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A Smooth Shioda-Tate Isomorphism for Elliptically Fibered 4-Manifolds

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Abstract

This paper studies a subgroup of the mapping class group of an elliptically fibered 44-manifold π:M→Bπ: M\to B, inspired by number theory. The smooth Mordell-Weil group MW(π)\mathrm{MW}(π) is the group of isotopy classes of smooth sections of ππ. We construct a smooth analog of the Shioda-Tate isomorphism, identifying MW(π)\mathrm{MW(π)} with the quotient of H2(M;Z)H^2(M;\mathbb{Z}) by the trivial lattice of ππ. This shows that MW(π)\mathrm{MW}(π) can be computed explicitly from H2(M;Z)H^2(M;\mathbb{Z}). As an application, we show that the natural inclusion of the holomorphic Mordell-Weil group into the smooth one is an isomorphism if and only if MM is a rational elliptic surface. As another application, we show that MW(π)\mathrm{MW}(π) satisfies a strong version of Nielsen realization: any torsion element of MW(π)\mathrm{MW}(π) is represented by a holomorphic translation of MM of the same order.

Introduction

We start by giving our main theorem and then explain the objects involved in it. For an elliptic fibration π:M→B\pi:M\to B with fixed zero-section σ0\sigma_{0}, the smooth Mordell–Weil group is

MW⁡(π)=π0({smooth sections of π}).\operatorname{MW}(\pi)=\pi_{0}(\{\text{smooth sections of }\pi\}).

The following is a smooth analog of the classical Shioda–Tate isomorphism between the holomorphic Mordell–Weil group MW⁡hol(π)\operatorname{MW}^{\mathrm{hol}}(\pi) of an elliptic surface and the quotient of its Néron–Severi lattice by the trivial lattice ([SS19, Theorem 6.5]).

Theorem 1.1. Let π:M→B\pi:M\to B be an elliptic fibration over a closed base curve BB with fixed zero-section σ0:B→M\sigma_{0}:B\to M. Then there exists a natural group isomorphism

MW⁡(π)→≅H2(M;Z)/Triv⁡(π)\operatorname{MW}(\pi)\xrightarrow{\cong} H^{2}(M;\mathbb{Z})/\operatorname{Triv}(\pi)
[σ]↦[PD⁡M(σ(B))−PD⁡M(σ0(B))],[\sigma]\mapsto[\operatorname{PD}_{M}(\sigma(B))-\operatorname{PD}_{M}(\sigma_{0}(B))],

where σ(B)\sigma(B) is viewed as a homology class in H2(M;Z)H_{2}(M;\mathbb{Z}) and PD⁡M(σ(B))\operatorname{PD}_{M}(\sigma(B)) denotes its Poincaré dual.

We apply Theorem 1.1 in concrete examples below. One useful consequence is that for any elliptic surface over a closed base, H2(M):=H2(M;Z)H^{2}(M):=H^{2}(M;\mathbb{Z}) is generated by horizontal elements (elements corresponding to sections) and vertical elements (ones of the trivial lattice). As a key application of Theorem 1.1 and the Shioda–Tate isomorphism, we show the following corollary.

Corollary 1.2 (Characterizing rational elliptic surfaces). For an elliptic surface π:M→B\pi:M\to B over a closed base curve BB with holomorphic zero-section σ0\sigma_{0}, the groups MW⁡(π)\operatorname{MW}(\pi) and MW⁡hol(π)\operatorname{MW}^{\mathrm{hol}}(\pi) are isomorphic if and only if MM is rational.

Main Objects. We introduce the main objects of this paper. An elliptic fibration is a triple (M,B,π)(M, B, \pi), where MM is a smooth complex surface, BB is a smooth complex curve and π:M→B\pi: M \to B is a proper, surjective, holomorphic map whose general fiber is a smooth genus 1 curve. In this paper, we further assume that an elliptic fibration comes equipped with a smooth zero-section σ0:B→M\sigma_0 : B \to M, that π\pi has at least one critical point, and that π\pi is relatively minimal (i.e. no fiber contains a complex curve of self-intersection −1-1). The choice of zero-section equips each smooth fiber with a distinguished point, which gives it an abelian group structure. This group structure extends to the smooth locus of the singular fibers, as explained in § 2.2.

The Inose K3 surface

(a) The Inose K3 surface has MW⁡(π)≅Z4\operatorname{MW}(\pi) \cong\mathbb{Z}^{4}.

The Kummer K3 surface

(b) The Kummer K3 surface has MW⁡(π)≅Z4×Z/2Z×Z/2Z\operatorname{MW}(\pi) \cong\mathbb{Z}^{4} \times\mathbb{Z}/2\mathbb{Z} \times\mathbb{Z}/2\mathbb{Z}.

Figure 1. Two elliptic K3 surfaces with different Mordell–Weil groups. In both figures, the large sphere represents a section of π\pi. The smaller spheres and nodes are components of the singular fibers of the two fibrations. All fibers which are not depicted are smooth tori.

Let Γsm(π)\Gamma^{\mathrm{sm}}(\pi) denote the group of smooth sections of π:M→B\pi: M \to B, where sections are added pointwise and the identity is the distinguished section σ0\sigma_0. The (smooth) Mordell–Weil group of an elliptic fibration π:M→B\pi: M \to B is

MW⁡(π):=π0(Γsm(π)).\operatorname{MW}(\pi) := \pi_0\left(\Gamma^{\mathrm{sm}}(\pi)\right).

Replacing smooth sections by holomorphic sections of π\pi and stipulating that the zero-section is holomorphic yields the classical (holomorphic) Mordell–Weil group MW⁡hol(π)\operatorname{MW}^{\mathrm{hol}}(\pi). If the base BB is closed, both MW⁡(π)\operatorname{MW}(\pi) and MW⁡hol(π)\operatorname{MW}^{\mathrm{hol}}(\pi) are finitely generated abelian groups (see [4 Theorem 3.4] and [12 Theorem 6.6]).

The trivial lattice associated to an elliptic fibration π:M→B\pi: M \to B is the subgroup of H2(M)H^2(M) generated by the Poincaré duals of the zero-section and the irreducible components of all fibers of π\pi.

Using Theorem 1.1, we compute the Mordell–Weil group of two elliptic K3 surfaces. We fill in the details of these examples in § 5.3.

Example 1.3 (Mordell–Weil Group of Inose K3 Surface). Consider the Inose K3 surface with two singular fibers of type II∗II^* and four singular fibers of type I1I_1 as in Figure 1a. The Poincaré duals of irreducible components of the two fibers of type II∗II^* which do not intersect the zero-section, the fiber class and the zero-section generate the trivial lattice. By computing intersection numbers as in Example 5.6 in a later section, we show that the trivial lattice is unimodular and thus primitively embedded in H2(M)H^2(M). Using vanishing cycles and Lefschetz thimbles, we can give the remaining 4 generators of H2(M)H^2(M). Theorem 1.1 implies

MW⁡(π)≅Z4.\operatorname{MW}(\pi) \cong\mathbb{Z}^{4}.

Example 1.4 (Mordell–Weil Group of Kummer Surface). Let π:M→P1\pi: M \to\mathbb{P}^{1} be an elliptically fibered Kummer surface as in Figure 1b. It has 4 singular fibers of type I0∗I_0^*. The trivial lattice is generated by the Poincaré duals of the irreducible components of the singular fiber, the class of the generic fiber and the zero-section. In § 5.3, we give explicit generators for H2(M)H^2(M) and conclude using Theorem 1.1 that

MW⁡(π)≅Z4×Z/2Z×Z/2Z.\operatorname{MW}(\pi) \cong\mathbb{Z}^{4} \times\mathbb{Z}/2\mathbb{Z} \times\mathbb{Z}/2\mathbb{Z}.

The elliptic surfaces in Example 1.3 and Example 1.4 are both K3 surfaces and thus diffeomorphic, as shown by Kodaira. The two examples show that the Mordell–Weil group detects the difference between the two elliptic fibration structures.

Proof Strategy

The main idea in proving Theorem 1.1 is to give a cohomological characterization for MW⁡(π)\operatorname{MW}(\pi) in terms of sheaf cohomology, similarly to [4 Proposition 3.3] and [10 Proposition 3.7]. Such a characterization is made difficult by the possibility of a nontrivial component group of the relative smooth locus of reducible singular fibers, so we proceed by removing the singular fibers.

For an elliptic fibration π:M→B\pi:M\to B, let Σ⊂B\Sigma\subset B be the set of critical values of π\pi. For each t∈Σt\in\Sigma, consider a small open disk DtD_t around tt and assume that the disks DtD_t are pairwise disjoint. Define

B∘:=B−⋃t∈ΣDtB^\circ:= B-\bigcup_{t\in\Sigma}D_t

and the compact 4-manifold with boundary

M∘:=π−1(B∘).M^\circ:= \pi^{-1}(B^\circ).

Denote by π∘:M∘→B∘\pi^\circ:M^\circ\to B^\circ the restriction of π\pi (see Figure 2). Any section σ:B∘→M∘\sigma:B^\circ\to M^\circ naturally represents an element [σ]∈H2(M∘,∂M∘)[\sigma]\in H_2(M^\circ,\partial M^\circ).

An elliptic fibration and its reduced elliptic fibration

Figure 2. M∘M^\circ is obtained by removing an open neighborhood of each singular fiber of MM.

Step 1. Construct an isomorphism between MW⁡(π∘)\operatorname{MW}(\pi^\circ), the group of isotopy classes of sections of π∘\pi^\circ, and the annihilator of the fiber class in H2(M∘)H^2(M^\circ). We first express MW⁡(π∘)\operatorname{MW}(\pi^\circ) in terms of sheaf cohomology (Proposition 3.1). Using a spectral sequence argument, similar to the one in [4] and [10], we construct the desired isomorphism (Proposition 3.2).

Step 2. Relate the groups MW⁡(π)\operatorname{MW}(\pi) and MW⁡(π∘)\operatorname{MW}(\pi^\circ). For t∈Bt\in B, let Mt:=π−1(t)M_t:=\pi^{-1}(t). We construct a map Ψ:MW⁡(π∘)→⨁t∈ΣH1(Mt)\Psi:\operatorname{MW}(\pi^\circ)\to\bigoplus_{t\in\Sigma}H_1(M_t), which can be described geometrically as in § 5.1. The following theorem shows that Ψ\Psi is the only obstruction to extending sections of π∘\pi^\circ to sections of π\pi up to isotopy.

Theorem 1.5 (Relation between MW⁡(π)\operatorname{MW}(\pi) and MW⁡(π∘)\operatorname{MW}(\pi^\circ)). For any elliptic fibration π:M→B\pi: M \to B over a closed base, there exists the following short exact sequence of groups:

0→MW⁡(π)→MW⁡(π∘)→Ψ⨁t∈ΣH1(Mt)→0.0 \to\operatorname{MW}(\pi) \to\operatorname{MW}(\pi^\circ) \xrightarrow{\Psi} \bigoplus_{t\in\Sigma} H_1(M_t) \to0.

Step 3. Conclusion Using Step 1, we show that the kernel of Ψ\Psi is isomorphic to H2(M)/Triv⁡(π)H^2(M)/\operatorname{Triv}(\pi), which by Step 2 proves Theorem 1.1.

MW(π\pi) as a Subgroup of the Mapping Class Group

The Mordell–Weil group can be rephrased in terms of diffeomorphisms as

MW⁡(π)=π0({f∈Diff⁡(M)∣f acts on each smooth fiber by translation}).\operatorname{MW}(\pi)=\pi_0(\{f\in\operatorname{Diff}(M)\mid f\text{ acts on each smooth fiber by translation}\}).

Indeed, a diffeomorphism f∈Diff⁡(M)f\in\operatorname{Diff}(M) that acts by translation on each smooth fiber determines a smooth section f∘σ0f\circ\sigma_0 of π\pi. Conversely, any smooth section σ\sigma determines a unique diffeomorphism fσ∈Diff⁡(M)f_\sigma\in\operatorname{Diff}(M), that acts by translation by σ\sigma on the smooth locus of MM (see [10 Lemma 3.1]).

A consequence of Theorem 1.1 is that MW⁡(π)\operatorname{MW}(\pi) acts faithfully on H2(M)H^2(M). This action factors as

MW⁡(π)→π0(Diff⁡(M))→Aut⁡(H2(M),⌣)\operatorname{MW}(\pi)\to\pi_0(\operatorname{Diff}(M))\to\operatorname{Aut}(H^2(M),\smile)

and injectivity of the composition implies that the map MW⁡(π)→π0(Diff⁡(M))\operatorname{MW}(\pi)\to\pi_0(\operatorname{Diff}(M)) is injective.

A strong version of Nielsen realization holds for Mordell–Weil elements: every torsion element of the Mordell–Weil group has a holomorphic representative that is torsion.

Theorem 1.6 (Nielsen realization). If π:M→B\pi: M \to B is an elliptic fibration over a closed base curve BB with a holomorphic zero-section σ0\sigma_0, then the natural inclusion MW⁡hol(π)↪MW⁡(π)\operatorname{MW}^{\mathrm{hol}}(\pi)\hookrightarrow\operatorname{MW}(\pi) induces an isomorphism of the torsion subgroups of these finitely generated abelian groups.

Theorem 1.6 provides a practical method for computing MW⁡(π)\operatorname{MW}(\pi). Let gg be the genus of BB. Compute the number of additive and multiplicative singular fibers of π\pi, denoted aa and mm. [10 Corollary 1.4] implies that the rank of MW⁡(π)\operatorname{MW}(\pi) is 4g+2a+m−44g+2a+m-4. Then determine the torsion part using classical methods.

Related Work

This paper extends previous work of the author [10]. The previous paper computed the narrow Mordell–Weil group, a finite-index subgroup of MW⁡(π)\operatorname{MW}(\pi) of an elliptic fibration. The smooth Mordell–Weil group was first introduced by Farb and Looijenga [4]. They proved finite generation and computed the smooth Mordell–Weil group of a generic (i.e. assuming that all fibers are nodal) elliptic fibration π:M→P1\pi: M \to\mathbb{P}^1. A symplectic version of the Mordell–Weil group under the assumption that all singular fibers are nodal was computed by Hacking-Keating [6]. Related ideas were used by Cox and Zucker [3], who used an injection of the tensor of holomorphic Mordell–Weil group with Q\mathbb{Q} into H1(B,R1π∗Q)H^1(B,R^1\pi_*\mathbb{Q}) for computations.

Outline

In Section 2, we collect some background on elliptic surfaces that is used throughout the paper. In Section 3, we give a cohomological characterization for MW⁡(π∘)\operatorname{MW}(\pi^\circ) and express this group as the annihilator of the fiber class. Section 4 contains an extensive analysis of an elliptic fibration over a disk with only one singular fiber at the origin, with explicit computations of MW⁡(π)\operatorname{MW}(\pi) and MW⁡(π∘)\operatorname{MW}(\pi^\circ). Section 5.1 establishes a complete obstruction to extending isotopy classes of sections of π∘\pi^\circ to isotopy classes of sections of π\pi up to isotopy. In Section 5.2, we prove Theorem 1.1. In Section 5.3, we apply Theorem 1.1 in some concrete examples.

Computational Resource Disclosure. Gemini Pro 3.1 and Claude Opus 5.5 were used in the creation of pictures. GPT-5.6 Terra was involved in checking the proofs and literature search. The only mathematical use of artificial intelligence in this paper was in Example 5.6, which was computed in conversation with GPT-6.1 Sol.

Acknowledgements. I am very grateful to my advisor Benson Farb for suggesting this project, for his constant support, and for extensive comments on earlier drafts. I am thankful to Eduard Looijenga for many useful discussions. I would like to thank Eduard Looijenga, Dan Margalit and Katherine Booth for helpful comments.

Background on Elliptic Surfaces

We record the background which is necessary for the paper.

Notation and Conventions: For an elliptic fibration π:M→B\pi: M \to B, and b∈Bb \in B, we denote Mt:=π−1(t)M_t := \pi^{-1}(t). All (co)homology is taken with Z\mathbb{Z}-coefficients, unless otherwise specified. For any closed nn-manifold XX, we denote by PD⁡X:Hk(X)→Hn−k(X)\operatorname{PD}_X : H_k(X) \to H^{n-k}(X) the Poincaré duality isomorphism in XX. For a compact nn-manifold XX with boundary, we denote by PD⁡[X,∂X]:Hk(X)→Hn−k(X,∂X)\operatorname{PD}_{[X,\partial X]} : H^k(X) \to H_{n-k}(X,\partial X) and PD⁡[X,∂X]:Hk(X,∂X)→Hn−k(X)\operatorname{PD}_{[X,\partial X]} : H^k(X,\partial X) \to H_{n-k}(X) the isomorphisms given by Poincaré–Lefschetz duality. We assume that the zero-section σ0\sigma_0 is holomorphic in a neighborhood of each critical value1^{1}. The topology on Diff⁡(M)\operatorname{Diff}(M) and Γsm(π)\Gamma^{\mathrm{sm}}(\pi) is the Whitney C∞C^\infty topology.

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