~\widetilde{Y} such that the restriction of the map to this fiber is ϕ\phi.

Furthermore, we may assume that the degrees of the terms in the Harder-Narasimhan filtration for the bundle \mathcal{E} that defines 𝔽w\mathbb{F}_{w} is constant for the entire family.

Proof.

By repeatedly taking resolutions and restricting to the smooth locus we can stratify NN into a finite collection of irreducible locally closed subsets NiN_{i} such that over each NiN_{i} there is a smooth family of surfaces 𝒮iNi\mathcal{S}_{i}\to N_{i} where the fiber over a point in NiN_{i} is a resolution of the corresponding point in NN. The main step is to show that after repeatedly replacing NiN_{i} by a non-empty open subset we may ensure the desired properties hold for NiN_{i}. For notational clarity we will continue to call this open set NiN_{i} even while making these changes.

Since every surface YY satisfies a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}), every resolution Y~\widetilde{Y} will admit a morphism to BB whose general fiber is birational to an irreducible K𝒳/B-K_{\mathcal{X}/B}-conic. In particular, the Picard rank of Y~\widetilde{Y} is the same as the rank of H2(Y~,)H^{2}(\widetilde{Y},\mathbb{Z}). Thus it is constant in each smooth family. Moreover the Néron-Severi groups of Y~\widetilde{Y} form a local system over NiN_{i}.

Take a base change WiNiW_{i}\to N_{i} that kills the monodromy action on the Néron-Severi groups of the fibers over NiN_{i}. We let 𝒮Wi\mathcal{S}_{W_{i}} denote the smooth family obtained by base change. Note that the restriction map N1(𝒮Wi)N1(Y~w)N^{1}(\mathcal{S}_{W_{i}})\to N^{1}(\widetilde{Y}_{w}) is surjective for every surface Y~w\widetilde{Y}_{w} in our family.

For any fiber Y~w\widetilde{Y}_{w} in our family consider the components of the reducible fibers of Y~wB\widetilde{Y}_{w}\to B. Using a relative Hilbert scheme argument, after perhaps shrinking WiW_{i} (and NiN_{i}) we obtain a finite collection of irreducible divisors DiD_{i} on 𝒮Wi\mathcal{S}_{W_{i}} such that the intersection of the DiD_{i} with the surfaces Y~i\widetilde{Y}_{i} are exactly the components of the reducible fibers. Due to the monodromy condition, after perhaps shrinking WiW_{i} (and NiN_{i}) again we see that in fact the restriction of DiD_{i} to each surface is irreducible and that when iji\neq j the restrictions of DiD_{i} and DjD_{j} to every fiber in our family are different components.

Using the constancy of intersection numbers, if the restriction of DiD_{i} to some Y~w\widetilde{Y}_{w} is a (1)(-1)-curve then it is a (1)(-1)-curve in every fiber. By running the relative MMP for 𝒮Wi\mathcal{S}_{W_{i}} over Wi×BW_{i}\times B we can contract the divisor DiD_{i}, and this contraction will result in the contraction of the corresponding (1)(-1)-curve on each fiber. This shows that any morphism ϕ:Y~w𝔽\phi:\widetilde{Y}_{w}\to\mathbb{F} obtained by contracting (1)(-1)-curves in fibers can be spread out to the entire family over WiW_{i}.

Finally, by Theorem 2.14 we can shrink NiN_{i} so that for any of our families of ruled surfaces obtained as above the bundles \mathcal{E} defining the ruled surfaces have the property that the terms in the Harder-Narasimhan filtration are of constant degree. This guarantees that all the desired properties hold for our new NiN_{i}. Repeating the argument on the complement and appealing to Noetherian induction we deduce the desired statement. ∎

Next we show that if we have a family NN of surfaces Y𝒳Y\subset\mathcal{X} satisfying a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}) then we can deform a section in one surface YY into other surfaces which lie in the same stratum as YY.

Corollary 5.2.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Suppose that we have a bounded family 𝒮N\mathcal{S}\to N where each fiber is a surface Y𝒳Y\subset\mathcal{X} such that YηY_{\eta} is geometrically irreducible and a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}). Let {Ni}\{N_{i}\} be the stratification of NN as in Lemma 5.1.

Let MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) be a component. Suppose that some sublocus of MM parametrizes a family of sections which sweep out a surface YY parametrized by NiN_{i}. Take the strict transform of these sections on the resolution Y~\widetilde{Y} identified by NiN_{i} and consider the corresponding birational map ρ:Y~𝔽\rho:\widetilde{Y}\to\mathbb{F} as in Corollary 4.3. Suppose that the sections C𝔽C_{\mathbb{F}} on 𝔽\mathbb{F} obtained in this way satisfy

K𝔽/BC𝔽neg(𝔽,K𝔽/B)+2max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}.-K_{\mathbb{F}/B}\cdot C_{\mathbb{F}}\geq\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+2\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}.

Then for every surface SS parametrized by NiN_{i} there is a unique component of Sec(S~/B)\mathrm{Sec}(\widetilde{S}/B) parametrizing sections of anticanonical degree K𝔽/BC𝔽-K_{\mathbb{F}/B}\cdot C_{\mathbb{F}} which have intersection profile compatible with the birational map to 𝔽\mathbb{F} and the image of these sections in 𝒳\mathcal{X} is parametrized by MM. In particular every surface parametrized by NiN_{i} is swept out by sections parametrized by MM.

Proof.

Lemma 5.1 yields a base change WiNiW_{i}\to N_{i} and a universal family 𝒮WiWi\mathcal{S}_{W_{i}}\to W_{i} such that 𝒮Wi\mathcal{S}_{W_{i}} admits a birational map to a family of ruled surfaces 𝒯Wi\mathcal{T}_{W_{i}} over WiW_{i} whose restriction to Y~\widetilde{Y} coincides with ρ\rho. Due to our height restriction on C𝔽C_{\mathbb{F}}, Proposition 4.9 shows that every ruled surface in 𝒯Wi\mathcal{T}_{W_{i}} admits a unique dominant family of sections which has the same anticanonical height as C𝔽C_{\mathbb{F}}. Using the description of these curves as sections of a twist of the bundle defining the ruled surface, we see that in fact all these sections form a single family on 𝒯Wi\mathcal{T}_{W_{i}}. By taking the strict transform of this family on 𝒮Wi\mathcal{S}_{W_{i}} and pushing forward to 𝒳\mathcal{X} we obtain the desired statement. ∎

The following theorem is the main result in this section.

Theorem 5.3.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. Let MM denote a component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing sections CC satisfying

K𝒳/BCC(𝒳):=max{\displaystyle-K_{\mathcal{X}/B}\cdot C\geq C(\mathcal{X}):=\max\{ 3g(B)+1,2neg(𝒳,K𝒳/B)+6g(B)2,\displaystyle 3g(B)+1,-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+6g(B)-2,
2g(B)1+2max{4g(B)2,3g(B)1neg(𝒳,K𝒳/B)}}.\displaystyle 2g(B)-1+2\max\{4g(B)-2,3g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}\}.

Suppose that the closure of the locus swept out by the corresponding sections is a surface YY. Then a(Yη,K𝒳/B|Y)a(Xη,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})\geq a(X_{\eta},-K_{\mathcal{X}/B}).

If equality of aa-invariants is achieved, then these sections satisfy the height bound of Corollary 5.2 with respect to the surface YY. Moreover, YY is swept out by a (possibly different) family of sections of height at most 2g(B)1+2max{4g(B)2,3g(B)1neg(𝒳,K𝒳/B)}2g(B)-1+2\max\{4g(B)-2,3g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}.

Proof.

Let ϕ:Y~Y\phi:\widetilde{Y}\to Y denote a resolution of singularities. Let C~\widetilde{C} denote the strict transform of a general deformation of the section CC. By assumption the deformations of C~\widetilde{C} are Zariski dense on Y~\widetilde{Y}; thus the natural map ψ:Y~B\psi:\widetilde{Y}\to B is an algebraic fiber space. Moreover our height bound guarantees that there is at least a 33-parameter family of deformations of CC on 𝒳\mathcal{X}, and hence also of C~\widetilde{C} on Y~\widetilde{Y}. By Bend-and-Break we see that Y~\widetilde{Y} is generically a 1\mathbb{P}^{1}-bundle over the base.

Since by assumption K𝒳/BC3g(B)+1-K_{\mathcal{X}/B}\cdot C\geq 3g(B)+1, the dimension of the space of deformations of CC is bounded below by 3g(B)+1+22g(B)=g(B)+33g(B)+1+2-2g(B)=g(B)+3. Since the deformations of CC are contained in YY, we can find a deformation of C~\widetilde{C} through g(B)+3g(B)+3 general points of Y~\widetilde{Y}. This implies that H0(C~,NC~/Y~)g(B)+3H^{0}(\widetilde{C},N_{\widetilde{C}/\widetilde{Y}})\geq g(B)+3, and in particular by Corollary 3.8 H1(C~,NC~/Y~)=0H^{1}(\widetilde{C},N_{\widetilde{C}/\widetilde{Y}})=0. Thus if MM denotes the the family of deformations of C~\widetilde{C} on Y~\widetilde{Y}, then

dim(M)=KY~/BC~+(1g(B)).\dim(M)=-K_{\widetilde{Y}/B}\cdot\widetilde{C}+(1-g(B)).

Since MM has at least the expected dimension on 𝒳\mathcal{X}, we obtain

(KY~/BϕK𝒳/B|Y)C~g(B)1.(K_{\widetilde{Y}/B}-\phi^{*}K_{\mathcal{X}/B}|_{Y})\cdot\widetilde{C}\leq g(B)-1.

Apply Corollary 4.3 to find a ruled surface 𝔽\mathbb{F} and a birational map ρ:Y~𝔽\rho:\widetilde{Y}\to\mathbb{F} which is an isomorphism on a neighborhood of C~\widetilde{C}. As in Proposition 4.9 (1) we can write C~C~0+kF+T\widetilde{C}\equiv\widetilde{C}_{0}+kF+T where FF is a general fiber of the map to BB and

k=12(KY~/BC~)12neg(𝔽,K𝔽/B).k=\frac{1}{2}(-K_{\widetilde{Y}/B}\cdot\widetilde{C})-\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}).

Then

g(B)1\displaystyle g(B)-1 KY~/BC~ϕK𝒳/B|YC~\displaystyle\geq K_{\widetilde{Y}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}
=KY~/BC~ϕK𝒳/B|YC~0+k(ϕK𝒳/B|YF)ϕK𝒳/B|YT\displaystyle=K_{\widetilde{Y}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}_{0}+k(-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F)-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot T
KY~/BC~+neg(𝒳,K𝒳/B)+k(ϕK𝒳/B|YF)\displaystyle\geq K_{\widetilde{Y}/B}\cdot\widetilde{C}+\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+k(-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F) (5.1)

where we have used the fact that K𝒳/B-K_{\mathcal{X}/B} is relatively nef at the last step. Suppose for a contradiction that there is an inequality a(Yη,K𝒳/B|Y)<a(Xη,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})<a(X_{\eta},-K_{\mathcal{X}/B}). This is equivalent to saying that ϕK𝒳/B|YF3-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F\geq 3. Rearranging and substituting in our value for kk, we find

12(KY~/BC~)32neg(𝔽,K𝔽/B)neg(𝒳,K𝒳/B)+g(B)1.\displaystyle\frac{1}{2}(-K_{\widetilde{Y}/B}\cdot\widetilde{C})\leq\frac{3}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+g(B)-1.

Using the inequality neg(𝔽,K𝔽/B)g(B)\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq g(B) from Corollary 4.3, we see that

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C KY~/BC~+g(B)1\displaystyle\leq-K_{\widetilde{Y}/B}\cdot\widetilde{C}+g(B)-1
2neg(𝒳,K𝒳/B)+6g(B)3.\displaystyle\leq-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+6g(B)-3.

contradicting our height bound.

Suppose now that the equality of aa-invariants is achieved so that ϕK𝒳/B|YF=2-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F=2. Using this to simplify Equation (5.1) we see that neg(𝒳,K𝒳/B)+g(B)1neg(𝔽,K𝔽/B)-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+g(B)-1\geq-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}). Furthermore we know neg(𝔽,K𝔽/B)g(B)\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq g(B) by Corollary 4.3. Thus

KY~/BC~\displaystyle-K_{\widetilde{Y}/B}\cdot\widetilde{C} ϕK𝒳/B|YC~+1g(B)\displaystyle\geq-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}+1-g(B)
g(B)+2max{4g(B)2,3g(B)1neg(𝒳,K𝒳/B)}\displaystyle\geq g(B)+2\max\{4g(B)-2,3g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}
neg(𝔽,K𝔽/B)+2max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}\displaystyle\geq\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+2\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\} (5.2)

proving the first claim. To see the last claim we will appeal to Proposition 4.9 (2) with r=0r=0. This guarantees the existence of a dominant family of sections C~1\widetilde{C}_{1} on Y~\widetilde{Y} which satisfy C~C~1sF\widetilde{C}\equiv\widetilde{C}_{1}-sF where

s=12(KY/BC)+12neg(𝔽,K𝔽/B)+max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}s=\frac{1}{2}(K_{Y/B}\cdot C)+\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}

and FF denotes a general fiber of π\pi. Since C~\widetilde{C} and C~1\widetilde{C}_{1} differ by a multiple of FF, the equality of aa-invariants shows that

g(B)1\displaystyle g(B)-1 KY~/BC~ϕK𝒳/B|YC~\displaystyle\geq K_{\widetilde{Y}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}
=KY~/BC~1ϕK𝒳/B|YC~1.\displaystyle=K_{\widetilde{Y}/B}\cdot\widetilde{C}_{1}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}_{1}.

Thus

ϕK𝒳/B|YC~1\displaystyle-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}_{1} g(B)1KY~/BC~1\displaystyle\leq g(B)-1-K_{\widetilde{Y}/B}\cdot\widetilde{C}_{1}
=g(B)1+neg(𝔽,K𝔽/B)+2max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}\displaystyle=g(B)-1+\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+2\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}
2g(B)1+2max{4g(B)2,3g(B)1neg(𝒳,K𝒳/B)}\displaystyle\leq 2g(B)-1+2\max\{4g(B)-2,3g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}

where the last step is given by the bound neg(𝔽,K𝔽/B)g(B)\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq g(B) from Corollary 4.3. Altogether this shows that YY is swept out by sections satisfying the desired height bound. ∎

Corollary 5.4.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. Then there is a proper closed subset V𝒳V\subsetneq\mathcal{X} such that any component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) parametrizing a non-dominant family of sections will parametrize sections contained in VV.

Proof.

Rigid sections are bounded in height and thus are contained in a closed subset. Thus it suffices to consider sections which sweep out a surface. By Theorem 5.3, any component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) parametrizing such a non-dominant family will satisfy one of the following properties:

  1. (1)

    MM will parametrize sections CC satisfying K𝒳/BC<C(𝒳)-K_{\mathcal{X}/B}\cdot C<C(\mathcal{X}), or

  2. (2)

    MM will parametrize sections CC satisfying K𝒳/BCC(𝒳)-K_{\mathcal{X}/B}\cdot C\geq C(\mathcal{X}) which sweep out a 22-dimensional subvariety YY satisfying

    a(Yη,K𝒳/B|Y)>a(𝒳η,K𝒳/B),a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})>a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}),

    or

  3. (3)

    MM will parametrize sections CC satisfying K𝒳/BCC(𝒳)-K_{\mathcal{X}/B}\cdot C\geq C(\mathcal{X}) which sweep out a 22-dimensional subvariety YY satisfying

    a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B})

    and which contains a section of height at most 2g(B)1+2max{4g(B)2,3g(B)1neg(𝒳,K𝒳/B)}2g(B)-1+2\max\{4g(B)-2,3g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}.

Lemma 2.2 shows that curves of the first type lie in a bounded family. Thus, the union of the subvarieties swept out by the non-dominant families satisfying this height bound will be a proper closed subset of 𝒳\mathcal{X}. Corollary 2.9 shows that the surfaces YY defined by the components of the second type will lie in a proper closed subset of 𝒳\mathcal{X}. Proposition 2.10 shows that the surfaces defined by the components of the third type form a bounded family 𝒮N\mathcal{S}\to N. We stratify the parameter space NN using Lemma 5.1. Let NiN_{i} denote a component of this stratification. Combining Corollary 5.2 and Theorem 5.3, we see that for any dC(𝒳)d\geq C(\mathcal{X}) a family of non-dominant sections of height dd which sweeps out a surface parametrized by NiN_{i} will in fact sweep out every surface parametrized by NiN_{i}. Thus if dim(Ni)1\dim(N_{i})\geq 1 then we would have a dominant family, a contradiction. This shows that there are only finitely many surfaces parametrized by our bounded family which can contain sections as in (3), proving our claim. ∎

6. Dominant families which are not relatively free

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. If BB has genus 1\geq 1 then a dominant family of sections need not be relatively free. In fact, such families can have arbitrarily large height and can have larger than the expected dimension.

Example 6.1.

Let BB be a curve of genus 1\geq 1. For dd sufficiently large, there is a unique component MMor(B,1)M\subset\mathrm{Mor}(B,\mathbb{P}^{1}) parametrizing degree dd-maps whose dimension is the expected value 2d+(1g(B))2d+(1-g(B)).

Give 𝒳=1×1×B\mathcal{X}=\mathbb{P}^{1}\times\mathbb{P}^{1}\times B the structure of a del Pezzo fibration using the projection π:𝒳B\pi:\mathcal{X}\to B. Consider the component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) parametrizing sections such that the induced map f:B1×1f:B\to\mathbb{P}^{1}\times\mathbb{P}^{1} is a degree dd cover of a fiber of the first projection. The dimension of MM is 2d+(1g(B))+12d+(1-g(B))+1. This is always greater than the expected dimension 2d+2(1g(B))2d+2(1-g(B)). In this situation we have NC/𝒳=𝒪Cf𝒪(2)N_{C/\mathcal{X}}=\mathcal{O}_{C}\oplus f^{*}\mathcal{O}(2) and the discrepancy between the actual and expected dimension is accounted for by H1(C,NC/𝒳)H^{1}(C,N_{C/\mathcal{X}}).

In this section we will show that the existence and behavior of such families is controlled by the generic Fujita invariant. We have two main goals. First, we show that there is a bounded family of surfaces YY with a(Yη,K𝒳/B)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}) which contains any section of this type of sufficiently large degree (Theorem 6.6). Second, we bound the dimension of such families so that we can control their contributions to the counting function (Lemma 6.5).

We start with a proposition that identifies the geometric properties of these dominant families under the assumption that the general curve does not intersect the singular locus of 𝒳\mathcal{X}.

Proposition 6.2.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Let MM denote a component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing a dominant family of sections such that a general member CC satisfies

K𝒳/BC6g(B)2.\displaystyle-K_{\mathcal{X}/B}\cdot C\geq 6g(B)-2.

If the general section parametrized by MM is not relatively free and is contained in the smooth locus of 𝒳\mathcal{X}, then:

  1. (1)

    The normal bundle of CC is unstable and split.

  2. (2)

    Let qq denote the maximal number of general points of 𝒳\mathcal{X} contained in a curve CC parametrized by MM. Then qg(B)q\leq g(B).

Proof.

Note that this situation can only happen if g(B)>0g(B)>0. Let CC be a general section in our family. We split into two cases.

Case 1: NC/𝒳N_{C/\mathcal{X}} is semistable. Using our height bound, we see the line bundles 1\mathcal{L}_{1}, 2\mathcal{L}_{2} as in Lemma 2.12 have degree 2g(B)1\geq 2g(B)-1. Thus h1(C,NC/𝒳)=0h^{1}(C,N_{C/\mathcal{X}})=0. Since we know that g(B)>0g(B)>0 we also see that NC/𝒳N_{C/\mathcal{X}} is generically globally generated. Thus CC is relatively free, a contradiction.

Case 2: NC/𝒳N_{C/\mathcal{X}} is unstable. Consider the maximal destabilizing exact sequence

02NC/𝒳100\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0

If NC/𝒳N_{C/\mathcal{X}} is indecomposable, then Lemma 2.12 shows that 1\mathcal{L}_{1} and 2\mathcal{L}_{2} have degree 2g(B)\geq 2g(B). In this case CC must be relatively free, a contradiction, finishing the proof of (1).

Since we know that the normal bundle of CC is split and unstable, we can write NC/𝒳=12N_{C/\mathcal{X}}=\mathcal{L}_{1}\oplus\mathcal{L}_{2} with deg(1)<deg(2)\deg(\mathcal{L}_{1})<\deg(\mathcal{L}_{2}). Suppose that deformations of CC go through the maximum number qq of general points of 𝒳\mathcal{X}. If q>g(B)q>g(B), then Proposition 3.6 shows h0(C,1)>g(B)h^{0}(C,\mathcal{L}_{1})>g(B). This implies that deg(1)>2g(B)2\deg(\mathcal{L}_{1})>2g(B)-2, and thus also deg(2)>2g(B)2\deg(\mathcal{L}_{2})>2g(B)-2. We deduce that h1(C,NC/𝒳)=0h^{1}(C,N_{C/\mathcal{X}})=0 and that the family is relatively free, a contradiction. This proves (2). ∎

Next we would like to extend the above proposition to sections which meet the singular locus of 𝒳\mathcal{X}. For this purpose we introduce the following invariant:

Definition 6.3.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Let β:𝒴𝒳\beta:\mathcal{Y}\to\mathcal{X} be a resolution of singularities such that β:YηXη\beta:Y_{\eta}\to X_{\eta} is an isomorphism. We define

m(𝒴/𝒳):=max{K𝒴/𝒳C|CSec(𝒴/B)}.m(\mathcal{Y}/\mathcal{X}):=\max\{K_{\mathcal{Y}/\mathcal{X}}\cdot C\,|\,C\in\mathrm{Sec}(\mathcal{Y}/B)\}.

This is a non-negative integer as K𝒴/𝒳K_{\mathcal{Y}/\mathcal{X}} is a π\pi-vertical effective divisor and any section CC meets with a vertical component with multiplicity at most 11. Then we define

m(𝒳/B):=min{m(𝒴/𝒳)|β:𝒴𝒳 a resolution}.m(\mathcal{X}/B):=\min\{m(\mathcal{Y}/\mathcal{X})|\beta:\mathcal{Y}\to\mathcal{X}\textrm{ a resolution}\}.
Corollary 6.4.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Let MM denote a component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing a dominant family of sections CC such that

K𝒳/BC6g(B)2+m(𝒳/B).\displaystyle-K_{\mathcal{X}/B}\cdot C\geq 6g(B)-2+m(\mathcal{X}/B).

Suppose that the generic section parametrized by MM is not relatively free. If we let qq denote the maximal number of general points of 𝒳\mathcal{X} contained in a curve CC parametrized by MM then qg(B)q\leq g(B).

Proof.

Let β:𝒴𝒳\beta:\mathcal{Y}\to\mathcal{X} be a resolution achieving m(𝒳/B)m(\mathcal{X}/B). Let C~\widetilde{C} be the strict transform of a general CMC\in M. If a general member of MM avoids the singular locus, then our assertion follows from Proposition 6.2. If all members of MM pass through the singular locus of 𝒳\mathcal{X}, then C~\widetilde{C} cannot be relatively free on 𝒴\mathcal{Y}. Indeed if it is relatively free, then the dimension of MM is equal to K𝒴/B+2(1g(B))-K_{\mathcal{Y}/B}+2(1-g(B)). However since 𝒳\mathcal{X} has terminal singularities K𝒴/BC~<K𝒳/BC-K_{\mathcal{Y}/B}\cdot\widetilde{C}<-K_{\mathcal{X}/B}\cdot C which is a contradiction with dimMK𝒳/B+2(1g(B))\dim M\geq-K_{\mathcal{X}/B}+2(1-g(B)).

Now our height bound implies that

K𝒴/BC~6g(B)2.-K_{\mathcal{Y}/B}\cdot\widetilde{C}\geq 6g(B)-2.

Thus our assertion follows from Proposition 6.2. ∎

This yields an estimate on the dimension of the components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing curves of this type.

Lemma 6.5.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. Suppose that MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is a component that parametrizes a dominant family of non-relatively free sections CC with

K𝒳/BC6g(B)2+m(𝒳/B).\displaystyle-K_{\mathcal{X}/B}\cdot C\geq 6g(B)-2+m(\mathcal{X}/B).

Then dim(M)K𝒳/BC+2g(B)+m(𝒳/B)\dim(M)\leq-K_{\mathcal{X}/B}\cdot C+2-g(B)+m(\mathcal{X}/B).

Proof.

Choose a resolution β:𝒴𝒳\beta:\mathcal{Y}\to\mathcal{X} achieving the minimum in the definition of m(𝒳/B)m(\mathcal{X}/B). Let CC^{\prime} be the strict transform of a general member of our family of sections on 𝒴\mathcal{Y}. Arguing as in the proof of Corollary 6.4 we see that the parameter space MM^{\prime} of deformations of CC^{\prime} has the same dimension as MM and that the sections CC^{\prime} have height 6g(B)2\geq 6g(B)-2.

Since 𝒴\mathcal{Y} is smooth we have dim(M)H0(C,NC/𝒴)\dim(M^{\prime})\leq H^{0}(C^{\prime},N_{C^{\prime}/\mathcal{Y}}). By Proposition 6.2 NC/𝒴N_{C^{\prime}/\mathcal{Y}} splits. Proposition 3.3 shows that NC/𝒴N_{C^{\prime}/\mathcal{Y}} is generically globally generated so that both summands must have non-negative degree. Our height bound implies that at least one of the summands will have degree 2g(B)1\geq 2g(B)-1. Thus H1(C,NC/𝒴)g(B)H^{1}(C^{\prime},N_{C^{\prime}/\mathcal{Y}})\leq g(B). By Riemann-Roch we obtain H0(C,NC/𝒴)K𝒴/BC+2g(B)H^{0}(C^{\prime},N_{C^{\prime}/\mathcal{Y}})\leq-K_{\mathcal{Y}/B}\cdot C^{\prime}+2-g(B), which proves the statement. ∎

The next theorem is our main result describing dominant families of sections that fail to be relatively free.

Theorem 6.6.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. Let MM denote a component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing a dominant family of sections such that for a general CMC\in M we have

K𝒳/BCmax{\displaystyle-K_{\mathcal{X}/B}\cdot C\geq\max\{ 6g(B)2+m(𝒳/B),2neg(𝒳,K𝒳/B)+12g(B)2,\displaystyle 6g(B)-2+m(\mathcal{X}/B),-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+12g(B)-2,
8g(B)+2max{4g(B)2,5g(B)1neg(𝒳,K𝒳/B)}},\displaystyle 8g(B)+2\max\{4g(B)-2,5g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}\},

and the general section CC is not relatively free.

Let qq denote the maximal number of general points contained in deformations of CC. Fix qq general points of 𝒳\mathcal{X} and fix a component NN of the sublocus of MM parametrizing sections through these qq points. Then the sections parametrized by NN will sweep out a surface YY that satisfies a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}). These sections will satisfy the height bound of Corollary 5.2 with respect to YY.

Furthermore, there is a component M1M_{1} of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which satisfies the following conditions:

  1. (1)

    The sections C1C_{1} parametrized by M1M_{1} have height

    K𝒳/BC18g(B)1+2max{4g(B)2,5g(B)1neg(𝒳,K𝒳/B)}.-K_{\mathcal{X}/B}\cdot C_{1}\leq 8g(B)-1+2\max\{4g(B)-2,5g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}.
  2. (2)

    The general surface YY constructed above is swept out by sections parametrized by a sublocus of M1M_{1}.

  3. (3)

    There is an integer r1r\geq 1 such that the closure of MM in M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) contains the union of a section parametrized by M1M_{1} with rr general fibers of YBY\to B.

Proof.

First note that we have g(B)1g(B)\geq 1 since any dominant family of rational sections generically parameterizes a free section. By Corollary 6.4 we have 1qg(B)1\leq q\leq g(B).

As in the statement of the theorem, let NN be any component of the sublocus of MM parametrizing curves through a fixed set of qq general points. A dimension count shows that the sections parametrized by NN will sweep out a surface YY. Let ϕ:Y~Y\phi:\widetilde{Y}\to Y be a resolution and let C~\widetilde{C} denote the strict transform of a general deformation of CC in YY. By our height bound on CC, we know there is at least a g(B)g(B) dimensional family of deformations of C~\widetilde{C} contained in Y~\widetilde{Y}. Since this situation can only happen when g(B)1g(B)\geq 1, by Bend-and-Break we deduce that the induced map ψ:Y~B\psi:\widetilde{Y}\to B is generically a 1\mathbb{P}^{1} fibration. We also see that h0(C~,NC~/Y~)>g(B)h^{0}(\widetilde{C},N_{\widetilde{C}/\widetilde{Y}})>g(B). By Kodaira vanishing the dimension of the space of sections of any line bundle of degree 2g12g-1 on C~\widetilde{C} is equal to g(B)g(B). Thus the normal bundle has degree 2g\geq 2g, and in particular, h1(C~,NC~/Y~)=0h^{1}(\widetilde{C},N_{\widetilde{C}/\widetilde{Y}})=0. We conclude that the family of deformations of C~\widetilde{C} in Y~\widetilde{Y} has the expected dimension on Y~\widetilde{Y}. Since the family also has at least the expected dimension on X~\widetilde{X}, we deduce

KY~/BC~+(1g(B))ϕK𝒳/B|YC~+2(1g(B))2q.-K_{\widetilde{Y}/B}\cdot\widetilde{C}+(1-g(B))\geq-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}+2(1-g(B))-2q.

Apply Corollary 4.3 to find a ruled surface 𝔽\mathbb{F} and a birational map ρ:Y~𝔽\rho:\widetilde{Y}\to\mathbb{F} which is an isomorphism on a neighborhood of C~\widetilde{C}. As in Proposition 4.9 (1) we can write C~C~0+kF+T\widetilde{C}\equiv\widetilde{C}_{0}+kF+T where FF is a general fiber of the map to BB and

k=12(KY~/BC~)12neg(𝔽,K𝔽/B).k=\frac{1}{2}(-K_{\widetilde{Y}/B}\cdot\widetilde{C})-\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}).

Then

3g(B)1\displaystyle 3g(B)-1 2q+g(B)1\displaystyle\geq 2q+g(B)-1
KY~/BC~ϕK𝒳/B|YC~\displaystyle\geq K_{\widetilde{Y}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}
=KY~/BC~ϕK𝒳/B|YC~0+k(ϕK𝒳/B|YF)ϕK𝒳/B|YT\displaystyle=K_{\widetilde{Y}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}_{0}+k(-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F)-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot T
KY~/BC~+neg(𝒳,K𝒳/B)+k(ϕK𝒳/B|YF)\displaystyle\geq K_{\widetilde{Y}/B}\cdot\widetilde{C}+\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+k(-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F) (6.1)

where we have used the fact that K𝒳/B-K_{\mathcal{X}/B} is relatively nef at the last step. Suppose for a contradiction that there is an inequality a(Yη,K𝒳/B|Y)<a(Xη,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})<a(X_{\eta},-K_{\mathcal{X}/B}). This is equivalent to saying that ϕK𝒳/B|YF3-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F\geq 3. Rearranging and substituting in our value for kk, we find

12(KY~/BC~)32neg(𝔽,K𝔽/B)neg(𝒳,K𝒳/B)+3g(B)1.\displaystyle\frac{1}{2}(-K_{\widetilde{Y}/B}\cdot\widetilde{C})\leq\frac{3}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+3g(B)-1.

Using the inequality neg(𝔽,K𝔽/B)g(B)\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq g(B) from Corollary 4.3, we see that

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C KY~/BC~+3g(B)1\displaystyle\leq-K_{\widetilde{Y}/B}\cdot\widetilde{C}+3g(B)-1
2neg(𝒳,K𝒳/B)+12g(B)3.\displaystyle\leq-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+12g(B)-3.

contradicting our height bound. Thus we see that a(Yη,K𝒳/B|Y)a(Xη,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})\geq a(X_{\eta},-K_{\mathcal{X}/B}). Since the subvarieties YY with larger generic aa-invariant lie in a closed set but MM defines a dominant family, we see that we must have equality of generic aa-invariants, i.e. ϕK𝒳/B|YF=2-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot F=2. Applying Equation (6.1) we see that

neg(𝔽,K𝔽/B)neg(𝒳,K𝒳/B)+3g(B)1.-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+3g(B)-1. (6.2)

Then

KY~/BC~\displaystyle-K_{\widetilde{Y}/B}\cdot\widetilde{C} ϕK𝒳/B|YC~+13g(B)\displaystyle\geq-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}+1-3g(B)
1+5g(B)+2max{4g(B)2,5g(B)1neg(𝒳,K𝒳/B)}\displaystyle\geq 1+5g(B)+2\max\{4g(B)-2,5g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}
1+4g(B)+neg(𝔽,K𝔽/B)+2max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}\displaystyle\geq 1+4g(B)+\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+2\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\} (6.3)

where we have used the fact that neg(𝔽,K𝔽/B)g(B)\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq g(B) as proved in Corollary 4.3. This verifies that the sections will satisfy the height bound of Corollary 5.2 with respect to YY.

Proposition 4.9 (2) guarantees the existence of a dominant family of sections C~1\widetilde{C}_{1} on YY which satisfy C~C~1+(s2g(B))F\widetilde{C}\equiv\widetilde{C}_{1}+(-s-2g(B))F where

s=12(KY/BC)+12neg(𝔽,K𝔽/B)+max{4g(B)2,2g(B)neg(𝔽,K𝔽/B)}s=\frac{1}{2}(K_{Y/B}\cdot C)+\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+\max\{4g(B)-2,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}

and FF denotes a general fiber of π\pi. Equation (6.3) shows that s2g(B)1-s-2g(B)\geq 1. In particular, by Proposition 4.9 (2) C~\widetilde{C} deforms to the union of C~1\widetilde{C}_{1} with sg(B)-s-g(B) general fibers of YY.

Since C~\widetilde{C} and C~1\widetilde{C}_{1} differ by a multiple of FF, we have

3g(B)1\displaystyle 3g(B)-1 KY~/BC~ϕK𝒳/B|YC~\displaystyle\geq K_{\widetilde{Y}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}
=KY~/BC~1ϕK𝒳/B|YC~1.\displaystyle=K_{\widetilde{Y}/B}\cdot\widetilde{C}_{1}-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}_{1}.

Note that

KY~/BC~1=4g(B)+neg(𝔽,K𝔽/B)+2max{4g(B)3,2g(B)neg(𝔽,K𝔽/B)}.-K_{\widetilde{Y}/B}\cdot\widetilde{C}_{1}=4g(B)+\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})+2\max\{4g(B)-3,2g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}.

Using the bound neg(𝔽,K𝔽/B)neg(𝒳,K𝒳/B)+3g(B)1-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+3g(B)-1 from (6.2), we conclude

ϕK𝒳/B|YC~1\displaystyle-\phi^{*}K_{\mathcal{X}/B}|_{Y}\cdot\widetilde{C}_{1} 3g(B)1+4g(B)+neg(𝔽,K𝔽/B)\displaystyle\leq 3g(B)-1+4g(B)+\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})
+2max{4g(B)2,5g(B)1neg(𝒳,K𝒳/B)}\displaystyle\hskip 21.68121pt+2\max\{4g(B)-2,5g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}
8g(B)1+2max{4g(B)2,5g(B)1neg(𝒳,K𝒳/B)}\displaystyle\leq 8g(B)-1+2\max\{4g(B)-2,5g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}

Now suppose we carry out this construction for every surface YY obtained above. Let C1C_{1} denote the image of C~1\widetilde{C}_{1} in 𝒳\mathcal{X}. Using a Hilbert scheme argument, we see that the corresponding families of sections C1C_{1} constructed for general YY must be members of some fixed component M1Sec(𝒳/B)M_{1}\in\mathrm{Sec}(\mathcal{X}/B). Indeed, as we vary over general sets of qq points in 𝒳\mathcal{X} the surfaces YY constructed above are parametrized by an irreducible variety. For each surface, we have constructed some sections C1C_{1} which have bounded relative anticanonical degree in 𝒳\mathcal{X}. Since there are only finitely many components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing sections of bounded degree, for a general surface YY these sections are all parametrized by the same irreducible component. Thus we have verified that these sections satisfy properties (1), (2), and (3). ∎

Corollary 6.7.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. There is a bounded family 𝒮N\mathcal{S}\to N of surfaces Y𝒳Y\subset\mathcal{X} with a(Yη,K𝒳/B|Y)=a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B}|_{Y})=a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}) such that every component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) parametrizing a dominant family of non-relatively free sections CC with

K𝒳/BCmax{\displaystyle-K_{\mathcal{X}/B}\cdot C\geq\max\{ 6g(B)2+m(𝒳/B),2neg(𝒳,K𝒳/B)+12g(B)2,\displaystyle 6g(B)-2+m(\mathcal{X}/B),-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+12g(B)-2,
2max{4g(B)2,5g(B)1neg(𝒳,K𝒳/B)}+8g(B)+1},\displaystyle 2\max\{4g(B)-2,5g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}+8g(B)+1\},

will generically parametrize sections contained in these surfaces YY.

Proof.

Let qq denote the maximal number of general points contained in deformations of CC. As in Theorem 6.6, the set of sections through qq general points sweeps out a surface YY. The theorem also shows that the general such YY contains a section C1C_{1} with

K𝒳/BC18g(B)1+2max{4g(B)2,5g(B)1neg(𝒳,K𝒳/B)}.-K_{\mathcal{X}/B}\cdot C_{1}\leq 8g(B)-1+2\max\{4g(B)-2,5g(B)-1-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}.

We conclude by Proposition 2.10 that the set of surfaces YY obtained in this way forms a bounded family. ∎

Later on we will need to compare the normal bundles of the sections CC and C1C_{1} in Theorem 6.6. This will be accomplished by the following lemma.

Lemma 6.8.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Let Y𝒳Y\subset\mathcal{X} be a surface such that if ϕ:Y~Y\phi:\widetilde{Y}\to Y denotes the minimal resolution then the general fiber FF of πϕ:Y~B\pi\circ\phi:\widetilde{Y}\to B is isomorphic to 1\mathbb{P}^{1}, satisfies K𝒳/BF=2-K_{\mathcal{X}/B}\cdot F=2, and its image in 𝒳\mathcal{X} has at worst nodal singularities.

Let C1,C2C_{1},C_{2} be sections of πϕ:Y~B\pi\circ\phi:\widetilde{Y}\to B such that

  • both CiC_{i}s are contained in the smooth locus of 𝒳\mathcal{X};

  • the difference C1C2C_{1}-C_{2} is numerically equivalent to a multiple of FF, and;

  • there exists an integer cc such that ϕK𝒳/BCi+KY~/BCic-\phi^{*}K_{\mathcal{X}/B}\cdot C_{i}+K_{\widetilde{Y}/B}\cdot C_{i}\leq c and KY~/BCimax{2g(B),c+2g(B)1}-K_{\widetilde{Y}/B}\cdot C_{i}\geq\max\{2g(B),c+2g(B)-1\}.

Then we have

h1(C1,NC1/𝒳)=h1(C2,NC2/𝒳).h^{1}(C_{1},N_{C_{1}/\mathcal{X}})=h^{1}(C_{2},N_{C_{2}/\mathcal{X}}).
Proof.

For the surfaces Y~\widetilde{Y} as above, define the normal sheaf NY~/𝒳N_{\widetilde{Y}/\mathcal{X}} as the cokernel of the map TY~ϕT𝒳T_{\widetilde{Y}}\to\phi^{*}T_{\mathcal{X}}. We first prove some properties of the normal sheaf. We assume above that a general fiber of the map π|Y:YB\pi|_{Y}:Y\to B is a rational conic in a fiber of π:𝒳B\pi:\mathcal{X}\to B with only nodal singularities. Thus the support of the torsion subsheaf of NY~/𝒳N_{\widetilde{Y}/\mathcal{X}} does not intersect a general fiber of YY. Now consider the exact sequence

TY~ϕT𝒳NY~/𝒳0.T_{\widetilde{Y}}\to\phi^{*}T_{\mathcal{X}}\to N_{\widetilde{Y}/\mathcal{X}}\to 0.

If we restrict this sequence to CiC_{i} and remove the direct summands coming from TCiT_{C_{i}}, we obtain an exact sequence

NCi/Y~NCi/𝒳NY~/𝒳|Ci0N_{C_{i}/\widetilde{Y}}\to N_{C_{i}/\mathcal{X}}\to N_{\widetilde{Y}/\mathcal{X}}|_{C_{i}}\to 0

which must be exact on the left due to the fact that NCi/Y~N_{C_{i}/\widetilde{Y}} is an invertible sheaf. Since CiC_{i} is a general section in a family of sections on Y~\widetilde{Y} which satisfy KY~/BCi2g(B)-K_{\widetilde{Y}/B}\cdot C_{i}\geq 2g(B), by Lemma 3.9 we may ensure that CiC_{i} avoids any codimension 22 locus in Y~\widetilde{Y}.

In particular, let (NY~/𝒳)tf(N_{\widetilde{Y}/\mathcal{X}})_{tf} denote the torsion-free quotient of NY~/𝒳N_{\widetilde{Y}/\mathcal{X}}. Note that (NY~/𝒳)tf(N_{\widetilde{Y}/\mathcal{X}})_{tf} is locally free away from a codimension 22 subset, since it is locally free at every codimension 11 point of Y~\widetilde{Y}. Thus we may ensure that CiC_{i} is contained in the locus where (NY~/𝒳)tf(N_{\widetilde{Y}/\mathcal{X}})_{tf} is locally free. Altogether this implies that

(NY~/𝒳|Ci)tor\displaystyle(N_{\widetilde{Y}/\mathcal{X}}|_{C_{i}})_{tor} =(NY~/𝒳)tor|Ci\displaystyle=(N_{\widetilde{Y}/\mathcal{X}})_{tor}|_{C_{i}}
=𝒪Z|Ci\displaystyle=\mathcal{O}_{Z}|_{C_{i}}

where ZZ is the divisor whose components are the codimension 11 components of the support of (NY~/𝒳)tor(N_{\widetilde{Y}/\mathcal{X}})_{tor} and the multiplicities are the lengths of the torsion subsheaf along the generic point of each component.

We claim that the restriction of NY~/𝒳N_{\widetilde{Y}/\mathcal{X}} to C1C_{1} and to C2C_{2} are isomorphic sheaves. We first prove that the restrictions of (NY~/𝒳)tor(N_{\widetilde{Y}/\mathcal{X}})_{tor} agree. Since a general fiber of Y~B\widetilde{Y}\to B will not intersect the torsion subsheaf of NY~/𝒳N_{\widetilde{Y}/\mathcal{X}} but C1C_{1} and C2C_{2} differ by a sum of general fibers, we see that the torsion subsheaves of NY~/𝒳|C1N_{\widetilde{Y}/\mathcal{X}}|_{C_{1}} and NY~/𝒳|C2N_{\widetilde{Y}/\mathcal{X}}|_{C_{2}} are isomorphic and in particular have the same length.

Next consider the restriction of (NY~/𝒳)tf(N_{\widetilde{Y}/\mathcal{X}})_{tf}. Since a general fiber FF of Y~B\widetilde{Y}\to B is 1\mathbb{P}^{1} and the degree of the restriction of (NY~/𝒳)tf(N_{\widetilde{Y}/\mathcal{X}})_{tf} to FF is zero, in the open locus of Y~\widetilde{Y} where the torsion free part is locally free the invertible sheaf (NY~/𝒳)tf(N_{\widetilde{Y}/\mathcal{X}})_{tf} is linearly equivalent to a sum of vertical curves. Since C1C_{1} and C2C_{2} have the same intersection profile, we conclude that the restrictions of the torsion free part to CiC_{i} are isomorphic.

Note that

deg(NY~/𝒳|Ci)=ϕK𝒳/BCi+KY~/BCic.\deg(N_{\widetilde{Y}/\mathcal{X}}|_{C_{i}})=-\phi^{*}K_{\mathcal{X}/B}\cdot C_{i}+K_{\widetilde{Y}/B}\cdot C_{i}\leq c.

On the other hand, we have

KY~/BCi\displaystyle-K_{\widetilde{Y}/B}\cdot C_{i} c+2g(B)1\displaystyle\geq c+2g(B)-1
deg(NY~/𝒳|Ci)+2g(B)1\displaystyle\geq\deg(N_{\widetilde{Y}/\mathcal{X}}|_{C_{i}})+2g(B)-1

Let 𝒦\mathcal{K} be the kernel fitting in the exact sequence

0𝒦NCi/𝒳(NY~/𝒳|Ci)tf0.0\to\mathcal{K}\to N_{C_{i}/\mathcal{X}}\to(N_{\widetilde{Y}/\mathcal{X}}|_{C_{i}})_{tf}\to 0.

The argument above shows that the degree of 𝒦\mathcal{K} is at least 2g(B)12g(B)-1 more than the degree of the rightmost term. Thus Ext1((NY~/𝒳|Ci)tf,𝒦)=0\mathrm{Ext}^{1}((N_{\widetilde{Y}/\mathcal{X}}|_{C_{i}})_{tf},\mathcal{K})=0 and we conclude that the exact sequence splits. By degree considerations h1(Ci,𝒦)=0h^{1}(C_{i},\mathcal{K})=0 and so (NY~/𝒳|C~i)tf(N_{\widetilde{Y}/\mathcal{X}}|_{\widetilde{C}_{i}})_{tf} contributes all of H1(Ci,NCi/𝒳)H^{1}(C_{i},N_{C_{i}/\mathcal{X}}). As explained above this implies that the dimension of this vector space is the same for both curves. ∎

7. Stable maps through general points

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Suppose that f:C𝒳f:C\to\mathcal{X} is a genus g(B)g(B) stable map obtained by deforming a section of π\pi. The goal of this section is to relate the number of general points of 𝒳\mathcal{X} contained in f(C)f(C) with its anticanonical degree. When CC is irreducible this is straightforward, but the situation is more subtle when CC is reducible.

In particular, we will show that when f(C)f(C) contains (almost) as many points as possible given its degree then CC will have a particularly simple form. In the next section, we use this fact to deduce that a section with semistable normal bundle will break in a particularly simple way, implying a special case of Movable Bend-and-Break.

We first discuss irreducible curves:

Lemma 7.1.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Fix n2g(B)+1n\geq 2g(B)+1. Let MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) denote a component such that for any nn general points of 𝒳\mathcal{X} there exists a member of MM containing those points. Then MM has the expected dimension and the curves CC parametrized by MM have height 2n+2g(B)2\geq 2n+2g(B)-2.

Proof.

Corollary 3.7 shows that a general CC is relatively free so that MM has the expected dimension. Since the points are general they will impose independent conditions on MM, so that dim(M)2n\dim(M)\geq 2n. Thus

2nK𝒳/BC+2(1g(B))2n\leq-K_{\mathcal{X}/B}\cdot C+2(1-g(B))

which rearranges to give the desired height bound. ∎

We will use the following definition to control the failure of families of sections to have the expected dimension.

Definition 7.2.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. Fix an integer dd. We let maxdef(d)\mathrm{maxdef}(d) denote the maximum dimension of any component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) parametrizing sections of height dd. When there is no section of height dd, we simply set maxdef(d)=\mathrm{maxdef}(d)=-\infty. We also define

maxdef(q)=max{0,maxdqmaxdef(d)}.\mathrm{maxdef}(\leq q)=\max\left\{0,\max_{d\leq q}\mathrm{maxdef}(d)\right\}.
Lemma 7.3.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Fix an integer dd. Choose a positive integer nn satisfying nmaxdef(d)n\geq\mathrm{maxdef}(d). Suppose that we have a connected effective curve C=C0+aiTiC=C_{0}+\sum a_{i}T_{i} where C0C_{0} is a section of height dd and each TiT_{i} is a π\pi-vertical rational curve. If CC contains nn general points of 𝒳\mathcal{X} then K𝒳/BCd+3n32maxdef(d)-K_{\mathcal{X}/B}\cdot C\geq d+3n-\frac{3}{2}\mathrm{maxdef}(d).

Proof.

Let MM be the component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) containing C0C_{0}. We split into several cases depending upon the dimension of the locus swept out by the sections in MM.

First suppose that C0C_{0} is a rigid section. In this case each general point contained in CC is contained in a π\pi-vertical component. There are only finitely many π\pi-vertical conics through a general point of 𝒳\mathcal{X}. By generality, none of these conics will intersect C0C_{0}. Thus any π\pi-vertical curve through a general point of 𝒳\mathcal{X} that intersects C0C_{0} must have anticanonical degree 3\geq 3. Thus K𝒳/BCd+3n-K_{\mathcal{X}/B}\cdot C\geq d+3n.

Next suppose that deformations of C0C_{0} sweep out a surface YY. Fix a general point pp of 𝒳\mathcal{X} and consider the finite set of π\pi-vertical conics through this point. Each such conic will intersect YY in a finite set of points. If a π\pi-vertical conic through pp is a component of CC, then C0C_{0} must contain one of these intersection points with YY to ensure that CC is connected. Furthermore, the conditions imposed on C0C_{0} by insisting that it contain the attachment points for conics through pp will be independent for different general points pp. Thus CC can have at most maxdef(d)\mathrm{maxdef}(d) components which are π\pi-vertical conics through general points. This proves that

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C d+2maxdef(d)+3(nmaxdef(d))\displaystyle\geq d+2\mathrm{maxdef}(d)+3(n-\mathrm{maxdef}(d))
=d+3nmaxdef(d).\displaystyle=d+3n-\mathrm{maxdef}(d).

Finally suppose that deformations of C0C_{0} form a dominant family. Suppose that qq of the general points are contained in C0C_{0}; this imposes 2q2q independent conditions on MM. In particular 2qmaxdef(d)2q\leq\mathrm{maxdef}(d). Meeting a π\pi-vertical conic through a fixed general point imposes one additional condition on C0C_{0}. Thus CC can have at most maxdef(d)2q\mathrm{maxdef}(d)-2q components which are π\pi-vertical conics through general points. This proves that

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C d+2(maxdef(d)2q)+3(nq(maxdef(d)2q))\displaystyle\geq d+2(\mathrm{maxdef}(d)-2q)+3(n-q-(\mathrm{maxdef}(d)-2q))
d+3nmaxdef(d)q\displaystyle\geq d+3n-\mathrm{maxdef}(d)-q
d+3n32maxdef(d).\displaystyle\geq d+3n-\frac{3}{2}\mathrm{maxdef}(d).

The two following propositions describe which stable maps can pass through the maximal number of general points of 𝒳\mathcal{X}. The first handles the case of even height.

Proposition 7.4.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Fix a positive integer

n32maxdef(6g(B))+2g(B)+2+max{0,neg(𝒳,K𝒳/B)}.n\geq\frac{3}{2}\mathrm{maxdef}(\leq 6g(B))+2g(B)+2+\max\{0,-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}.

Suppose that f:C𝒳f:C\to\mathcal{X} is a genus g(B)g(B) stable map with anticanonical height 2n+2g(B)22n+2g(B)-2 such that the unique component of CC whose image is not π\pi-vertical maps birationally to a section. Then:

  1. (1)

    Suppose the image of CC contains nn general points of 𝒳\mathcal{X}. Then ff is a birational map to a relatively free section.

  2. (2)

    Fix a general curve ZZ in a basepoint free linear series in a general fiber of π\pi. Suppose the image of CC contains n1n-1 general points of 𝒳\mathcal{X} and intersects ZZ. Suppose also that the image of CC is reducible and at least one of our general points is contained in a π\pi-vertical component of CC. Then CC has exactly two components and ff maps one component birationally onto a relatively free section and the other birationally onto either a conic or a cubic in a general fiber of π\pi. Moreover the intersection of the section and the π\pi-vertical curve is a smooth point of the π\pi-vertical curve.

Construction 7.5.

Before giving the proof, we clarify what “general” means in the statement of the proposition. We let ZZ be a fixed general member of a basepoint free linear system in a general fiber of π\pi. We may then ensure that the nn points satisfy the following conditions:

  1. (1)

    Suppose we fix any subset of our set of points of size dd. Then we may ensure that these points impose independent conditions on every family of height 2n+2g(B)2\leq 2n+2g(B)-2. In particular, when d2g(B)+1d\geq 2g(B)+1 then Corollary 3.7 (3) shows that a general deformation of a section through all dd points will be relatively free. Thus when choosing dd general points we may ensure that there are only finitely many sections of height 2d+2g(B)22d+2g(B)-2 which contain this subset of points and that every section of this height containing the points will be relatively free. Also we may ensure there are finitely many loci of dimension 1\leq 1 in Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) that parametrize sections of height 2d+2g(B)12d+2g(B)-1 which contain this set of points and that the general section in these families is relatively free.

  2. (2)

    We may ensure that every fiber of π\pi that contains one of the general points or ZZ is a smooth del Pezzo surface. Moreover we may assume that each general point and ZZ are contained in different fibers of π\pi. Furthermore, we may ensure that a general point is not contained in any (1)(-1)-curve in its fiber FF and that the finite set of conics in FF through the point have the expected dimension of intersection against the sections described in (1); namely, for any 0-dimensional component of the parameter space the corresponding section is disjoint from each conic, and for any 11-dimensional component of the parameter space there are only finitely many sections intersecting each conic. We may also ensure that these finitely many sections are relatively free when they contain more than 2g(B)2g(B) general points.

  3. (3)

    By choosing ZZ general we may ensure that the sections in (1) and (2) meet ZZ in the expected dimension: for any 0-dimensional component of the parameter space the corresponding section is disjoint from ZZ, and for any 11-dimensional component of the parameter space there are only finitely many sections intersecting ZZ. We may further ensure that these finitely many sections are relatively free when they contain more than 2g(B)2g(B) general points.

  4. (4)

    Consider a subset of dd of our general points where d12g(B)+1d-1\geq 2g(B)+1. Fix one of these general points pp and let TT be any π\pi-vertical anticanonical conic which contains pp. By choosing the points general we may ensure that there are only finitely many sections of height 2d+2g(B)22n+2g(B)22d+2g(B)-2\leq 2n+2g(B)-2 passing through the remaining d1d-1 general points and meeting with ZZ and TT. Indeed, by Corollary 3.7 (3) it suffices to consider families which generically parametrize relatively free sections. Lemma 3.10 shows that a general member of such a family will not intersect ZZ. Due to the generality of the point pp we may ensure that no π\pi-vertical conic through pp meets every section that intersects ZZ. Finally, since general points impose codimension 22 conditions on the remaining subfamily we obtain the desired claim. Furthermore, we may ensure that the finitely many sections satisfying these incidence conditions are relatively free.

  5. (5)

    Note that if we take a general point in a del Pezzo surface SS there are only finitely many rational anticanonical cubics containing this point and any other general point in SS. We ensure that all of our nn points satisfy this condition in their fiber.

    In (1), (2), (3), and (4) we have constructed certain incidence conditions such that the families of sections satisfying these conditions are parametrized by a 0-dimensional space. For each choice of conditions, consider the set of π\pi-vertical rational anticanonical cubics passing through one of our nn general points. These anticanonical cubics are parameterized by a 11-dimensional family, and they sweep out the fiber FF of π\pi containing the point. By choosing our remaining points general, we may ensure that sections satisfying the above incidence conditions go through a general point of FF. Using an incidence correspondence, we see that for general choices of nn points there will only be finitely many anticanonical cubics through one of our general points which meet these sections.

  6. (6)

    We may ensure that there is no section as in (2) or (4) that intersects two different conics through two different points in our set. Indeed, since each such conic imposes independent conditions on the parameter space of sections, the set of sections through two general conics cannot meet the 11-dimensional locus parametrizing sections through the other general points and ZZ. By a similar argument we may ensure that any section as in (1)-(4) that is parametrized by a 0-dimensional set does not meet with any line intersecting ZZ.

  7. (7)

    Since nmaxdef(6g(B))n\geq\mathrm{maxdef}(\leq 6g(B)), we may ensure that for any d<6g(B)+1d<6g(B)+1 and any subset of our set of points of size maxdef(d)\geq\mathrm{maxdef}(d) the points are general in the sense of Lemma 7.3.

Proof of Proposition 7.4:.

Note that our hypotheses imply that the π\pi-vertical connected components of C\C0C\backslash C_{0} are trees of rational curves.

(1). It suffices to show that the image of ff is irreducible. Suppose otherwise, so that f(C)=C0+iIaiTif(C)=C_{0}+\sum_{i\in I}a_{i}T_{i} for some π\pi-vertical curves TiT_{i}. Let dd denote the height of C0C_{0} and set ti=K𝒳/BTit_{i}=-K_{\mathcal{X}/B}\cdot T_{i}, so that

2n+2g(B)2=d+iIaiti.2n+2g(B)-2=d+\sum_{i\in I}a_{i}t_{i}.

Note that C0C_{0} can contain at most max{0,d2+1g(B)}\max\{0,\lfloor\frac{d}{2}\rfloor+1-g(B)\} general points of 𝒳\mathcal{X} if it is relatively free. By Corollary 3.7 C0C_{0} can contain at most 2g(B)2g(B) general points of 𝒳\mathcal{X} if it is not relatively free. An irreducible vertical curve TiT_{i} can contain at most 11 general point and if it does then ti2t_{i}\geq 2. Let III^{\prime}\subset I denote the set of vertical curves that contain one of the general points.

We now break the argument into several cases.

Case 1: d6g(B)d\geq 6g(B). Then the number of general points contained in f(C)f(C) is bounded above by the number of general points contained in C0C_{0} and in the TiT_{i}. Thus:

max{0,d2+1g(B),2g(B)}+|I|\displaystyle\max\left\{0,\left\lfloor\frac{d}{2}\right\rfloor+1-g(B),2g(B)\right\}+|I^{\prime}| n\displaystyle\geq n
=d2+1g(B)+iIaiti/2.\displaystyle=\frac{d}{2}+1-g(B)+\sum_{i\in I}a_{i}t_{i}/2.

Since d6g(B)d\geq 6g(B) the RHS is an upper bound for the LHS. Thus the inequality above must be an equality. This means that dd is even, that C0C_{0} goes through d2+1g(B)\left\lfloor\frac{d}{2}\right\rfloor+1-g(B) general points, that C0C_{0} is relatively free (since it contains at least 2g(B)+12g(B)+1 general points), that each ai=1a_{i}=1, and that each component of TT is a free vertical curve through one of the general points with ti=2t_{i}=2. In particular, the set of d2+1g(B)\frac{d}{2}+1-g(B) general points determines a finite number of possibilities for C0C_{0}, and each vertical curve is also determined by a general point up to a finite set of possibilities. If there are any vertical components, then for general choices f(C)f(C) will not be connected, an impossibility. Thus f(C)f(C) is irreducible.

Case 2: d<6g(B)d<6g(B). Due to our lower bound on nn we may apply Lemma 7.3. It shows that CC must have height

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C neg(𝒳,K𝒳/B)+3n32maxdef(6g(B)1)\displaystyle\geq\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+3n-\frac{3}{2}\mathrm{maxdef}(\leq 6g(B)-1)

Applying our assumption on the lower bound for nn, we see that

K𝒳/BC>2n+2g(B)2\displaystyle-K_{\mathcal{X}/B}\cdot C>2n+2g(B)-2

contradicting our assumption that CC have height 2n+2g(B)22n+2g(B)-2.


(2). Write f(C)=C0+iIaiTif(C)=C_{0}+\sum_{i\in I}a_{i}T_{i} for some π\pi-vertical curves TiT_{i}. Let dd denote the height of C0C_{0} and set ti=K𝒳/BTit_{i}=-K_{\mathcal{X}/B}\cdot T_{i}, so that

2n+2g(B)2=d+iIaiti.2n+2g(B)-2=d+\sum_{i\in I}a_{i}t_{i}.

Let III^{\prime}\subset I denote the set of vertical curves that contain one of the general points. Again we separate into cases:

Case 1: d6g(B)+1d\geq 6g(B)+1 and C0C_{0} intersects ZZ. Meeting ZZ will impose one condition on a relatively free section. Since C0C_{0} intersects ZZ it can contain at most max{0,d+12g(B),2g(B)}\max\{0,\lfloor\frac{d+1}{2}\rfloor-g(B),2g(B)\} general points of 𝒳\mathcal{X}. The number of general points contained in f(C)f(C) is bounded above by the number of general points contained in C0C_{0} and in the TiT_{i}. Thus:

max{0,d+12g(B),2g(B)1}+|I|\displaystyle\max\left\{0,\left\lfloor\frac{d+1}{2}\right\rfloor-g(B),2g(B)-1\right\}+|I^{\prime}| n1\displaystyle\geq n-1
d2g(B)+iIaiti/2.\displaystyle\geq\frac{d}{2}-g(B)+\sum_{i\in I}a_{i}t_{i}/2.

If dd is even, then we must have equality everywhere. This means that C0C_{0} contains the maximal number of general points, the set of deformations of C0C_{0} which meet ZZ and go through the maximal number of points is at most 11-dimensional, that every ai=1a_{i}=1, and that each component of TT is a free vertical curve through one of the general points with ti=2t_{i}=2. However, for C0C_{0} to meet a vertical conic through a general point is a codimension 11 condition, so by generality there can be at most one vertical component and we obtain the desired expression. Moreover the intersection of the section and the vertical curve must be a smooth point of the vertical curve due to generality. Since C0C_{0} contains at least 2g(B)+12g(B)+1 general points, it must be relatively free by generality.

If dd is odd, then the equation simplifies to 1/2+|I|iIaiti/21/2+|I^{\prime}|\geq\sum_{i\in I}a_{i}t_{i}/2. There are only three options for the vertical components:

  1. (1)

    every component of TT has anticanonical degree 22 and contains a general point, or

  2. (2)

    every component of TT but one has anticanonical degree 22 and contains a general point, and the last one has anticanonical degree 33 and contains a general point, or,

  3. (3)

    every component of TT but one has anticanonical degree 22 and contains a general point, and the last component has anticanonical degree 11.

Note that there are only finitely many deformations of C0C_{0} which meet ZZ and go through d+12g(B)\frac{d+1}{2}-g(B) points. Thus such C0C_{0} is relatively free by generality as it contains at least 2g(B)+12g(B)+1 general points. Recall that by assumption there is a vertical component of f(C)f(C) through a general point. However, since there are only finitely many vertical conics through a general point, by generality no such conic can intersect C0C_{0}. This rules out the first and third situations, showing that CC must be the union of a free section and a cubic in a fiber. Moreover there are only finitely many cubics containing a general point and meeting with C0C_{0} thus by generality the intersection of the section and the cubic is a smooth point of the cubic.

Case 2: d6g(B)+1d\geq 6g(B)+1 and C0C_{0} does not intersect ZZ. Just as before, the number of general points contained in f(C)f(C) is bounded above by the number of general points contained in C0C_{0} and in the TiT_{i}. Thus:

max{0,d2+1g(B),2g(B)1}+|I|\displaystyle\max\left\{0,\left\lfloor\frac{d}{2}\right\rfloor+1-g(B),2g(B)-1\right\}+|I^{\prime}| n1\displaystyle\geq n-1
d2g(B)+iIaiti/2.\displaystyle\geq\frac{d}{2}-g(B)+\sum_{i\in I}a_{i}t_{i}/2.

Since C0C_{0} does not intersect ZZ, there must be a vertical curve that does intersect ZZ but does not contain any general points, so that

iIaiti/2|I|iIaiti/2iIaiti/21/2.\sum_{i\in I}a_{i}t_{i}/2-|I^{\prime}|\geq\sum_{i\in I}a_{i}t_{i}/2-\sum_{i\in I^{\prime}}a_{i}t_{i}/2\geq 1/2.

Thus when dd is even, C0C_{0} must contain the maximal number of points d2+1g(B)\frac{d}{2}+1-g(B) and must be relatively free by generality. In this situation the difference between |I||I^{\prime}| and iIaiti/2\sum_{i\in I^{\prime}}a_{i}t_{i}/2 is at most 1/21/2. There are four options for the vertical components:

  1. (1)

    every component of TT but one has anticanonical degree 22 and contains a general point, and the last has anticanonical degree 11 and meets ZZ.

  2. (2)

    every component of TT but two has anticanonical degree 22 and contains a general point, one has anticanonical degree 11 and meets ZZ, and the last one has anticanonical degree 33 and contains a general point,

  3. (3)

    every component of TT but two has anticanonical degree 22 and contains a general point, and the last two components have anticanonical degree 11, one of which meets ZZ,

  4. (4)

    every component of TT has anticanonical degree 22, all but one contain a general point, and the last component meets ZZ.

Since by generality there are only finitely many deformations of C0C_{0} through the required number of points, such C0C_{0} can not intersect a vertical line meeting ZZ or a vertical conic through a general point. This rules out the first three cases immediately, and the fourth is also ruled out since by assumption there exists at least one vertical curve which contains some general point.

When dd is odd then C0C_{0} must contain the maximal number of points d2+1g(B)\lfloor\frac{d}{2}\rfloor+1-g(B). In this case there is only one option: every component of TT but one has anticanonical degree 22 and contains a general point, and the last has anticanonical degree 11 and meets ZZ. However, since by generality C0C_{0} can only deform in a one-parameter family while containing the maximal number of points, it is impossible for C0C_{0} to meet both a line intersecting ZZ and a conic through a general point. Since by assumption f(C)f(C) contains a vertical component through a general point, this case is also ruled out.

Case 3: d<6g(B)+1d<6g(B)+1. In this case Lemma 7.3 shows that CC must have height

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C neg(𝒳,K𝒳/B)+3(n1)32maxdef(6g(B))\displaystyle\geq\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+3(n-1)-\frac{3}{2}\mathrm{maxdef}(\leq 6g(B))
>2n+2g(B)2\displaystyle>2n+2g(B)-2

proving the impossibility of this case. ∎

The next proposition is the analogue of Proposition 7.4 for sections of odd height.

Proposition 7.6.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Fix a positive integer

n32maxdef(6g(B))+2g(B)+max{0,neg(𝒳,K𝒳/B)}.n\geq\frac{3}{2}\mathrm{maxdef}(\leq 6g(B))+2g(B)+\max\{0,-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}.

Suppose that f:C𝒳f:C\to\mathcal{X} is a genus g(B)g(B) stable map with anticanonical height 2n+2g(B)12n+2g(B)-1 such that the unique component of CC whose image is not π\pi-vertical maps birationally to a section. Then:

  1. (1)

    Fix a general curve ZZ in a basepoint free linear series in a general fiber of π\pi. Suppose the image of CC contains nn general points of 𝒳\mathcal{X} and intersects ZZ. Then ff is a birational map to a relatively free section.

  2. (2)

    Suppose the image of CC contains nn general points of 𝒳\mathcal{X}. Suppose also that the image of CC is reducible and at least one general point is contained in a π\pi-vertical component of CC. Then CC has exactly two components and ff maps one component birationally onto a relatively free section and the other birationally onto a conic or a cubic in a general fiber of π\pi. Moreover the intersection of the section and the π\pi-vertical curve is a smooth point of the π\pi-vertical curve.

The proof is essentially the same as the proof of Proposition 7.4, but slightly easier.

8. Movable Bend-and-Break for del Pezzo fibrations

We next establish Movable Bend-and-Break for sections of del Pezzo fibrations such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample.

Theorem 8.1.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Define

Q(𝒳)=max{\displaystyle Q(\mathcal{X})=\max\{ 10g(B)+3,3maxdef(6g(B))+6g(B)+3+2max{0,neg(𝒳,K𝒳/B)},\displaystyle 10g(B)+3,3\mathrm{maxdef}(\leq 6g(B))+6g(B)+3+2\max\{0,-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\},
2neg(𝒳,K𝒳/B)+12g(B)+5,2neg(𝒳,K𝒳/B)+21g(B)3,\displaystyle-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+12g(B)+5,-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+21g(B)-3,
3maxdef(8g(B)neg(𝒳,K𝒳/B))neg(𝒳,K𝒳/B)+6g(B)+1}.\displaystyle 3\mathrm{maxdef}(\leq 8g(B)-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B}))-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+6g(B)+1\}.

Suppose that MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is a component that parametrizes a family of relatively free sections CC satisfying K𝒳/BCQ(𝒳)-K_{\mathcal{X}/B}\cdot C\geq Q(\mathcal{X}). Then the closure of MM in M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) contains a point representing a stable map whose domain has exactly two components, one which maps birationally onto a relatively free section and one which maps birationally onto a free π\pi-vertical curve. Moreover the section and the vertical curve meet at a smooth point of the vertical curve.

It is helpful to introduce the following definition:

Definition 8.2.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. We define MBBbound(𝒳)\mathrm{MBBbound}(\mathcal{X}) to be the smallest non-negative integer rr such that any component of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) which generically parametrizes relatively free sections of height at least rr will also parametrize a stable map whose domain has exactly two components, one which maps birationally onto a relatively free section and one which maps birationally onto a free π\pi-vertical curve, and such that the section intersects a smooth point of the vertical curve.

Thus Theorem 8.1 establishes that MBBbound(𝒳)\mathrm{MBBbound}(\mathcal{X}) exists and gives an explicit upper bound MBBbound(𝒳)Q(𝒳)\mathrm{MBBbound}(\mathcal{X})\leq Q(\mathcal{X}).

We will prove Theorem 8.1 by splitting into several cases. The first situation (Cases (1) and (2)) is when NC/𝒳N_{C/\mathcal{X}} is “almost” semistable. In this case we can appeal to Proposition 7.4 and Proposition 7.6 to obtain a suitable breaking of CC. The second situation (Cases (3) and (4)) is when NC/𝒳N_{C/\mathcal{X}} is unstable. By taking all deformations of CC through a suitable number of general points we obtain a surface Σ\Sigma as in Section 3.4. Since CC deforms a lot in Σ\Sigma, we can break CC inside Σ\Sigma and then show that this breaking satisfies the desired properties. Note that in this case the argument depends upon whether the degree of the destabilizing quotient of NC/𝒳N_{C/\mathcal{X}} is large or small.

Proof of Theorem 8.1:.

Suppose that MM is a component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing a relatively free family of sections that satisfy

K𝒳/BCQ(𝒳).\displaystyle-K_{\mathcal{X}/B}\cdot C\geq Q(\mathcal{X}).

Since each section is smooth we can consider its normal bundle, and we separate into several cases based on the normal bundle of the general curve CC parametrized by MM.

Case 1: NC/𝒳N_{C/\mathcal{X}} is semistable. First assume that the height of CC is even. Choose nn so that K𝒳/BC=2n+2g(B)2-K_{\mathcal{X}/B}\cdot C=2n+2g(B)-2. Our height bound implies that

n32maxdef(6g(B))+2g(B)+52+max{0,neg(𝒳,K𝒳/B)}52,n\geq\frac{3}{2}\mathrm{maxdef}(\leq 6g(B))+2g(B)+\frac{5}{2}+\max\{0,-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}\geq\frac{5}{2},

which implies that n3n\geq 3. Since CC is relatively free Riemann-Roch implies that

h0(C,NC/𝒳)=2n.h^{0}(C,N_{C/\mathcal{X}})=2n.

Fix n1n-1 general points and a basepoint free curve ZZ in a general fiber of π\pi. Proposition 3.6 shows there is a one parameter family of deformations of CC passing through n1n-1 general points and meeting with ZZ. By Bend-and-Break as in Lemma 2.11 CC degenerates to a stable map whose image is the union of a section with π\pi-vertical rational curves where at least one π\pi-vertical component contains a general point. Now our assertion follows from Proposition 7.4.

When the height is odd, choose nn so that K𝒳/BC=2n+2g(B)1-K_{\mathcal{X}/B}\cdot C=2n+2g(B)-1. Our height bound implies that

n32maxdef(6g(B))+2g(B)+2+max{0,neg(𝒳,K𝒳/B)}2.n\geq\frac{3}{2}\mathrm{maxdef}(\leq 6g(B))+2g(B)+2+\max\{0,-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})\}\geq 2.

Since CC is relatively free Riemann-Roch implies that

h0(C,NC/𝒳)=2n+1.h^{0}(C,N_{C/\mathcal{X}})=2n+1.

Fix nn general points.. Proposition 3.6 shows there is a one parameter family of deformations of CC passing through nn general points. By Bend-and-Break as in Lemma 2.11 CC degenerates to a stable map whose image is the union of a section with π\pi-vertical rational curves where at least one π\pi-vertical component contains a general point. Now our assertion follows from Proposition 7.6.

Case 2: NC/𝒳N_{C/\mathcal{X}} is unstable with the maximal destabilizing exact sequence

02NC/𝒳100\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0

such that deg(2)deg(1)1\deg(\mathcal{L}_{2})-\deg(\mathcal{L}_{1})\leq 1. Due to the relative freeness of the curve and the bound on the degrees of the components we have

h0(C,1)=h0(C,NC/𝒳)2.h^{0}(C,\mathcal{L}_{1})=\left\lfloor\frac{h^{0}(C,N_{C/\mathcal{X}})}{2}\right\rfloor.

Thus the same proof for Case 1 works without any modification.

Case 3: NC/𝒳N_{C/\mathcal{X}} is unstable with the maximal destabilizing exact sequence

02NC/𝒳100\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0

such that 3g(B)deg(1)deg(2)23g(B)\leq\deg(\mathcal{L}_{1})\leq\deg(\mathcal{L}_{2})-2.

We write a=H0(C,1)=deg(1)+1g(B)a=H^{0}(C,\mathcal{L}_{1})=\deg(\mathcal{L}_{1})+1-g(B) and b=H0(C,2)=deg(2)+1g(B)b=H^{0}(C,\mathcal{L}_{2})=\deg(\mathcal{L}_{2})+1-g(B). Our assumption implies that a2g(B)+1a\geq 2g(B)+1.

By Proposition 3.6 deformations of CC can contain aa general points of 𝒳\mathcal{X}. Consider a component Σ\Sigma of the locus swept out by the curves CC parametrized by MM through aa general points {x1,,xa}\{x_{1},\ldots,x_{a}\}; we may assume that the general curve sweeping out Σ\Sigma has generic normal bundle and {x1,,xa}\{x_{1},\ldots,x_{a}\} are general on CC. We know that Σ𝒳\Sigma\subsetneq\mathcal{X} and a dimension count shows that it is a surface. In fact, since each general point imposes 22 independent conditions on the moduli space, there is a (ba)(b-a)-dimensional family of curves through these general points which sweep out Σ\Sigma.

Let ν:ΣΣ\nu:\Sigma^{\prime}\to\Sigma be the normalization and let ϕ:Σ~Σ\phi:\widetilde{\Sigma}\to\Sigma be the minimal resolution. The results in Section 3.4 show that Σ~Σ\widetilde{\Sigma}\to\Sigma is finite on an open neighborhood of a general section CC sweeping out Σ\Sigma and the strict transforms C~\widetilde{C} will define a dominant family of sections of Σ~\widetilde{\Sigma} which have normal bundle 2\mathcal{L}_{2}. In particular the induced map ψ:Σ~B\psi:\widetilde{\Sigma}\to B has connected fibers. Since deg(2)g(B)+2\deg(\mathcal{L}_{2})\geq g(B)+2 the usual Bend-and-Break theorem shows that the general fiber of ψ\psi is 1\mathbb{P}^{1}.

By Corollary 4.3 we find a ruled surface 𝔽\mathbb{F} and a birational map ρ:Σ~𝔽\rho:\widetilde{\Sigma}\to\mathbb{F} which is an isomorphism on a neighborhood of C~\widetilde{C}. Let C0C_{0} be a section of 𝔽B\mathbb{F}\to B of minimal height and write ρC~C0+kF\rho_{*}\widetilde{C}\equiv C_{0}+kF where FF is some fixed general fiber.

Claim 8.3.

The section ρC~\rho_{*}\widetilde{C} deforms on 𝔽\mathbb{F} to the sum of a relatively free section on 𝔽\mathbb{F} and a general fiber of ψ\psi.

Proof of claim:.

Assume for a contradiction that it does not. By Theorem 4.7 we see that

max{2,2g(B)+1,4g(B)+1neg(𝔽,K𝔽/B)}>K𝔽/BC~=deg(2).\max\{2,2g(B)+1,4g(B)+1-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\}>-K_{\mathbb{F}/B}\cdot\widetilde{C}=\deg(\mathcal{L}_{2}).

By Lemma 2.12 we have neg(𝔽,K𝔽/B)g(B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\geq-g(B), so that the supremum is achieved by 4g(B)+1neg(𝔽,K𝔽/B)4g(B)+1-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}) unless g(B)=0g(B)=0 where the supremum is 22. Thus (even in the genus 0 case) we have

neg(𝔽,K𝔽/B)deg(2)4g(B)2.-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\geq\deg(\mathcal{L}_{2})-4g(B)-2. (8.1)

On the other hand, note that

deg(1)+deg(2)\displaystyle\deg(\mathcal{L}_{1})+\deg(\mathcal{L}_{2}) =K𝒳/BC\displaystyle=-K_{\mathcal{X}/B}\cdot C
=ϕK𝒳/BρC0kϕK𝒳/BF\displaystyle=-\phi^{*}K_{\mathcal{X}/B}\cdot\rho^{*}C_{0}-k\phi^{*}K_{\mathcal{X}/B}\cdot F
ϕK𝒳/BC~0kϕK𝒳/BF\displaystyle\geq-\phi^{*}K_{\mathcal{X}/B}\cdot\widetilde{C}_{0}-k\phi^{*}K_{\mathcal{X}/B}\cdot F

where the last inequality follows from the fact that ρC0C~0\rho^{*}C_{0}-\widetilde{C}_{0} is effective and ϕK𝒳/B-\phi^{*}K_{\mathcal{X}/B} is ψ\psi-relatively nef. Also, by arguing on 𝔽\mathbb{F} we see that

deg(2)=K𝔽/BρC~=K𝔽/BC0+2k.\deg(\mathcal{L}_{2})=-K_{\mathbb{F}/B}\cdot\rho_{*}\widetilde{C}=-K_{\mathbb{F}/B}\cdot C_{0}+2k. (8.2)

Substituting and simplifying, we see that

deg(1)neg(𝒳,K𝒳/B)+k(ϕK𝒳/BF2)neg(𝔽,K𝔽/B).\deg(\mathcal{L}_{1})\geq\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+k(-\phi^{*}K_{\mathcal{X}/B}\cdot F-2)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}). (8.3)

We now split the argument into two cases. First, suppose that K𝒳/BF3-K_{\mathcal{X}/B}\cdot F\geq 3. Then we obtain

deg(1)\displaystyle\deg(\mathcal{L}_{1}) neg(𝒳,K𝒳/B)+kneg(𝔽,K𝔽/B)\displaystyle\geq\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+k-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})
=neg(𝒳,K𝒳/B)+12deg(2)32neg(𝔽,K𝔽/B)\displaystyle=\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+\frac{1}{2}\deg(\mathcal{L}_{2})-\frac{3}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})

Using the lower bound on neg(𝔽,K𝔽/B)-\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}) from Equation (8.1), we find altogether

deg(2)deg(1)neg(𝒳,K𝒳/B)+2deg(2)6g(B)3.\deg(\mathcal{L}_{2})\geq\deg(\mathcal{L}_{1})\geq\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+2\deg(\mathcal{L}_{2})-6g(B)-3.

Thus

K𝒳/BC2deg(2)22neg(𝒳,K𝒳/B)+12g(B)+4-K_{\mathcal{X}/B}\cdot C\leq 2\deg(\mathcal{L}_{2})-2\leq-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+12g(B)+4

contradicting our degree bounds.

Second, suppose that K𝒳/BF=2-K_{\mathcal{X}/B}\cdot F=2. Then the inequality (8.3) and (8.1) yield

deg(1)\displaystyle\deg(\mathcal{L}_{1}) neg(𝒳,K𝒳/B)+deg(2)4g(B)2.\displaystyle\geq\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+\deg(\mathcal{L}_{2})-4g(B)-2.

In particular this means that

K𝒳/BC=deg(1)+deg(2)2deg(1)neg(𝒳,K𝒳/B)+4g(B)+2.-K_{\mathcal{X}/B}\cdot C=\deg(\mathcal{L}_{1})+\deg(\mathcal{L}_{2})\leq 2\deg(\mathcal{L}_{1})-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+4g(B)+2. (8.4)

Then we have

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C =ρϕK𝒳/BρC~\displaystyle=-\rho_{*}\phi^{*}K_{\mathcal{X}/B}\cdot\rho_{*}\widetilde{C}
ϕK𝒳/BC~0+2k\displaystyle\geq-\phi^{*}K_{\mathcal{X}/B}\cdot\widetilde{C}_{0}+2k

where the last inequality follows from the relative nefness of K𝒳/B-K_{\mathcal{X}/B}. Combining with Equation (8.2) and (8.1), we see that

2deg(1)2deg(2)+8g(B)+4neg(𝒳,K𝒳/B)>ϕK𝒳/BC~0.2\deg(\mathcal{L}_{1})-2\deg(\mathcal{L}_{2})+8g(B)+4-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})>-\phi^{*}K_{\mathcal{X}/B}\cdot\widetilde{C}_{0}.

In particular, the image C0C_{0} of C~0\widetilde{C}_{0} in 𝒳\mathcal{X} has height at most 8g(B)neg(𝒳,K𝒳/B)8g(B)-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B}). Note that any aa general points of Σ~\widetilde{\Sigma} will also be general in 𝒳\mathcal{X}. Thus by adding on aa general fibers to C~0\widetilde{C}_{0} and taking the image in 𝒳\mathcal{X}, we obtain a reducible curve C0+SC_{0}+S where C0C_{0} is a section, SS is π\pi-vertical, and the entire curve goes through aa general points of 𝒳\mathcal{X}. By Lemma 7.3 either

K𝒳/BC0+2aK𝒳/BC0+3a32maxdef(8g(B)neg(𝒳,K𝒳/B))-K_{\mathcal{X}/B}\cdot C_{0}+2a\geq-K_{\mathcal{X}/B}\cdot C_{0}+3a-\frac{3}{2}\mathrm{maxdef}(\leq 8g(B)-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B}))

or a<maxdef(8g(B)neg(𝒳,K𝒳/B))a<\mathrm{maxdef}(\leq 8g(B)-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})). Together these show that a32maxdef(8g(B)neg(𝒳,K𝒳/B))a\leq\frac{3}{2}\mathrm{maxdef}(\leq 8g(B)-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})). Then by Equation (8.4) and the fact that deg(1)=a+g(B)1\deg(\mathcal{L}_{1})=a+g(B)-1 we have

K𝒳/BC3maxdef(8g(B)neg(𝒳,K𝒳/B))neg(𝒳,K𝒳/B)+6g(B)-K_{\mathcal{X}/B}\cdot C\leq 3\mathrm{maxdef}(\leq 8g(B)-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B}))-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+6g(B)

contradicting our degree bound. ∎

Having proved the claim, we now return to the main argument. Since a general deformation of a relatively free section on 𝔽\mathbb{F} will avoid any codimension 22 locus, we may assume that the curves C~1\widetilde{C}_{1} and FF constructed on 𝔽\mathbb{F} in Claim 8.3 avoid the exceptional centers of Σ~𝔽\widetilde{\Sigma}\to\mathbb{F}. Thus by taking the strict transforms of these curves, we have shown that on Σ~\widetilde{\Sigma} the curves C~\widetilde{C} deform to curves of the form C~1+F\widetilde{C}_{1}+F where FF is a general fiber of π\pi and C~1\widetilde{C}_{1} is relatively free in Σ~\widetilde{\Sigma} that is general in its deformation class. Moreover since C~\widetilde{C} avoids the preimage of the singularities in 𝒳\mathcal{X} and Σ\Sigma^{\prime}, we may ensure that C~1\widetilde{C}_{1} avoids the preimage of the singularities of 𝒳\mathcal{X} and Σ\Sigma^{\prime}. Indeed since a relatively free section avoids any codimension 22 loci, C~1\widetilde{C}_{1} avoids 0-dimensional preimages of singularities. For 11-dimensional preimages of singularities since C~\widetilde{C} avoids such loci, the intersection number of C~\widetilde{C} to such loci is 0. Then since C~1\widetilde{C}_{1} shares the same intersection property with C~\widetilde{C}, we conclude that it avoids any preimage of singularities. Moreover we may assume that the image of the intersection of C~1\widetilde{C}_{1} and FF is a smooth point of the image of FF in 𝒳\mathcal{X}.

Our plan is to show that C~1\widetilde{C}_{1} is relatively free in 𝒳\mathcal{X} and that FF is free in 𝒳\mathcal{X}, yielding the desired deformation of CC. We separate the argument into two cases depending on the stability of the normal bundle of C~1\widetilde{C}_{1}.

If NC~1/𝒳N_{\widetilde{C}_{1}/\mathcal{X}} is semistable, then C~1\widetilde{C}_{1} is relatively free by Proposition 3.6 and Corollary 3.7 (2). Indeed, it follows from Proposition 3.14 that the normal bundle NC~/Σ~N_{\widetilde{C}/\widetilde{\Sigma}} is given by 2\mathcal{L}_{2}. Then since deg(NC~1/Σ~)=deg(2)2deg(1)\deg(N_{\widetilde{C}_{1}/\widetilde{\Sigma}})=\deg(\mathcal{L}_{2})-2\geq\deg(\mathcal{L}_{1}) and since Σ~\widetilde{\Sigma} contains the aa general points {x1,,xa}\{x_{1},\cdots,x_{a}\} that we have fixed, we conclude that a deformation of C~1\widetilde{C}_{1} also contains these aa general points so that h0(C~1,NC~1/𝒳)4g(B)+2h^{0}(\widetilde{C}_{1},N_{\widetilde{C}_{1}/\mathcal{X}})\geq 4g(B)+2 by Proposition 3.6 (2). Thus C~1\widetilde{C}_{1} is relatively free by Corollary 3.7 (2). Since FF is free on Σ~\widetilde{\Sigma} and Σ\Sigma contains a general point of 𝒳\mathcal{X}, the image of FF is free on 𝒳\mathcal{X}, finishing the argument in this case.

Suppose that NC~1/𝒳N_{\widetilde{C}_{1}/\mathcal{X}} is unstable with the maximal destabilizing exact sequence:

02NC~1/𝒳10.0\to\mathcal{L}_{2}^{\prime}\to N_{\widetilde{C}_{1}/\mathcal{X}}\to\mathcal{L}_{1}^{\prime}\to 0.

Then after reselecting aa general points q1,,qaq_{1},\cdots,q_{a} on C~1\widetilde{C}_{1} we have

h0(C~1,NC~1/𝒳)=h0(C~1,NC~1/𝒳(q1qa))+2a.h^{0}(\widetilde{C}_{1},N_{\widetilde{C}_{1}/\mathcal{X}})=h^{0}(\widetilde{C}_{1},N_{\widetilde{C}_{1}/\mathcal{X}}(-q_{1}-\cdots-q_{a}))+2a.

Note that our surface Σ\Sigma does not depend on the choice of qiq_{i}’s because of Lemma 3.13. This means that

h0(C~1,1)=h0(C~1,1(q1qa))+aa.h^{0}(\widetilde{C}_{1},\mathcal{L}_{1}^{\prime})=h^{0}(\widetilde{C}_{1},\mathcal{L}_{1}^{\prime}(-q_{1}-\cdots-q_{a}))+a\geq a.

Corollary 3.7 (1) shows that C~1\widetilde{C}_{1} is relatively free on 𝒳\mathcal{X}. Similarly, since FF is free on Σ~\widetilde{\Sigma}, it is also free on 𝒳\mathcal{X}.

Case 4: NC/𝒳N_{C/\mathcal{X}} is unstable with the maximal destabilizing exact sequence

02NC/𝒳100\to\mathcal{L}_{2}\to N_{C/\mathcal{X}}\to\mathcal{L}_{1}\to 0

such that deg(1)<3g(B)<7g(B)+3deg(2)\deg(\mathcal{L}_{1})<3g(B)<7g(B)+3\leq\deg(\mathcal{L}_{2}). As before we write a=H0(C,1)=deg(1)+1g(B)2g(B)a=H^{0}(C,\mathcal{L}_{1})=\deg(\mathcal{L}_{1})+1-g(B)\leq 2g(B) and b=H0(C,2)=deg(2)+1g(B)b=H^{0}(C,\mathcal{L}_{2})=\deg(\mathcal{L}_{2})+1-g(B). By Proposition 3.6 deformations of CC can contain aa general points of 𝒳\mathcal{X}. Consider a component Σ\Sigma of the locus swept out by the curves in MM through aa general points {x1,,xa}\{x_{1},\ldots,x_{a}\}; we may assume that the normal bundle of the general curve sweeping out Σ\Sigma has a Harder-Narasimhan filtration of generic type and {x1,,xa}\{x_{1},\ldots,x_{a}\} are general on CC. We know that Σ𝒳\Sigma\subsetneq\mathcal{X} and a dimension count shows that it is a surface. In fact, since each general point imposes 22 independent conditions on the moduli space, there is a (ba)(b-a)-dimensional family of curves through these general points which sweep out Σ\Sigma.

Let ϕ:Σ~Σ\phi:\widetilde{\Sigma}\to\Sigma be the minimal resolution. The results in Section 3.4 show that Σ~Σ\widetilde{\Sigma}\to\Sigma is finite on an open neighborhood of a general section CC sweeping out Σ\Sigma and the strict transforms C~\widetilde{C} will define a dominant family of sections of Σ~\widetilde{\Sigma} which have normal bundle 2\mathcal{L}_{2}. In particular the induced map ψ:Σ~B\psi:\widetilde{\Sigma}\to B has connected fibers. Since deg(2)g(B)+2\deg(\mathcal{L}_{2})\geq g(B)+2 the usual Bend-and-Break theorem shows that the general fiber of ψ\psi is 1\mathbb{P}^{1}.

Apply Corollary 4.3 to find a ruled surface 𝔽\mathbb{F} and a birational map ρ:Σ~𝔽\rho:\widetilde{\Sigma}\to\mathbb{F} which is an isomorphism on a neighborhood of C~\widetilde{C}. As in Proposition 4.9 (1) we can write C~C~0+kF+T\widetilde{C}\equiv\widetilde{C}_{0}+kF+T where FF is a general fiber of the map to BB and

k=12(KΣ~/BC~)12neg(𝔽,K𝔽/B).k=\frac{1}{2}(-K_{\widetilde{\Sigma}/B}\cdot\widetilde{C})-\frac{1}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B}).

Since NC~/Σ~=2N_{\widetilde{C}/\widetilde{\Sigma}}=\mathcal{L}_{2} has vanishing H1H^{1}, the component parametrizing deformations of C~\widetilde{C} in Σ\Sigma has the expected dimension. Thus we have

KΣ~/BC~+1g(B)K𝒳/BC+2(1g(B))2a-K_{\widetilde{\Sigma}/B}\cdot\widetilde{C}+1-g(B)\geq-K_{\mathcal{X}/B}\cdot C+2(1-g(B))-2a

Then

5g(B)1\displaystyle 5g(B)-1 2a+g(B)1\displaystyle\geq 2a+g(B)-1
KΣ~/BC~ϕK𝒳/B|ΣC~\displaystyle\geq K_{\widetilde{\Sigma}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma}\cdot\widetilde{C}
=KΣ~/BC~ϕK𝒳/B|ΣC~0+k(ϕK𝒳/B|ΣF)ϕK𝒳/B|ΣT\displaystyle=K_{\widetilde{\Sigma}/B}\cdot\widetilde{C}-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma}\cdot\widetilde{C}_{0}+k(-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma}\cdot F)-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma}\cdot T
KΣ~/BC~+neg(𝒳,K𝒳/B)+k(ϕK𝒳/B|ΣF)\displaystyle\geq K_{\widetilde{\Sigma}/B}\cdot\widetilde{C}+\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+k(-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma}\cdot F) (8.5)

where we have used the fact that K𝒳/B-K_{\mathcal{X}/B} is relatively nef at the last step. Suppose for a contradiction that there is an inequality a(Σ~η,ϕK𝒳/B|Σ)<a(Xη,K𝒳/B)a(\widetilde{\Sigma}_{\eta},-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma})<a(X_{\eta},-K_{\mathcal{X}/B}). This is equivalent to saying that ϕK𝒳/B|ΣF3-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma}\cdot F\geq 3. Rearranging and substituting in our value for kk, we find

12(KΣ~/BC~)32neg(𝔽,K𝔽/B)neg(𝒳,K𝒳/B)+5g(B)1.\displaystyle\frac{1}{2}(-K_{\widetilde{\Sigma}/B}\cdot\widetilde{C})-\frac{3}{2}\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq-\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+5g(B)-1.

Using the inequality neg(𝔽,K𝔽/B)g(B)\mathrm{neg}(\mathbb{F},-K_{\mathbb{F}/B})\leq g(B) from Corollary 4.3, we see that

K𝒳/BC\displaystyle-K_{\mathcal{X}/B}\cdot C KΣ~/BC~+5g(B)1\displaystyle\leq-K_{\widetilde{\Sigma}/B}\cdot\widetilde{C}+5g(B)-1
2neg(𝒳,K𝒳/B)+18g(B)3.\displaystyle\leq-2\mathrm{neg}(\mathcal{X},-K_{\mathcal{X}/B})+18g(B)-3.

contradicting our height bound. Thus we see that a(Ση,K𝒳/B|Σ)a(Xη,K𝒳/B)a(\Sigma_{\eta},-K_{\mathcal{X}/B}|_{\Sigma})\geq a(X_{\eta},-K_{\mathcal{X}/B}). Since the subvarieties Σ\Sigma with larger generic aa-invariant lie in a closed set but CC is a member of a dominant family, we see that we must have equality of generic aa-invariants, i.e. ϕK𝒳/B|ΣF=2-\phi^{*}K_{\mathcal{X}/B}|_{\Sigma}\cdot F=2. Using the arguments in Case 3 we conclude that ρC~\rho_{*}\widetilde{C} deforms on 𝔽\mathbb{F} to the sum of a section C~1\widetilde{C}_{1} that is relatively free in Σ~\widetilde{\Sigma} and a general fiber FF of ψ\psi. When Σ\Sigma contains some singular points of 𝒳\mathcal{X}, we may assume that C~\widetilde{C} does not meet with the preimage of these singular points on Σ~\widetilde{\Sigma}. This implies that we can assume that C~1\widetilde{C}_{1} also avoids this preimage. Note that since Σ\Sigma contains a general point of 𝒳\mathcal{X}, the general fiber of ΣB\Sigma\to B will be a nodal rational curve of anticanonical degree 22 by Lemma 2.15. Applying Lemma 6.8 to C~\widetilde{C} and C~1\widetilde{C}_{1} with the surface Σ\Sigma and the constant c=5g(B)1c=5g(B)-1, we see that

h1(C~1,NC~1/𝒳)=h1(C,NC/𝒳)=0.h^{1}(\widetilde{C}_{1},N_{\widetilde{C}_{1}/\mathcal{X}})=h^{1}(C,N_{C/\mathcal{X}})=0.

Hence C~1\widetilde{C}_{1} is relatively free in 𝒳\mathcal{X}. ∎

By applying Movable Bend-and-Break repeatedly, one can prove the following version.

Corollary 8.4.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Let MM be a component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing a family of relatively free sections of height MBBbound(𝒳)\geq\mathrm{MBBbound}(\mathcal{X}). Then the closure M¯\overline{M} in M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) contains a point representing the union of a relatively free section of height <MBBbound(𝒳)<\mathrm{MBBbound}(\mathcal{X}) with a chain of π\pi-vertical free curves of anticanonical degree 3\leq 3 contained in a general fiber of π\pi. Furthermore the section meets the chain of π\pi-vertical curves at a smooth point of the chain.

The argument is very similar to the arguments in [LT19a, Section 7], and so we will only sketch the proof.

Proof.

First, by applying Movable Bend-and-Break inductively we can find a stable map in M¯\overline{M} whose domain is a comb – that is, the union of a curve C0C_{0} of genus g(B)g(B) with several rational curves meeting C0C_{0} transversally at distinct points – which maps C0C_{0} onto a relatively free section of height <MBBbound(𝒳)<\mathrm{MBBbound}(\mathcal{X}) and each rational curve onto a free π\pi-vertical curve. By deforming and gluing the π\pi-vertical components as in [LT19a, Theorem 7.7] using Lemma 3.11, one can then find a stable map in M¯\overline{M} whose domain is the union of a genus g(B)g(B) curve and a single rational curve such that the genus g(B)g(B) curve is mapped to a relatively free section of height <MBBbound(𝒳)<\mathrm{MBBbound}(\mathcal{X}) and the rational curve is mapped to a free π\pi-vertical curve in a general fiber FF of π\pi. Moreover we may assume that the intersection of the section and the vertical rational curve is a smooth point of the vertical curve. Finally, applying [LT19a, Lemma 2.12] we can deform this π\pi-vertical curve in FF to a chain of anticanonical conics and cubics while fixing the attachment point to C0C_{0}. ∎

By regluing all but one of the vertical components to the section, we obtain the following version:

Corollary 8.5.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. Let MM be a component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) parametrizing a family of sections of height MBBbound(𝒳)\geq\mathrm{MBBbound}(\mathcal{X}). Then the closure M¯\overline{M} in M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) contains a point representing the union of a relatively free section with a π\pi-vertical free curve of anticanonical degree 3\leq 3. Furthermore the section meets the π\pi-vertical curve at a smooth point.

We also obtain a statement about the fibers of the evaluation map for the universal family of sections.

Theorem 8.6.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration with K𝒳/B-K_{\mathcal{X}/B} relatively ample. Suppose that MM is a component of Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} where dMBBbound(𝒳)+2d\geq\mathrm{MBBbound}(\mathcal{X})+2 and that MM generically parametrizes relatively free sections. Then any resolution of the evaluation map of the universal family over MM has connected fibers.

The proof is similar to [LT19a, Corollary 7.10]: let Y𝒳Y\to\mathcal{X} denote the Stein factorization of the evaluation map. We first use Movable Bend-and-Break to break off some π\pi-vertical free rational curves on 𝒳\mathcal{X}. By construction these must be the images of some π\pi-vertical free rational curves on YY. Then by applying [LT17, Theorem 6.2] to the generic fiber of π\pi we see that Y𝒳Y\to\mathcal{X} must be birational. We omit the details here, referring the reader to [LT19a, Corollary 7.10].

9. Batyrev’s heuristic

Suppose that π:𝒳B\pi:\mathcal{X}\to B is a del Pezzo fibration. Batyrev’s heuristic for Manin’s Conjecture indicates that the number of components of Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} should be bounded above by a polynomial in dd. In this section we prove this statement for Fano fibrations of relative dimension 11 and 22.

Proposition 9.1.

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration of relative dimension 11. Fix a numerical class αN1(𝒳)\alpha\in N_{1}(\mathcal{X}). When the anticanonical degree of α\alpha is sufficiently large, there is at most one component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) representing α\alpha. Equivalently, for dd sufficiently large there are exactly |Λ||\Lambda| components of Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} where Λ\Lambda denotes the number of intersection profiles.

In particular this implies that there is a polynomial P(d)P(d) such that the number of components of Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} is bounded above by P(d)P(d).

Proof.

For each intersection profile λi\lambda_{i} Lemma 4.5 yields a birational map ϕi:𝒳𝔽i\phi_{i}:\mathcal{X}\to\mathbb{F}_{i} to a ruled surface 𝔽i\mathbb{F}_{i}. The set of components of Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} with intersection profile λ\lambda is in bijection with the set of components of Sec(𝔽i/B)d\mathrm{Sec}(\mathbb{F}_{i}/B)_{d}. Thus it suffices to prove the statement for ruled surfaces.

Let \mathcal{E} denote a rank 22 bundle on BB defining the 1\mathbb{P}^{1}-bundle 𝔽i\mathbb{F}_{i}. Suppose that the height dd is sufficiently large so that every twist of \mathcal{E} by a divisor of degree dd is globally generated and has vanishing H1H^{1}. Then there is a unique component of Sec(𝔽i/B)\mathrm{Sec}(\mathbb{F}_{i}/B) of degree dd. This proves the first statement.

To see the second statement, note that in each intersection profile there is at most one numerical class of anticanonical degree dd. By combining with the argument above we obtain the second statement. ∎

We next turn to the del Pezzo fibration case.

Theorem 9.2.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively ample. There is some polynomial P(d)P(d) such that the number of components of Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} is bounded above by P(d)P(d).

The hardest case of the theorem is when the component MM parametrizes a dominant family of sections that is not relatively free so we explain this case separately.

Proposition 9.3.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that K𝒳/B-K_{\mathcal{X}/B} is relatively nef. There is an upper bound R=R(𝒳)R=R(\mathcal{X}) on the number of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which parametrize a dominant family of non-relatively free curves representing a fixed numerical class.

Proof.

Suppose that MM parametrizes a dominant family of non-relatively-free sections on 𝒳\mathcal{X} of sufficiently large height and let qq be the maximal number of general points contained in the sections parametrized by MM. Fix the bounded family of surfaces 𝒮N\mathcal{S}\to N defined by Corollary 6.7. Let M[q]M^{[q]} be the space of sections parametrized by MM with qq marked points. This is an irreducible variety; we denote its normalization by M~[q]\widetilde{M}^{[q]}. Consider the evaluation map M~[q]Xq\widetilde{M}^{[q]}\to X^{q}. Theorem 6.6 shows that for any component of a general fiber of this map the sections parametrized by this component will sweep out an irreducible surface parametrized by 𝒮\mathcal{S}. Thus the Stein factorization of M~[q]Xq\widetilde{M}^{[q]}\to X^{q} admits a rational map to the parameter space 𝒩\mathcal{N}. This means that if we let {Ni}\{N_{i}\} denote the stratification of NN as in Lemma 5.1 there is a unique stratum NiN_{i} which contains the general surface swept out by sections in MM through qq general points. Corollary 5.2 shows that in fact for every surface parametrized by NiN_{i} there will be a family of sections on a resolution of the surface which will be parametrized by some sublocus of MM. Thus the sublocus of MM swept out by families of sections on the surfaces parametrized by the stratum NiN_{i} will contain a dense open subset of MM.

In particular, fix a surface Y~\widetilde{Y} parametrized by NiN_{i}. The component MM is uniquely determined by the anticanonical degree of the sections in Y~\widetilde{Y} and the intersection profile of any family of sections in Y~\widetilde{Y} which are contained in MM. Note that if we fix the numerical class of the sections in 𝒳\mathcal{X} and fix an intersection profile in Y~\widetilde{Y} then there is a unique family on Y~\widetilde{Y} which pushes forward to the given numerical class on 𝒳\mathcal{X} because our height is sufficiently large. Thus we see that there is a universal upper bound on the number of families of curves that sweep out surfaces in the stratum NiN_{i} and which push forward to a given numerical class on 𝒳\mathcal{X}. Since there are only finitely many strata NiN_{i}, we obtain the desired upper bound. ∎

Proof of Theorem 9.2:.

We consider separately non-dominant families, dominant but not relatively free families, and relatively free families. Note that by Lemma 2.2 in each case it suffices to prove the statement only for those sections whose anticanonical degree is sufficiently large.

Every non-dominant family of sections of sufficiently large height will sweep out a surface YY in 𝒳\mathcal{X}. By Theorem 5.3 when the height is sufficiently large this surface YY will be a ruled surface and by Corollary 5.4 only finitely many such surfaces can be obtained in this way. It suffices to prove the statement for each surface YY separately. This follows from Proposition 9.1. (Note that the height function used here may be different from the height function in Proposition 9.1. Nevertheless, it is easy to show that a polynomial bound with respect to one height function will yield a polynomial bound for the other.)

Suppose that MSec(𝒳/B)dM\subset\mathrm{Sec}(\mathcal{X}/B)_{d} is a component parametrizing a dominant family of non-relatively free sections. Proposition 9.3 proves that there is an upper bound RR on the number of such components representing any fixed numerical class, and this immediately implies the desired polynomial bound.

Finally, suppose that MSec(𝒳/B)dM\subset\mathrm{Sec}(\mathcal{X}/B)_{d} is a component parametrizing a dominant family of sections which are generically relatively free. By Corollary 8.4 MM can be obtained by gluing a relatively free section CC of height <MBBbound(𝒳)<\mathrm{MBBbound}(\mathcal{X}) to a chain of π\pi-vertical free curves each which has anticanonical degree 22 or 33. By [LT19b, Theorem 5.13] there is a polynomial Q(r)Q(r) which bounds the number of components of M¯0,0(𝒳)\overline{M}_{0,0}(\mathcal{X}) of anticanonical degree rr that can be obtained by smoothing chains of free curves of these types. Let cc be the maximal degree of the Stein factorization of the evaluation map for any family of relatively free sections of height <MBBbound(𝒳)<\mathrm{MBBbound}(\mathcal{X}) and set r=d+K𝒳/BCr=d+K_{\mathcal{X}/B}\cdot C. Then by gluing CC to a smoothing of a chain of π\pi-vertical curves of total anticanonical degree rr we can get at most cQ(r)cQ(r) components of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}). By summing up these contributions over the finite set of families of relatively free sections of height <MBBbound(𝒳)<\mathrm{MBBbound}(\mathcal{X}), we obtain the desired bound. ∎

10. Geometric Manin’s Conjecture

In this section we recall the definition of the counting function in Geometric Manin’s Conjecture and clarify its relationship to the structural theorems proved earlier.

Suppose that π:𝒳B\pi:\mathcal{X}\to B is a del Pezzo fibration such that 𝒳\mathcal{X} is smooth. Recall from Section 2 that N1(𝒳)N_{1}(\mathcal{X}) is defined to be the space of real 11-cycles modulo numerical equivalence and N1(𝒳)N_{1}(\mathcal{X})_{\mathbb{Z}} is the lattice of integral 11-cycles. Similarly, N1(𝒳)N^{1}(\mathcal{X}) is the space of \mathbb{R}-divisors modulo numerical equivalence and N1(𝒳)N^{1}(\mathcal{X})_{\mathbb{Z}} is the lattice of integral Cartier divisors. Dual to the restriction map N1(𝒳)N1(𝒳η)N^{1}(\mathcal{X})\to N^{1}(\mathcal{X}_{\eta}) we have a pushforward map N1(𝒳η)N1(𝒳)N_{1}(\mathcal{X}_{\eta})\to N_{1}(\mathcal{X}). Henceforth we will identify N1(𝒳η)N_{1}(\mathcal{X}_{\eta}) with this subspace of N1(𝒳)N_{1}(\mathcal{X}). Note however that the lattice N1(𝒳η)N_{1}(\mathcal{X}_{\eta})_{\mathbb{Z}} may be strictly contained in the lattice N1(𝒳η)N1(𝒳)N_{1}(\mathcal{X}_{\eta})\cap N_{1}(\mathcal{X})_{\mathbb{Z}}.

10.1. Counting components

Let π:𝒳B\pi:\mathcal{X}\to B be a Fano fibration. A key piece of Geometric Manin’s Conjecture is a precise bound on the number of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) representing a fixed numerical class. We expect the following principle to hold:

Principle 10.1.

Any “sufficiently positive” algebraic equivalence class of sections on 𝒳\mathcal{X} is represented by at most one family of relatively free sections.

Here “sufficiently positive” is supposed to be taken with respect to the cone Nef1(𝒳η)\mathrm{Nef}_{1}(\mathcal{X}_{\eta}) in N1(𝒳)N_{1}(\mathcal{X}). We will give a more precise formulation of this statement for del Pezzo fibrations below. The best evidence for Principle 10.1 comes from fibrations of the form X×1X\times\mathbb{P}^{1} where XX is a Fano variety: there are many classes of Fano variety for which the components of Mor(1,X)\mathrm{Mor}(\mathbb{P}^{1},X) have been classified and all examples that we know of are compatible with this principle (see Section 1.4).

In order to translate this statement to numerical equivalence, one must know how many algebraic equivalence classes there are representing a fixed numerical class. Let 𝒳\mathcal{X} be a smooth threefold admitting a morphism π\pi to a curve BB whose fibers are connected and rationally connected. For any section CC of π\pi the pushforward map CH0(C)CH0(𝒳)\mathrm{CH}_{0}(C)\to\mathrm{CH}_{0}(\mathcal{X}) is surjective. Thus by [Voi03, Theorem 10.17] we have H2,0(𝒳)=0H^{2,0}(\mathcal{X})=0 so that

Br(𝒳)H3(𝒳,)tors.\mathrm{Br}(\mathcal{X})\cong H^{3}(\mathcal{X},\mathbb{Z})_{\mathrm{tors}}.

According to the universal coefficient theorem, we can equally well think of Br(𝒳)\mathrm{Br}(\mathcal{X}) as the torsion classes of H2(𝒳,)H_{2}(\mathcal{X},\mathbb{Z}). Let Q1(𝒳)Q_{1}(\mathcal{X}) denote the set of algebraic equivalence classes of curves of 𝒳\mathcal{X}. [BS83, Theorem 1] shows that algebraic and homological equivalence coincide for curve classes on 𝒳\mathcal{X} and [Voi06, Theorem 2] proves the integral Hodge conjecture for 𝒳\mathcal{X}. Together these show:

Theorem 10.2 ([BS83], [Voi06]).

Let 𝒳\mathcal{X} be a smooth threefold admitting a morphism to a curve BB whose fibers are connected and rationally connected. Then |Br(𝒳)||\mathrm{Br}(\mathcal{X})| is the size of the kernel of the quotient map q:Q1(𝒳)N1(𝒳)q:Q_{1}(\mathcal{X})\to N_{1}(\mathcal{X})_{\mathbb{Z}}.

Thus, Principle 10.1 can be interpreted as follows:

Conjecture 10.3.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration with 𝒳\mathcal{X} smooth. Fix an intersection profile λ\lambda and let NλN_{\lambda} denote the affine subset of N1(𝒳)N_{1}(\mathcal{X}) consisting of curve classes whose intersection numbers with π\pi-vertical divisors are described by λ\lambda. Define Nefλ=Nef1(𝒳)Nλ\mathrm{Nef}_{\lambda}=\mathrm{Nef}_{1}(\mathcal{X})\cap N_{\lambda}. There is some translate 𝒯\mathcal{T} of Nefλ\mathrm{Nef}_{\lambda} in NλN_{\lambda} such that every class in 𝒯\mathcal{T}_{\mathbb{Z}} is represented by exactly |Br(𝒳)||\mathrm{Br}(\mathcal{X})| different families of relatively free sections.

10.2. Formulating Geometric Manin’s Conjecture

Throughout this section π:𝒳B\pi:\mathcal{X}\to B denotes a del Pezzo fibration such that 𝒳\mathcal{X} is smooth and K𝒳/B-K_{\mathcal{X}/B} is relatively ample. For simplicity, we will assume that the general fibers are not isomorphic to 2\mathbb{P}^{2} or 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}. (In these two cases one must adjust the counting function slightly to reflect the fact that the general fiber does not contain any curve class with anticanonical degree 11.)

The most general version of Geometric Manin’s Conjecture is formulated using the Fujita invariant to construct the exceptional set as in [LST18]. For del Pezzo fibrations, the general construction of the exceptional set in [LST18] has the following simple description.

Definition 10.4 ([LT19c] Theorem 9.1).

We say that a component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) is an accumulating component if either:

  1. (1)

    the sections sweep out a surface YY whose intersection with a general fiber is an anticanonical line, or

  2. (2)

    ρ(𝒳η)=1\rho(\mathcal{X}_{\eta})=1 and the sections sweep out a surface YY whose intersection with a general fiber is a singular anticanonical conic.

Any component MM which is not an accumulating component is called a Manin component. We let Manini\mathrm{Manin}_{i} denote the set of Manin components that parametrize sections CC satisfying K𝒳/BC=i-K_{\mathcal{X}/B}\cdot C=i.

Remark 10.5.

Definition 10.4 (2) is very restrictive. Since the condition ρ(𝒳η)=1\rho(\mathcal{X}_{\eta})=1 implies that the Picard group is generated by a multiple of K𝒳η-K_{\mathcal{X}_{\eta}} the existence of an anticanonical conic means that 𝒳η\mathcal{X}_{\eta} must be a del Pezzo surface of degree 2\leq 2.

Remark 10.6.

The relationship between Definition 10.4 and families of non-relatively free sections is a little subtle. We will make this connection precise in the following section.

The counting function in Geometric Manin’s Conjecture encodes the number and dimension of Manin components representing sections of height at most dd.

Definition 10.7.

Fix a real number q>1q>1. For any positive integer dd define

N(𝒳,K𝒳/B,q,d):=i=1dMManiniqdimM.N(\mathcal{X},-K_{\mathcal{X}/B},q,d):=\sum_{i=1}^{d}\sum_{M\in\mathrm{Manin}_{i}}q^{\dim M}.

Geometric Manin’s Conjecture predicts the asymptotic growth rate of this counting function as we let dd go to \infty. The expected growth rate is

N(𝒳,K𝒳/B,q,d)dCqddρ(𝒳η)1N(\mathcal{X},-K_{\mathcal{X}/B},q,d)\sim_{d\to\infty}Cq^{d}d^{\rho(\mathcal{X}_{\eta})-1}

for some constant CC.

Remark 10.8.

Given a section CC of a del Pezzo fibration π:𝒳B\pi:\mathcal{X}\to B, we can always construct a relatively free section as follows. Choose a resolution ϕ:𝒳~𝒳\phi:\widetilde{\mathcal{X}}\to\mathcal{X} and let C~\widetilde{C} denote the strict transform of CC. By gluing C~\widetilde{C} with suitably chosen free curves in the fibers of ϕπ\phi\circ\pi we can ensure that after smoothing we obtain a section T~\widetilde{T} through 2g(B)+12g(B)+1 general points of 𝒳~\widetilde{\mathcal{X}}. By Corollary 3.7 a general deformation of the pushforward of T~\widetilde{T} to 𝒳\mathcal{X} will be relatively free.

By varying the choice of curves we glue on, it is not hard to show that the resulting relatively free sections generate a translate of a full-dimensional subcone of Nef1(𝒳η)\mathrm{Nef}_{1}(\mathcal{X}_{\eta}). In particular, this shows that the asymptotic growth rate of N(𝒳,K𝒳/B,q,d)N(\mathcal{X},-K_{\mathcal{X}/B},q,d) is bounded below by Cqddρ(𝒳η)1Cq^{d}d^{\rho(\mathcal{X}_{\eta})-1} for some constant CC.

10.3. Upper bounds on the counting function

As in the previous section π:𝒳B\pi:\mathcal{X}\to B denotes a del Pezzo fibration such that 𝒳\mathcal{X} is smooth and K𝒳/B-K_{\mathcal{X}/B} is relatively ample and (for simplicity) we assume that the general fiber of π\pi is not isomorphic to 2\mathbb{P}^{2} or 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}.

In order to verify Geometric Manin’s Conjecture, we first must explicitly identify the accumulating components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B). We also must bound the contributions of the Manin components to the counting function. The following claims summarize the roles of each type of component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) in Geometric Manin’s Conjecture:

  1. (1)

    Most non-dominant families of sections will be accumulating components; the ones which are not will give a negligible contribution to the asymptotic growth of the counting function N(𝒳,K𝒳/B,q,d)N(\mathcal{X},-K_{\mathcal{X}/B},q,d).

  2. (2)

    Most dominant families of sections which are not relatively free will give a negligible contribution to the asymptotic growth of N(𝒳,K𝒳/B,q,d)N(\mathcal{X},-K_{\mathcal{X}/B},q,d); the ones which do not will be accumulating components.

  3. (3)

    Dominant families of sections which are generically relatively free will give a contribution to the asymptotic growth that can be computed using Movable Bend-and-Break.

We will verify these claims in the proof of the following theorem.

Theorem 10.9.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that 𝒳\mathcal{X} is smooth, K𝒳/B-K_{\mathcal{X}/B} is relatively ample, and the general fiber is a del Pezzo surface that is not 2\mathbb{P}^{2} or 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}. Then there is some non-negative integer rr such that

N(𝒳,K𝒳/B,q,d)=O(qddr).N(\mathcal{X},-K_{\mathcal{X}/B},q,d)=O(q^{d}d^{r}).
Proof.

Suppose we fix an intersection profile λ\lambda. The set of sections with intersection profile λ\lambda will be contained in an affine translate 𝒩\mathcal{N} of the subspace N1(𝒳η)N_{1}(\mathcal{X}_{\eta}). We will further restrict our attention to a fixed coset Ξ\Xi of N1(𝒳η)N_{1}(\mathcal{X}_{\eta})_{\mathbb{Z}} inside of 𝒩\mathcal{N}_{\mathbb{Z}}. Since our goal is to prove an upper bound and since there are only finitely many cosets in all the intersection profiles, it suffices to prove an upper bound of the desired type for each coset individually.

Fix a coset Ξ\Xi and choose a translation ψ:𝒩N1(𝒳η)\psi:\mathcal{N}\to N_{1}(\mathcal{X}_{\eta}) which identifies the coset Ξ\Xi with the lattice N1(𝒳η)N_{1}(\mathcal{X}_{\eta})_{\mathbb{Z}}. We now analyze separately the three different types of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which lie in Ξ\Xi. Since we only care about the asymptotic behavior, it suffices to restrict our attention to the families of sections with sufficiently large height.

Case 1: Consider a component MSec(𝒳/B)M\subset\mathrm{Sec}(\mathcal{X}/B) parametrizing a non-dominant family of sections of sufficiently large height. By Theorem 5.3 there is a finite set of surfaces YY satisfying a(Yη,K𝒳/B)a(𝒳η,K𝒳/B)a(Y_{\eta},-K_{\mathcal{X}/B})\geq a(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}) such that the sections parametrized by MM will sweep out one of these surfaces YY. In the case when the inequality of a-invariants is strict the component MM will be accumulating. If instead we have an equality of aa-invariants, there are two cases to consider. First, suppose that ρ(𝒳η)>1\rho(\mathcal{X}_{\eta})>1. According to Proposition 9.1 the surface YY can only contain finitely many components of relative anticanonical degree dd. On the other hand, due to the Picard rank assumption the number of components of Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d} will grow at least linearly. So in this case the contributions of YY to the counting function are negligible. Second, suppose that ρ(𝒳η)=1\rho(\mathcal{X}_{\eta})=1. Note that in this situation the generic fiber YηY_{\eta} must be geometrically irreducible, yielding an anticanonical conic over the ground field in 𝒳η\mathcal{X}_{\eta}. Due to the restriction on the Picard rank, the only option is that 𝒳η\mathcal{X}_{\eta} is a del Pezzo surface of degree 2\leq 2 and Picard rank 11 and that this conic is either:

  1. (1)

    a rational curve in |KX||-K_{X}| if 𝒳η\mathcal{X}_{\eta} has degree 22, or

  2. (2)

    a rational curve in |2KX||-2K_{X}| if 𝒳η\mathcal{X}_{\eta} has degree 11.

Note that each curve of these types is singular and thus is included in the exceptional set. So every component of this type is an accumulating component.

Case 2: Consider the dominant families of non-relatively free sections with sufficiently large height. Let T1,,TrT_{1},\ldots,T_{r} denote all the families of rational anticanonical conics on 𝒳η\mathcal{X}_{\eta} which are defined over the ground field and let β1,,βrN1(𝒳η)\beta_{1},\ldots,\beta_{r}\in N_{1}(\mathcal{X}_{\eta}) denote their numerical classes (which may coincide). We claim that there is some bounded subset 𝒮N1(𝒳η)\mathcal{S}\subset N_{1}(\mathcal{X}_{\eta}) such that the ψ\psi-image of a class α\alpha of any dominant but not relatively free family is contained in 𝒮+mβj\mathcal{S}+m\beta_{j} for some index jj and some non-negative integer mm. This is an immediate consequence of Theorem 6.6 (3) which shows that any such class α\alpha is the sum of the class of a section of bounded height with some multiple of the class of a π\pi-vertical conic.

We are now ready to analyze the contributions of such families to the counting function. First, suppose that ρ(𝒳η)>1\rho(\mathcal{X}_{\eta})>1. As demonstrated by Corollary 9.3 there is an upper bound RR on the number of components of dominant families of sections that are not relatively free which represent any fixed numerical class. Furthermore, Lemma 6.5 proves there is a constant m(𝒳/B)m(\mathcal{X}/B) such that dim(M)K𝒳/BC+22g(B)+m(𝒳/B)\dim(M)\leq-K_{\mathcal{X}/B}\cdot C+2-2g(B)+m(\mathcal{X}/B) for all such components MM. Thus, the contribution of all the dominant non-relatively-free families contained in Ξ\Xi to the counting function is bounded above by

i=1dR|𝒮|rqi+s\sum_{i=1}^{d}R\cdot|\mathcal{S}|\cdot r\cdot q^{i+s}

for some constant ss. Since we are assuming that ρ(𝒳η)>1\rho(\mathcal{X}_{\eta})>1, this contribution to the counting function is asymptotically negligible compared to the growth rate as in Remark 10.8. Second, suppose that ρ(𝒳η)=1\rho(\mathcal{X}_{\eta})=1. As explained in Case 1, in this situation the rational curves on surfaces swept out by fiberwise conics must be accumulating components.

Case 3: Consider the dominant families of relatively free sections with sufficiently large height. In order to count the contributions of such components, our plan is to translate into a sum over lattice points in N(𝒳η)N(\mathcal{X}_{\eta}).

We first claim there is some class βN1(𝒳η)\beta\in N_{1}(\mathcal{X}_{\eta}) such that every class α\alpha of a dominant family of sections in our coset satisfies ψ(α)β+Nef1(𝒳η)\psi(\alpha)\in\beta+\mathrm{Nef}_{1}(\mathcal{X}_{\eta}). Indeed, by Theorem 8.1 we see that every dominant family of sections of sufficiently large height is numerically equivalent to a sum of a π\pi-vertical free rational curve and a section of bounded height. Furthermore, if we take a π\pi-vertical free rational curve in a general fiber FF then its image under the map N1(F)N1(𝒳)N_{1}(F)\to N_{1}(\mathcal{X}) is contained in Nef1(𝒳η)\mathrm{Nef}_{1}(\mathcal{X}_{\eta}). Thus we deduce that the ψ\psi-image of all dominant families of sections lies in a finite union of translates of Nef1(𝒳η)\mathrm{Nef}_{1}(\mathcal{X}_{\eta}), proving the claim.

We now use ψ\psi to translate the sum over to N1(𝒳η)N_{1}(\mathcal{X}_{\eta})_{\mathbb{Z}}. Let bb be the relative anticanonical degree of the class β\beta and let cc denote the constant which is the difference in relative anticanonical degrees between any numerical class in Ξ\Xi and its image under ψ\psi. By definition every component MM of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) that generically parametrizes relatively free sections has the expected dimension. Furthermore, Theorem 9.2 gives a polynomial upper bound P(d)P(d) on the number of components representing Sec(𝒳/B)d\mathrm{Sec}(\mathcal{X}/B)_{d}. Altogether we see that the contribution of the relatively free sections to the counting function is bounded above by

αNef1(𝒳η)K𝒳/BαdbcP(K𝒳/Bα+b+c)qK𝒳/Bα+b+c+22g(B).\sum_{\begin{subarray}{c}\alpha\in\mathrm{Nef}_{1}(\mathcal{X}_{\eta})_{\mathbb{Z}}\\ -K_{\mathcal{X}/B}\cdot\alpha\leq d-b-c\end{subarray}}P(-K_{\mathcal{X}/B}\cdot\alpha+b+c)q^{-K_{\mathcal{X}/B}\cdot\alpha+b+c+2-2g(B)}.

Using standard lattice counting techniques this shows the desired result. ∎

If we assume Conjecture 10.3 then we can compute explicitly the contributions of relatively free families. By summing up over all cosets as in the proof of [LT19a, Theorem 9.10], we obtain the following:

Theorem 10.10.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that 𝒳\mathcal{X} is smooth, K𝒳/B-K_{\mathcal{X}/B} is relatively ample, and the general fiber is a del Pezzo surface of degree 2\geq 2 that is not 2\mathbb{P}^{2} or 1×1\mathbb{P}^{1}\times\mathbb{P}^{1}. Assume that Conjecture 10.3 holds. Then

N(𝒳,K𝒳/B,q,d)d(τXα(𝒳η,K𝒳/B)|Br(𝒳)|qq1)qddρ(𝒳η)1.N(\mathcal{X},-K_{\mathcal{X}/B},q,d)\mathrel{\mathop{\sim}_{d\to\infty}}\left(\tau_{X}\cdot\alpha(\mathcal{X}_{\eta},-K_{\mathcal{X}/B})\cdot|\mathrm{Br}(\mathcal{X})|\cdot\frac{q}{q-1}\right)q^{d}d^{\rho(\mathcal{X}_{\eta})-1}.

Here the α\alpha-constant of 𝒳η\mathcal{X}_{\eta} is defined by

α(𝒳η,K𝒳/B):=dimN1(𝒳η)μ(Nef1(𝒳η){γN1(𝒳η)|K𝒳ηγ1})\alpha(\mathcal{X}_{\eta},-K_{\mathcal{X}/B}):=\dim N_{1}(\mathcal{X}_{\eta})\cdot\mu(\mathrm{Nef}_{1}(\mathcal{X}_{\eta})\cap\{\gamma\in N_{1}(\mathcal{X}_{\eta})\,|-K_{\mathcal{X}_{\eta}}\cdot\gamma\leq 1\})

where the volume is computed with respect to the lattice structure N1(𝒳η)N_{1}(\mathcal{X}_{\eta})_{\mathbb{Z}} and the τ\tau-constant of 𝒳\mathcal{X} is defined by

τ𝒳=|Λ|[N1(𝒳)N1(𝒳η):N1(𝒳η)]\tau_{\mathcal{X}}=|\Lambda|\cdot[N_{1}(\mathcal{X})_{\mathbb{Z}}\cap N_{1}(\mathcal{X}_{\eta}):N_{1}(\mathcal{X}_{\eta})_{\mathbb{Z}}]

where Λ\Lambda denotes the set of allowable intersection profiles for 𝒳\mathcal{X}.

11. Geometric Manin’s Conjecture for certain families

In this section we prove Geometric Manin’s Conjecture for certain special types of del Pezzo fibrations.

11.1. Singularities of fibers

Suppose that SS is a (normal) del Pezzo surface with canonical singularities over an algebraically closed field of characteristic 0. [HW81] shows that the minimal resolution of SS is a weak del Pezzo surface.

Definition 11.1.

Let SS be a del Pezzo surface with canonical singularities. We say that a line bundle LL on SS defines a system of lines if it satisfies KSL=3-K_{S}\cdot L=3 and L2=1L^{2}=1.

The terminology is motivated by the following description of such LL.

Lemma 11.2.

Let SS be a del Pezzo surface with canonical singularities and let LL define a system of lines on SS. Then LL is the pullback of 𝒪(1)\mathcal{O}(1) under a birational morphism to 2\mathbb{P}^{2}.

Proof.

Let ϕ:SS\phi:S^{\prime}\to S be a minimal resolution so that SS^{\prime} is a weak del Pezzo surface. We have h0(S,L)=h0(S,ϕL)=3h^{0}(S,L)=h^{0}(S^{\prime},\phi^{*}L)=3 by Riemann-Roch. By [ADHL15, Proposition 5.2.2.4] we see that |ϕL||\phi^{*}L| is basepoint free. Thus the linear series defines a morphism to 2\mathbb{P}^{2} and since L2=1L^{2}=1 this morphism must be birational. We claim that |L||L| is also basepoint free. Indeed, let ss be any point in SS and let ss^{\prime} denote a preimage in SS^{\prime}. We can find an irreducible rational curve in |ϕL||\phi^{*}L| that avoids ss^{\prime}. This divisor has vanishing intersection with every (2)(-2)-curve, so it cannot intersect any such curve. Thus this divisor avoids the entire fiber over ss. In this way we see that LL defines a birational morphism to 2\mathbb{P}^{2}. ∎

Corollary 11.3.

Let SS be a del Pezzo surface with canonical singularities and let LL denote a system of lines on SS. Fix a general point ss and let |L|s|L||L|_{s}\subset|L| denote the sublinear series of divisors through ss. Then the general member of |L|s|L|_{s} is a smooth rational curve which avoids Sing(S)\mathrm{Sing}(S). Any divisor parametrized by |L|s|L|_{s} which avoids Sing(S)\mathrm{Sing}(S) will be one of the following:

  1. (1)

    a smooth anticanonical cubic,

  2. (2)

    a (1)(-1)-curve and a smooth anticanonical conic meeting transversally, or

  3. (3)

    a chain of three (1)(-1)-curves meeting transversally.

Proof.

The first statement follows from the fact that |L||L| defines a birational morphism ψ:S2\psi:S\to\mathbb{P}^{2}. We still must classify the possible types of divisors D|L|sD\in|L|_{s} which avoid Sing(S)\mathrm{Sing}(S). Note that every component will be a (1)(-1)-curve, an anticanonical conic, or an anticanonical cubic. Since DD avoids Sing(S)\mathrm{Sing}(S), the image of DD in 2\mathbb{P}^{2} is a line such that there are at most 22 ψ\psi-exceptional centers along DD. The three cases in the theorem occur when DD meets 0, 11, or 22 of these points. ∎

11.2. Global systems of lines

We now globalize our discussion from the previous section.

Definition 11.4.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. We say that π\pi admits a global system of lines if:

  1. (1)

    Every fiber of π\pi is a normal del Pezzo surface with canonical singularities.

  2. (2)

    There is a line bundle \mathcal{L} on 𝒳\mathcal{X} such that for every fiber FF of π\pi the restriction |F\mathcal{L}|_{F} is a system of lines.

[Ish82] constructs a coarse moduli space parametrizing families of smooth del Pezzo surfaces which admit a global system of lines. By [Ish82, Theorem 3] this space can be compactified by allowing the surfaces to acquire A1A_{1}-singularities on the boundary. Thus there are many del Pezzo fibrations satisfying the conditions of Definition 11.4.

Suppose that π:𝒳B\pi:\mathcal{X}\to B is a del Pezzo fibration such that every fiber is a del Pezzo surface with canonical singularities. If 𝒳\mathcal{X} admits a line bundle \mathcal{L} as in Definition 11.4 (2) then the restriction |𝒳η\mathcal{L}|_{\mathcal{X}_{\eta}} defines a system of lines on the generic fiber that is defined over the ground field. Conversely, suppose that 𝒳η\mathcal{X}_{\eta} admits a birational morphism over k(B)k(B) to projective space. By taking the closure of an element of this linear system in 𝒳\mathcal{X}, we obtain a Weil divisor 𝒟\mathcal{D} on 𝒳\mathcal{X} whose restriction to a general fiber is a system of lines. This is not quite enough to verify Definition 11.4, since 𝒟\mathcal{D} might not be Cartier. If 𝒳\mathcal{X} is \mathbb{Q}-factorial, then since it is terminal Gorenstein [Kaw88, Lemma 5.1] implies every divisor on 𝒳\mathcal{X} is Cartier. In summary:

Lemma 11.5.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that every fiber is a del Pezzo surface with canonical singularities. Suppose that 𝒳\mathcal{X} is \mathbb{Q}-factorial and that 𝒳η\mathcal{X}_{\eta} admits a birational morphism to k(B)2\mathbb{P}^{2}_{k(B)} over k(B)k(B). Then π\pi admits a global system of lines.

The key idea in this section is the following. Suppose that C1,C2C_{1},C_{2} are numerically equivalent sections on 𝒳\mathcal{X}. We would like to show that after adding some π\pi-vertical free curves to C1C_{1} and C2C_{2} we can obtain stable maps which lie in the same component of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}). Our strategy is to first find a well-behaved surface YY containing C1C_{1} and C2C_{2} and then to construct the desired stable maps inside of YY.

The first step is to identify this well-behaved surface YY.

Proposition 11.6.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration which admits a global system of lines \mathcal{L}. Suppose that M1,M2M_{1},M_{2} are components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which generically parametrize relatively free sections which contain 2g(B)+1\geq 2g(B)+1 general points of 𝒳\mathcal{X}. Then for general sections C1C_{1} parametrized by M1M_{1} and C2C_{2} parametrized by M2M_{2} there is a surface Y𝒳Y\subset\mathcal{X} satisfying the following properties.

  1. (1)

    YY contains C1C_{1} and C2C_{2}.

  2. (2)

    YY is contained in the smooth locus of 𝒳\mathcal{X} and its intersection with any fiber FF is contained in the smooth locus of FF.

  3. (3)

    The restriction of YY to any fiber FF of π\pi is a member of a system of lines on FF.

Proof.

Let ZZ denote the union of the singular loci of all singular fibers of π\pi (so in particular ZZ contains the singular locus of 𝒳\mathcal{X}). Note that ZZ has codimension 33 in 𝒳\mathcal{X}. Thus by Lemma 3.10 general choices of C1C_{1} and C2C_{2} will avoid ZZ.

Suppose we fix a singular fiber F0F_{0} and fix a general section C2C_{2}. In particular by Lemma 3.10 we may ensure that there are only finitely many divisors in the system of lines ||F0||\mathcal{L}|_{F_{0}}| which contain F0C2F_{0}\cap C_{2} and meet ZZ. As we take the union of these divisors as we vary over all fibers F0F_{0}, we obtain a codimension 22 subset WW of 𝒳\mathcal{X}. In particular, a general C1C_{1} will not intersect WW.

Consider the rational points on 𝒳η\mathcal{X}_{\eta} corresponding to the general C1,C2C_{1},C_{2} as described in the previous paragraph. There is a unique line in 𝒳η\mathcal{X}_{\eta} in the system of lines |𝒳η\mathcal{L}|_{\mathcal{X}_{\eta}} which contains these two points, and this line will be defined over the ground field. Let YY denote the corresponding surface in 𝒳\mathcal{X}. Then the restriction of YY to any fiber FF will be the unique element in the system of lines |F\mathcal{L}|_{F} connecting these two points. In particular this YY satisfies all the desired properties. ∎

The next lemma enables us to “connect” two sections of a fibration π:YB\pi:Y\to B of relative dimension 11.

Lemma 11.7.

Let YY be a smooth projective surface equipped with a morphism π:YB\pi:Y\to B whose general fiber is 1\mathbb{P}^{1}. Suppose that C1C_{1} and C2C_{2} are two sections of π\pi. Then there are stable maps f1:Z1Yf_{1}:Z_{1}\to Y and f2:Z2Yf_{2}:Z_{2}\to Y such that:

  1. (1)

    Both Z1Z_{1} and Z2Z_{2} consist of one genus g(B)g(B) curve attached to trees of rational curves.

  2. (2)

    The map fif_{i} maps the genus g(B)g(B) curve in ZiZ_{i} isomorphically to CiC_{i} and the trees of rational curves to π\pi-vertical curves.

  3. (3)

    Fix any point bBb\in B and let Z1,bZ_{1,b} denote the part of Z1Z_{1} whose support maps to the fiber FbF_{b} over bb. If FbF_{b} is reducible then f1Z1,b<Fbf_{1*}Z_{1,b}<F_{b}. We also have the analogous statement for f2f_{2}.

  4. (4)

    f1f_{1} and f2f_{2} lie in the same component of M¯g(B),0(Y)\overline{M}_{g(B),0}(Y).

Proof.

Choose any birational contraction ρ:Y𝔽\rho:Y\to\mathbb{F} where 𝔽\mathbb{F} is a ruled surface. There are π\pi-vertical effective curves T1,T2T_{1},T_{2} such that ρρC1=C1+T1\rho^{*}\rho_{*}C_{1}=C_{1}+T_{1} and ρρC2=C2+T2\rho^{*}\rho_{*}C_{2}=C_{2}+T_{2}. An easy induction on the relative Picard rank of ρ\rho shows that T1T_{1} is supported on reducible fibers and that the component of T1T_{1} supported on any fiber is less effective than that fiber. An analogous statement holds for T2T_{2}.

If we add on sufficiently many general fibers to ρC1\rho_{*}C_{1} and ρC2\rho_{*}C_{2} we can guarantee that the resulting curves are contained in the closure of the same component of Sec(𝔽/B)\mathrm{Sec}(\mathbb{F}/B) (see Proposition 4.9). Note that a general section in this component will miss the ρ\rho-exceptional centers, so that the strict transform will be the same as the pullback. Thus we see that ρρC1\rho^{*}\rho_{*}C_{1} and ρρC2\rho^{*}\rho_{*}C_{2} are algebraically equivalent and both lie in the closure of a single component of Sec(Y/B)\mathrm{Sec}(Y/B). By construction the portion of these 11-cycles supported on any reducible fiber FbF_{b} is less effective than the entire fiber.

Recall that Sec(Y/B)\mathrm{Sec}(Y/B) admits an embedding into M¯g(B),0(Y)\overline{M}_{g(B),0}(Y). By taking limits as the image curve approaches ρρC1\rho^{*}\rho_{*}C_{1} and ρρC2\rho^{*}\rho_{*}C_{2}, we obtain stable maps f1:Z1Yf_{1}:Z_{1}\to Y and f2:Z2Yf_{2}:Z_{2}\to Y whose corresponding cycles are ρρC1\rho^{*}\rho_{*}C_{1} and ρρC2\rho^{*}\rho_{*}C_{2}. These stable maps satisfy all the desired properties. ∎

Finally, we prove that we can “connect” two sections in a del Pezzo fibration with a global system of lines.

Lemma 11.8.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration that admits a global system of lines. Let M1,M2M_{1},M_{2} be components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which generically parametrize relatively free sections which can contain 2g(B)+1\geq 2g(B)+1 general points of 𝒳\mathcal{X}. Let C1,C2C_{1},C_{2} be general sections parametrized by M1,M2M_{1},M_{2} respectively. There are stable maps f1:Z1𝒳f_{1}:Z_{1}\to\mathcal{X} and f2:Z2𝒳f_{2}:Z_{2}\to\mathcal{X} such that

  1. (1)

    the image of f1f_{1} and the image of f2f_{2} do not intersect the singular locus of 𝒳\mathcal{X} or the singular locus of any fiber FF,

  2. (2)

    both f1f_{1} and f2f_{2} are smooth points of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}),

  3. (3)

    the domain of f1f_{1} is a comb which maps the handle to C1C_{1} and the teeth to π\pi-vertical free curves, and similarly for f2f_{2}, and

  4. (4)

    f1f_{1} and f2f_{2} lie in the same component of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}).

Proof.

Using Proposition 11.6 we obtain a surface YY containing both C1C_{1} and C2C_{2}. Note that YY is contained in smooth locus of 𝒳\mathcal{X} and does not intersect the singular locus of any fiber of π\pi. Furthermore, the restriction of YY to any fiber yields a system of lines. Let YY^{\prime} denote a minimal resolution of YY. By Corollary 11.3 the singular fibers of the map YBY\to B consist of a chain of two or three rational curves meeting transversally. Thus YY has only AnA_{n} singularities. This means that every fiber of YBY^{\prime}\to B is a chain of rational curves. Furthermore, the two curves on the end of this chain are not contracted by the birational map to YY.

Apply Lemma 11.7 to the strict transforms of C1C_{1} and C2C_{2} on YY^{\prime} to find stable maps f1f^{\prime}_{1} and f2f^{\prime}_{2} and let f~1,f~2\widetilde{f}_{1},\widetilde{f}_{2} be the corresponding stable maps to 𝒳\mathcal{X}. We claim that f~1\widetilde{f}_{1} and f~2\widetilde{f}_{2} represent smooth points of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}). Indeed, by combining Lemma 11.7 (3) with the explicit description of the fibers of YBY^{\prime}\to B as chains of rational curves we see that the part of the image of f~1\widetilde{f}_{1} supported on any fiber of YBY\to B is less effective than the fiber itself, and the same is true of f~2\widetilde{f}_{2}. The classification of Corollary 11.3 yields the following possibilities for the vertical components of f~1,f~2\widetilde{f}_{1},\widetilde{f}_{2} contained in a fiber: a smooth anticanonical cubic, a smooth anticanonical conic, a (1)(-1)-curve, or a union of two (1)(-1)-curves meeting transversally. Furthermore, since the locus of intersection points of (1)(-1)-curves in fibers has codimension 22 in 𝒳\mathcal{X} a general section in our families will avoid it. Thus in each of these cases f~1,f~2\widetilde{f}_{1},\widetilde{f}_{2} are local immersions near the neighborhood of any node and [GHS03, Lemma 2.6] applies to show the smoothness of the stable map.

The last step is to improve the properties of f~1\widetilde{f}_{1} and f~2\widetilde{f}_{2}. Consider the part of the image of f~1\widetilde{f}_{1} that is supported in a given fiber F0F_{0}. We know that it is contained in the smooth locus of F0F_{0}. In fact, since F0F_{0} admits a system of lines there are many very free curves contained in the smooth locus of F0F_{0}. By successively gluing on general very free curves in the smooth locus of F0F_{0} to the various components of f~1\widetilde{f}_{1}, we obtain another stable map f^1\widehat{f}_{1} such that the components in F0F_{0} can be smoothed to a free curve while keeping the intersection point with the section fixed (see [Kol96, II.7.9 Theorem]). We simultaneously glue members of these families of vertical free curves to general points of f~2\widetilde{f}_{2} to get f^2\widehat{f}_{2}. Since the original stable maps were smooth points of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) which lie in the same component, we can ensure that f^1\widehat{f}_{1} and f^2\widehat{f}_{2} will again be smooth points of M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) which lie in the same component. We then replace f~2\widetilde{f}_{2} by f^2\widehat{f}_{2} and f~1\widetilde{f}_{1} by a deformation of f^1\widehat{f}_{1} which smooths the part supported in F0F_{0}. Repeating this process several times we obtain the desired statement. ∎

11.3. Geometric Manin’s Conjecture for del Pezzo fibrations with global systems of lines

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration. We start by discussing a monoid action on the set of relatively free sections which comes from Movable Bend-and-Break.

Fix a general fiber FF of π\pi and let \mathcal{R} denote the set of components of M¯0,0(F)\overline{M}_{0,0}(F) which generically parametrize birational maps onto free rational curves. If FF is a del Pezzo surface of degree 2\geq 2 then [Tes09, Theorem 5.1] combined with [LT19a, Lemma 2.13] shows that every class in Nef1(F)\mathrm{Nef}_{1}(F)_{\mathbb{Z}} is represented by at most one element of \mathcal{R}. Furthermore, two free curves on FF are guaranteed to intersect unless they are both fibers of the same map to 1\mathbb{P}^{1}. With this one exception, if we choose two components of \mathcal{R} then by gluing and smoothing general curves in this component we obtain a unique component of \mathcal{R}. To handle the exception, for each family RR of anticanonical conics with square 0 and for each integer k2k\geq 2 we formally add the element kRkR to \mathcal{R} – conceptually, we think of these classes as “gluing curves from RR kk times”. With this addition and by formally adding in a 0 class which acts trivially the gluing operation gives \mathcal{R} the structure of a commutative monoid.

Let \mathcal{M} denote the set of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which generically parametrize relatively free sections with height MBBbound(𝒳)+2\geq\mathrm{MBBbound}(\mathcal{X})+2. By Theorem 8.6 the universal map over any component of \mathcal{M} has connected fibers. Thus if we choose any component in \mathcal{M} and any component of \mathcal{R} then by gluing and smoothing we obtain a unique new component of \mathcal{M}. Furthermore by [LT19b, Lemma 5.11] if we perform this operation twice with two different families in \mathcal{R} then the resulting component does not depend on which order we glue. In this way \mathcal{M} is given the structure of an \mathcal{R}-module.

Lemma 11.9.

There are finitely many components M1,,MsM_{1},\ldots,M_{s}\in\mathcal{M} such that every component of \mathcal{M} can be obtained by gluing π\pi-vertical free curves to some MiM_{i} and smoothing.

Proof.

Let MM be any component of \mathcal{M}. By Corollary 8.5 the closure of MM in M¯g(B),0(𝒳)\overline{M}_{g(B),0}(\mathcal{X}) contains a point representing the union of a relatively free section with a π\pi-vertical curve of anticanonical degree 22 or 33. By repeatedly breaking off such components, we see that we may define the MiM_{i} to be the finite set of components of \mathcal{M} which have anticanonical degree at least MBBbound(𝒳)+2\mathrm{MBBbound}(\mathcal{X})+2 and no more than MBBbound(𝒳)+5\mathrm{MBBbound}(\mathcal{X})+5. ∎

It will be useful to reinterpret this lemma using the monoid action. Let 𝒮\mathcal{S} denote the disjoint union of ss copies of \mathcal{R}. Define the map ξ:𝒮\xi:\mathcal{S}\to\mathcal{M} which sends a component RR in the jjth copy of \mathcal{R} to RMjR\cdot M_{j}. Then the lemma shows that this map is surjective.

We are now prepared to prove Geometric Manin’s Conjecture for certain types of families. Suppose that π:𝒳B\pi:\mathcal{X}\to B is a del Pezzo fibration which admits a global system of lines. Then the relative Picard rank of π\pi is ρ(𝒳η)\rho(\mathcal{X}_{\eta}). As in the discussion after Definition 10.7 there is a translate of N1(𝒳η)N1(𝒳)N_{1}(\mathcal{X}_{\eta})\subset N_{1}(\mathcal{X}) which contains all the classes of sections of π\pi; we denote this translate by NFN_{F}.

Theorem 11.10.

Let π:𝒳B\pi:\mathcal{X}\to B be a del Pezzo fibration such that:

  1. (1)

    𝒳η\mathcal{X}_{\eta} is a del Pezzo surface of degree 2\geq 2 such that ρ(𝒳η)\rho(\mathcal{X}_{\eta}) coincides with the geometric Picard rank of 𝒳η\mathcal{X}_{\eta}, and

  2. (2)

    π\pi admits a global system of lines.

There is a numerical class αNF\alpha\in N_{F} such that for any numerical class βα+Nef1(𝒳η)\beta\in\alpha+\mathrm{Nef}_{1}(\mathcal{X}_{\eta}) there is exactly one component of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which both represents β\beta and generically parametrizes relatively free sections.

Combined with Lemma 11.5 this proves Theorem 1.15.

Proof.

Let i:F𝒳i:F\to\mathcal{X} denote the inclusion of a general fiber. By our assumption on the monodromy action we see that 𝒳\mathcal{X} has Picard rank ρ(F)+1\rho(F)+1. Thus as demonstrated earlier every class in Nef1(𝒳η)N1(𝒳)\mathrm{Nef}_{1}(\mathcal{X}_{\eta})\subset N_{1}(\mathcal{X}) is represented by a unique family of free rational curves. In particular, by gluing such curves onto a relatively free section and smoothing we obtain the existence of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) representing numerical classes in a translation of Nef1(𝒳η)\mathrm{Nef}_{1}(\mathcal{X}_{\eta}), and it only remains to prove the uniqueness.

Let \mathcal{M} denote the set of components of Sec(𝒳/B)\mathrm{Sec}(\mathcal{X}/B) which generically parametrize relatively free sections with height MBBbound(𝒳)+2\geq\mathrm{MBBbound}(\mathcal{X})+2. Consider the map μ:N1(𝒳)\mu:\mathcal{M}\to N_{1}(\mathcal{X})_{\mathbb{Z}} which sends a component to its numerical class. We would like to show that for some class α\alpha as in the statement of the theorem the fibers of μ\mu over α+Nef1(𝒳η)\alpha+\mathrm{Nef}_{1}(\mathcal{X}_{\eta}) are singletons.

Let M1,,MsM_{1},\ldots,M_{s} be a finite set of components in \mathcal{M} as in Lemma 11.9 and let 𝒮\mathcal{S} denote the corresponding \mathcal{R}-module as defined above. We have a surjective map ξ:𝒮\xi:\mathcal{S}\to\mathcal{M}. Our strategy for understanding the fibers of μ\mu is to study the fibers of ξ\xi and μξ\mu\circ\xi and to prove that they are often the same.

The first step is to better understand the fibers of ξ\xi. Suppose we fix our attention on the iith copy of \mathcal{R} in 𝒮\mathcal{S}, so that the restriction of ξ\xi sends RRMiR\mapsto R\cdot M_{i}. Recall that there is a unique component of \mathcal{R} representing any class of Nef1(F)\mathrm{Nef}_{1}(F). Thus, the restrictions of both ξ\xi and μξ\mu\circ\xi to this subset of 𝒮\mathcal{S} are injective. Since 𝒮\mathcal{S} consists of ss copies of \mathcal{R}, we deduce that the fibers of ξ\xi and of μξ\mu\circ\xi have size at most ss.

We will use the following claim to show that these fibers often are as large as possible.

Claim 11.11.

Suppose that M,MM,M^{\prime}\in\mathcal{M}. Then there are elements R,RR,R^{\prime}\in\mathcal{R} such that

RM=RM.R\cdot M=R^{\prime}\cdot M^{\prime}.
Proof of claim:.

First, by adding on suitable elements of \mathcal{R} and smoothing we may assume that M,MM,M^{\prime} generically parametrize relatively free curves which can go through 2g(B)+1\geq 2g(B)+1 general points of 𝒳\mathcal{X}. (Note that if we prove our statement for these new components, the claim for the original components follows.) We then apply Lemma 11.8, which immediately implies the desired claim. ∎

We now apply the claim to all possible pairs of elements from M1,,MsM_{1},\ldots,M_{s}. In this way we obtain R1,,RsR_{1},\ldots,R_{s} in \mathcal{R} such that

R1M1=R2M2==RsMs.R_{1}\cdot M_{1}=R_{2}\cdot M_{2}=\ldots=R_{s}\cdot M_{s}.

Let MM^{\prime} be this common family in \mathcal{M} and let α\alpha be its numerical class. Then for any RR\in\mathcal{R} the fiber of ξ\xi over RMR\cdot M^{\prime} is as large as possible: it contains ss elements, one in each component of 𝒮\mathcal{S}. (Precisely, the iith copy of \mathcal{R} in 𝒮\mathcal{S} contributes the element RRiR\cdot R_{i} to this fiber.) This of course means that the fibers of μξ\mu\circ\xi over α+R\alpha+R also have the maximal size ss. These two statements together show that for any RR\in\mathcal{R} the map μ\mu is injective over the class α+R\alpha+R. Since the numerical class map from \mathcal{R} to Nef1(F)\mathrm{Nef}_{1}(F)_{\mathbb{Z}} is surjective, we have proved the desired statement. ∎

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