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 π : M → B with fixed zero-section σ 0 \sigma_{0} σ 0 , the smooth Mordell–Weil group is
MW ( π ) = π 0 ( { smooth sections of π } ) . \operatorname{MW}(\pi)=\pi_{0}(\{\text{smooth sections of }\pi\}). MW ( π ) = π 0 ({ smooth sections of π }) .
The following is a smooth analog of the classical Shioda–Tate isomorphism between the holomorphic Mordell–Weil group MW h o l ( π ) \operatorname{MW}^{\mathrm{hol}}(\pi) MW hol ( π ) 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 π : M → B be an elliptic fibration over a closed base curve B B B with fixed zero-section σ 0 : B → M \sigma_{0}:B\to M σ 0 : B → M . Then there exists a natural group isomorphism
MW ( π ) → ≅ H 2 ( M ; Z ) / Triv ( π ) \operatorname{MW}(\pi)\xrightarrow{\cong} H^{2}(M;\mathbb{Z})/\operatorname{Triv}(\pi) MW ( π ) ≅ H 2 ( M ; Z ) / Triv ( π ) [ σ ] ↦ [ PD M ( σ ( B ) ) − PD M ( σ 0 ( B ) ) ] , [\sigma]\mapsto[\operatorname{PD}_{M}(\sigma(B))-\operatorname{PD}_{M}(\sigma_{0}(B))], [ σ ] ↦ [ PD M ( σ ( B )) − PD M ( σ 0 ( B ))] , where σ ( B ) \sigma(B) σ ( B ) is viewed as a homology class in H 2 ( M ; Z ) H_{2}(M;\mathbb{Z}) H 2 ( M ; Z ) and PD M ( σ ( B ) ) \operatorname{PD}_{M}(\sigma(B)) PD M ( σ ( 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, H 2 ( M ) : = H 2 ( M ; Z ) H^{2}(M):=H^{2}(M;\mathbb{Z}) H 2 ( M ) := H 2 ( M ; 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 π : M → B over a closed base curve B B B with holomorphic zero-section σ 0 \sigma_{0} σ 0 , the groups MW ( π ) \operatorname{MW}(\pi) MW ( π ) and MW h o l ( π ) \operatorname{MW}^{\mathrm{hol}}(\pi) MW hol ( π ) are isomorphic if and only if M M M is rational.
Main Objects. We introduce the main objects of this paper. An elliptic fibration is a triple ( M , B , π ) (M, B, \pi) ( M , B , π ) , where M M M is a smooth complex surface, B B B is a smooth complex curve and π : M → B \pi: M \to B π : M → 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 σ 0 : B → M \sigma_0 : B \to M σ 0 : B → M , that π \pi π has at least one critical point, and that π \pi π is relatively minimal (i.e. no fiber contains a complex curve of self-intersection − 1 -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 .
(a) The Inose K3 surface has MW ( π ) ≅ Z 4 \operatorname{MW}(\pi) \cong\mathbb{Z}^{4} MW ( π ) ≅ Z 4 .
(b) The Kummer K3 surface has MW ( π ) ≅ Z 4 × Z / 2 Z × Z / 2 Z \operatorname{MW}(\pi) \cong\mathbb{Z}^{4} \times\mathbb{Z}/2\mathbb{Z} \times\mathbb{Z}/2\mathbb{Z} MW ( π ) ≅ Z 4 × Z /2 Z × Z /2 Z .
Figure 1. Two elliptic K3 surfaces with different Mordell–Weil groups. In both figures, the large sphere represents a section of π \pi π . 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 Γ s m ( π ) \Gamma^{\mathrm{sm}}(\pi) Γ sm ( π ) denote the group of smooth sections of π : M → B \pi: M \to B π : M → B , where sections are added pointwise and the identity is the distinguished section σ 0 \sigma_0 σ 0 . The (smooth) Mordell–Weil group of an elliptic fibration π : M → B \pi: M \to B π : M → B is
MW ( π ) : = π 0 ( Γ s m ( π ) ) . \operatorname{MW}(\pi) := \pi_0\left(\Gamma^{\mathrm{sm}}(\pi)\right). MW ( π ) := π 0 ( Γ sm ( π ) ) .
Replacing smooth sections by holomorphic sections of π \pi π and stipulating that the zero-section is holomorphic yields the classical (holomorphic) Mordell–Weil group MW h o l ( π ) \operatorname{MW}^{\mathrm{hol}}(\pi) MW hol ( π ) . If the base B B B is closed, both MW ( π ) \operatorname{MW}(\pi) MW ( π ) and MW h o l ( π ) \operatorname{MW}^{\mathrm{hol}}(\pi) MW hol ( π ) 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 π : M → B is the subgroup of H 2 ( M ) H^2(M) H 2 ( M ) generated by the Poincaré duals of the zero-section and the irreducible components of all fibers of π \pi π .
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 I I ∗ II^* I I ∗ and four singular fibers of type I 1 I_1 I 1 as in Figure 1a . The Poincaré duals of irreducible components of the two fibers of type I I ∗ II^* I I ∗ 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 H 2 ( M ) H^2(M) H 2 ( M ) . Using vanishing cycles and Lefschetz thimbles, we can give the remaining 4 generators of H 2 ( M ) H^2(M) H 2 ( M ) . Theorem 1.1 implies
MW ( π ) ≅ Z 4 . \operatorname{MW}(\pi) \cong\mathbb{Z}^{4}. MW ( π ) ≅ Z 4 .
Example 1.4 (Mordell–Weil Group of Kummer Surface). Let π : M → P 1 \pi: M \to\mathbb{P}^{1} π : M → P 1 be an elliptically fibered Kummer surface as in Figure 1b . It has 4 singular fibers of type I 0 ∗ I_0^* 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 H 2 ( M ) H^2(M) H 2 ( M ) and conclude using Theorem 1.1 that
MW ( π ) ≅ Z 4 × Z / 2 Z × Z / 2 Z . \operatorname{MW}(\pi) \cong\mathbb{Z}^{4} \times\mathbb{Z}/2\mathbb{Z} \times\mathbb{Z}/2\mathbb{Z}. MW ( π ) ≅ Z 4 × Z /2 Z × Z /2 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) MW ( π ) 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 π : M → B , let Σ ⊂ B \Sigma\subset B Σ ⊂ B be the set of critical values of π \pi π . For each t ∈ Σ t\in\Sigma t ∈ Σ , consider a small open disk D t D_t D t around t t t and assume that the disks D t D_t D t are pairwise disjoint. Define
B ∘ : = B − ⋃ t ∈ Σ D t B^\circ:= B-\bigcup_{t\in\Sigma}D_t B ∘ := B − t ∈ Σ ⋃ D t
and the compact 4-manifold with boundary
M ∘ : = π − 1 ( B ∘ ) . M^\circ:= \pi^{-1}(B^\circ). M ∘ := π − 1 ( B ∘ ) .
Denote by π ∘ : M ∘ → B ∘ \pi^\circ:M^\circ\to B^\circ π ∘ : M ∘ → B ∘ the restriction of π \pi π (see Figure 2 ). Any section σ : B ∘ → M ∘ \sigma:B^\circ\to M^\circ σ : B ∘ → M ∘ naturally represents an element [ σ ] ∈ H 2 ( M ∘ , ∂ M ∘ ) [\sigma]\in H_2(M^\circ,\partial M^\circ) [ σ ] ∈ H 2 ( M ∘ , ∂ M ∘ ) .
Figure 2. M ∘ M^\circ M ∘ is obtained by removing an open neighborhood of each singular fiber of M M M .
Step 1. Construct an isomorphism between MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) , the group of isotopy classes of sections of π ∘ \pi^\circ π ∘ , and the annihilator of the fiber class in H 2 ( M ∘ ) H^2(M^\circ) H 2 ( M ∘ ) . We first express MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) 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) MW ( π ) and MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) . For t ∈ B t\in B t ∈ B , let M t : = π − 1 ( t ) M_t:=\pi^{-1}(t) M t := π − 1 ( t ) . We construct a map Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \Psi:\operatorname{MW}(\pi^\circ)\to\bigoplus_{t\in\Sigma}H_1(M_t) Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) , which can be described geometrically as in § 5.1 . The following theorem shows that Ψ \Psi Ψ is the only obstruction to extending sections of π ∘ \pi^\circ π ∘ to sections of π \pi π up to isotopy.
Theorem 1.5 (Relation between MW ( π ) \operatorname{MW}(\pi) MW ( π ) and MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) ). For any elliptic fibration π : M → B \pi: M \to B π : M → B over a closed base, there exists the following short exact sequence of groups:
0 → MW ( π ) → MW ( π ∘ ) → Ψ ⨁ t ∈ Σ H 1 ( M t ) → 0. 0 \to\operatorname{MW}(\pi) \to\operatorname{MW}(\pi^\circ) \xrightarrow{\Psi} \bigoplus_{t\in\Sigma} H_1(M_t) \to0. 0 → MW ( π ) → MW ( π ∘ ) Ψ t ∈ Σ ⨁ H 1 ( M t ) → 0.
Step 3. Conclusion Using Step 1, we show that the kernel of Ψ \Psi Ψ is isomorphic to H 2 ( M ) / Triv ( π ) H^2(M)/\operatorname{Triv}(\pi) H 2 ( M ) / Triv ( π ) , which by Step 2 proves Theorem 1.1.
MW(π \pi π ) as a Subgroup of the Mapping Class Group
The Mordell–Weil group can be rephrased in terms of diffeomorphisms as
MW ( π ) = π 0 ( { 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}\}). MW ( π ) = π 0 ({ f ∈ Diff ( M ) ∣ f acts on each smooth fiber by translation }) .
Indeed, a diffeomorphism f ∈ Diff ( M ) f\in\operatorname{Diff}(M) f ∈ Diff ( M ) that acts by translation on each smooth fiber determines a smooth section f ∘ σ 0 f\circ\sigma_0 f ∘ σ 0 of π \pi π . Conversely, any smooth section σ \sigma σ determines a unique diffeomorphism f σ ∈ Diff ( M ) f_\sigma\in\operatorname{Diff}(M) f σ ∈ Diff ( M ) , that acts by translation by σ \sigma σ on the smooth locus of M M M (see [10 Lemma 3.1] ).
A consequence of Theorem 1.1 is that MW ( π ) \operatorname{MW}(\pi) MW ( π ) acts faithfully on H 2 ( M ) H^2(M) H 2 ( M ) . This action factors as
MW ( π ) → π 0 ( Diff ( M ) ) → Aut ( H 2 ( M ) , ⌣ ) \operatorname{MW}(\pi)\to\pi_0(\operatorname{Diff}(M))\to\operatorname{Aut}(H^2(M),\smile) MW ( π ) → π 0 ( Diff ( M )) → Aut ( H 2 ( M ) , ⌣ )
and injectivity of the composition implies that the map MW ( π ) → π 0 ( Diff ( M ) ) \operatorname{MW}(\pi)\to\pi_0(\operatorname{Diff}(M)) MW ( π ) → π 0 ( 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 π : M → B is an elliptic fibration over a closed base curve B B B with a holomorphic zero-section σ 0 \sigma_0 σ 0 , then the natural inclusion MW h o l ( π ) ↪ MW ( π ) \operatorname{MW}^{\mathrm{hol}}(\pi)\hookrightarrow\operatorname{MW}(\pi) MW hol ( π ) ↪ MW ( π ) 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) MW ( π ) . Let g g g be the genus of B B B . Compute the number of additive and multiplicative singular fibers of π \pi π , denoted a a a and m m m . [10 Corollary 1.4] implies that the rank of MW ( π ) \operatorname{MW}(\pi) MW ( π ) is 4 g + 2 a + m − 4 4g+2a+m-4 4 g + 2 a + 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) MW ( π ) 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 → P 1 \pi: M \to\mathbb{P}^1 π : M → 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} Q into H 1 ( B , R 1 π ∗ Q ) H^1(B,R^1\pi_*\mathbb{Q}) H 1 ( B , R 1 π ∗ 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) MW ( π ∘ ) 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) MW ( π ) and MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) . Section 5.1 establishes a complete obstruction to extending isotopy classes of sections of π ∘ \pi^\circ π ∘ to isotopy classes of sections of π \pi π 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 π : M → B , and b ∈ B b \in B b ∈ B , we denote M t : = π − 1 ( t ) M_t := \pi^{-1}(t) M t := π − 1 ( t ) . All (co)homology is taken with Z \mathbb{Z} Z -coefficients, unless otherwise specified. For any closed n n n -manifold X X X , we denote by PD X : H k ( X ) → H n − k ( X ) \operatorname{PD}_X : H_k(X) \to H^{n-k}(X) PD X : H k ( X ) → H n − k ( X ) the Poincaré duality isomorphism in X X X . For a compact n n n -manifold X X X with boundary, we denote by PD [ X , ∂ X ] : H k ( X ) → H n − k ( X , ∂ X ) \operatorname{PD}_{[X,\partial X]} : H^k(X) \to H_{n-k}(X,\partial X) PD [ X , ∂ X ] : H k ( X ) → H n − k ( X , ∂ X ) and PD [ X , ∂ X ] : H k ( X , ∂ X ) → H n − k ( X ) \operatorname{PD}_{[X,\partial X]} : H^k(X,\partial X) \to H_{n-k}(X) PD [ X , ∂ X ] : H k ( X , ∂ X ) → H n − k ( X ) the isomorphisms given by Poincaré–Lefschetz duality. We assume that the zero-section σ 0 \sigma_0 σ 0 is holomorphic in a neighborhood of each critical value1 ^{1} 1 . The topology on Diff ( M ) \operatorname{Diff}(M) Diff ( M ) and Γ s m ( π ) \Gamma^{\mathrm{sm}}(\pi) Γ sm ( π ) is the Whitney C ∞ C^\infty C ∞ topology.
Proposition 2.1. If π : M → B \pi: M \to B π : M → B is an elliptic fibration over a closed base B B B , then π \pi π induces an isomorphism
π ∗ : H 1 ( M ) → ≅ H 1 ( B ) . \pi_* : H_1(M) \xrightarrow{\cong} H_1(B). π ∗ : H 1 ( M ) ≅ H 1 ( B ) .
Proof. We assume that an elliptic fibration is non-trivial and has a section. In particular, an elliptic fibration has no multiple fibers. Hence, [5 p. 157, Proposition 2.1] implies that π \pi π induces an isomorphism π ∗ : π 1 ( M ) → π 1 ( B ) \pi_* : \pi_1(M) \to\pi_1(B) π ∗ : π 1 ( M ) → π 1 ( B ) . Applying abelianization and the Hurewicz isomorphism on both sides yields the conclusion.
Proposition 2.2 ([7 Proposition 5.4] ). If π : M → D \pi: M \to D π : M → D is an elliptic fibration over a disk with only one critical value at the origin, then M M M strong deformation retracts to M 0 M_0 M 0 .
Monodromy and Kodaira’s Classification of Singular Fibers
Let π : M → B \pi: M \to B π : M → B be an elliptic surface with set of singular values Σ ⊂ B \Sigma\subset B Σ ⊂ B , and let M t M_t M t be a singular fiber. As a divisor, it can be written M t = ∑ m i C i M_t = \sum m_i C_i M t = ∑ m i C i , where C i C_i C i are the distinct irreducible components of M t M_t M t and m i ≥ 1 m_i \ge1 m i ≥ 1 is the multiplicity of the component C i C_i C i . The definition of a section gives π ∘ σ 0 = id B \pi\circ\sigma_0 = \operatorname{id}_B π ∘ σ 0 = id B and by the chain rule, d π σ 0 ( t ) ∘ d σ 0 ( t ) = id T b B d\pi_{\sigma_0(t)} \circ d\sigma_0(t) = \operatorname{id}_{T_bB} d π σ 0 ( t ) ∘ d σ 0 ( t ) = id T b B . Hence d π σ 0 ( t ) d\pi_{\sigma_0(t)} d π σ 0 ( t ) has full rank and σ 0 ( t ) \sigma_0(t) σ 0 ( t ) lies in a multiplicity-one component of M t M_t M t . In particular, there exists i i i such that m i = 1 . 2 m_i = 1.^2 m i = 1 . 2 To a reduced singular fiber M t M_t M t we associate a dual graph: a graph with vertices corresponding to C i C_i C i and C i ⋅ C j C_i \cdot C_j C i ⋅ C j edges connecting the vertices corresponding to C i C_i C i and C j C_j C j , if i ≠ j i \ne j i = j .
Let us fix a regular value b ∈ B b \in B b ∈ B and let
ρ : π 1 ( B − Σ , b ) → Mod ( M b ) \rho: \pi_1(B - \Sigma,b) \to\operatorname{Mod}(M_b) ρ : π 1 ( B − Σ , b ) → Mod ( M b )
be the monodromy representation of π \pi π . For a critical value t ∈ B t \in B t ∈ B , the monodromy around t t t is ρ ( [ γ ] ) ∈ Mod ( M b ) \rho([\gamma]) \in\operatorname{Mod}(M_b) ρ ([ γ ]) ∈ Mod ( M b ) , where γ \gamma γ is a loop based at b b b , containing only the critical value t t t . Choosing a basis for H 1 ( M b ) H_1(M_b) H 1 ( M b ) provides an identification Mod ( M b ) ≅ SL ( 2 , Z ) \operatorname{Mod}(M_b) \cong\operatorname{SL}(2,\mathbb{Z}) Mod ( M b ) ≅ SL ( 2 , Z ) .
The singular fibers of an elliptic surface were first classified by Kodaira [8 ] and later by Néron [11 ] and Tate [14 ] . Below, we give the classification of singular fibers from [9 Theorem I.6.6, Table VI.2.1] , excluding the possibility of multiple fibers.
Theorem 2.3 (Kodaira Classification). The dual graph of a reducible fiber of an elliptic surface is an extended Dynkin diagram of type ADE and the multiplicities of the irreducible components are as shown in Figure 3 . Furthermore, all fibers of an elliptic surface have one of the types in Table 1 .
Table 1. Kodaira’s classification of singular fibers of an elliptic surface.
Figure 3. Extended Dynkin Diagrams of type ADE with component multiplicities.
Consider a reducible singular fiber M t M_t M t with irreducible components C 0 , … , C r C_0,\ldots,C_r C 0 , … , C r , where C 0 C_0 C 0 intersects σ 0 \sigma_0 σ 0 . The dual graph of M t M_t M t is an extended Dynkin diagram, so we can associate an extended Cartan matrix A ~ \widetilde{A} A with entries A ~ i , j = − C i ⋅ C j \widetilde{A}_{i,j}=-C_i\cdot C_j A i , j = − C i ⋅ C j . Let m ˉ ∈ Z r + 1 \bar{m}\in\mathbb{Z}^{r+1} m ˉ ∈ Z r + 1 be the vector of multiplicities of the components of M t M_t M t . Then the kernel of A ~ \widetilde{A} A is spanned by m ˉ \bar{m} m ˉ . We can also associate a (non-extended) Dynkin diagram of type ADE by removing the vertex corresponding to C 0 C_0 C 0 from the dual graph of M t M_t M t . Thus, there exists a Cartan matrix A A A , which satisfies
A ~ = ( 2 v T v A ) . \widetilde{A}=
\begin{pmatrix}
2 & v^T\\
v & A
\end{pmatrix}. A = ( 2 v v T A ) .
The matrix A A A has full rank and its determinant is equal to the number of components of multiplicity 1 of M b M_b M b .
The Smooth Locus of a Singular Fiber as a Group
Consider an elliptic fibration π : M → B \pi: M \to B π : M → B . The smooth locus of π \pi π is M # : = { x ∈ M : d π x has full rank } M^\# := \{x \in M : d\pi_x \text{ has full rank}\} M # := { x ∈ M : d π x has full rank } . For any t ∈ B t \in B t ∈ B , the smooth locus of the fiber M t M_t M t is M t # : = M t ∩ M # M^\#_t := M_t \cap M^\# M t # := M t ∩ M # . If M t M_t M t is smooth, M t # = M t M^\#_t = M_t M t # = M t . Otherwise, M t # M^\#_t M t # is obtained by removing all singular points and higher-multiplicity components of M t M_t M t .
An analytic fiber system of groups over a complex manifold Δ \Delta Δ is a complex manifold G \mathcal{G} G with a holomorphic submersion Ψ : G → Δ \Psi: \mathcal{G} \to\Delta Ψ : G → Δ and a holomorphic section e : Δ → G e : \Delta\to\mathcal{G} e : Δ → G , such that
D : = { ( g 1 , g 2 ) ∈ G × G : Ψ ( g 1 ) = Ψ ( g 2 ) } ⊂ G × G , D := \{(g_1,g_2) \in\mathcal{G} \times\mathcal{G} : \Psi(g_1) = \Psi(g_2)\} \subset\mathcal{G} \times\mathcal{G}, D := {( g 1 , g 2 ) ∈ G × G : Ψ ( g 1 ) = Ψ ( g 2 )} ⊂ G × G ,
the map D → G D \to\mathcal{G} D → G given by ( g 1 , g 2 ) ↦ g 1 g 2 − 1 (g_1,g_2) \mapsto g_1g_2^{-1} ( g 1 , g 2 ) ↦ g 1 g 2 − 1 is holomorphic.
We show that locally, the smooth locus of an elliptic fibration is an analytic fiber system of groups.
Let t ∈ B t \in B t ∈ B be a critical value and let U t ⊂ B U_t \subset B U t ⊂ B be a disk around t t t such that σ 0 ∣ U t \sigma_0|_{U_t} σ 0 ∣ U t is holomorphic. Denote U t ′ : = U t − { t } U'_t := U_t - \{t\} U t ′ := U t − { t } and M U t ′ : = π − 1 ( U t ′ ) M'_{U_t} := \pi^{-1}(U'_t) M U t ′ := π − 1 ( U t ′ ) . Then π : M U t ′ → U t ′ \pi: M'_{U_t} \to U'_t π : M U t ′ → U t ′ is an analytic fiber system of groups with the holomorphic section σ 0 ∣ U t \sigma_0|_{U_t} σ 0 ∣ U t . The following shows that the group structure extends to the smooth locus of the singular fibers.
Theorem 2.4 ([8 Theorem 9.1] ). Let π : M → B \pi: M \to B π : M → B be an elliptic fibration and let t ∈ B t \in B t ∈ B be a critical value. For a disk U t ⊂ B U_t \subset B U t ⊂ B containing t t t , such that σ 0 ∣ U t \sigma_0|_{U_t} σ 0 ∣ U t is holomorphic, let M U t : = π − 1 ( U t ) M_{U_t} := \pi^{-1}(U_t) M U t := π − 1 ( U t ) . Then there exists on M U t # M^\#_{U_t} M U t # a unique structure of analytic fiber system of abelian groups over U t U_t U t , which is an extension of the structure on M U t ′ M'_{U_t} M U t ′ of analytic fiber system of abelian groups over U t ′ U'_t U t ′ .
Let t ∈ B t \in B t ∈ B be a critical value of π \pi π and denote by C 0 C_0 C 0 the irreducible component of M t M_t M t intersecting σ 0 \sigma_0 σ 0 . Let C 0 # : = C 0 ∩ M t # C^\#_0 := C_0 \cap M^\#_t C 0 # := C 0 ∩ M t # be the connected component of the zero-element in M t # M^\#_t M t # and define G ( M t ) : = π 0 ( M t # ) G(M_t) := \pi_0(M^\#_t) G ( M t ) := π 0 ( M t # ) . These fit into the following short exact sequence of topological groups:
0 → C 0 # → M t # → G ( M t ) → 0. 0 \to C^\#_0 \to M^\#_t \to G(M_t) \to0. 0 → C 0 # → M t # → G ( M t ) → 0.
Topologically, C 0 # C^\#_0 C 0 # is a sphere with one or two points removed (by Kodaira’s classification). Hence, as a group, C 0 # C^\#_0 C 0 # is isomorphic to C \mathbb{C} C or C × \mathbb{C}^\times C × . If C 0 # ≅ C C^\#_0 \cong\mathbb{C} C 0 # ≅ C , the fiber M t M_t M t is an additive fiber , otherwise M t M_t M t is a multiplicative fiber . By Kodaira’s classification, the only multiplicative fibers are those of type I n I_n I n for n ≥ 0 n \ge0 n ≥ 0 . The Lie group structure of G ( M t ) G(M_t) G ( M t ) , depending on the type of the singular fiber M t M_t M t is given in Table 2 .
Table 2. The group structure on the smooth locus of M t M_t M t is the semidirect product of C 0 # C^\#_0 C 0 # and G ( M t ) G(M_t) G ( M t ) .
Lemma 2.5. Let π : M → B \pi: M \to B π : M → B be an elliptic fibration. Fix a regular value b ∈ B b \in B b ∈ B and a critical value t ∈ B t \in B t ∈ B . Let f ∈ Mod ( M b ) f \in\operatorname{Mod}(M_b) f ∈ Mod ( M b ) be the monodromy around M t M_t M t and let f ∗ f_* f ∗ be the action it induces on H 1 ( M b ) H_1(M_b) H 1 ( M b ) . Then
G ( M t ) ≅ ( Z 2 / ( I − f ∗ ) Z 2 ) t o r . G(M_t) \cong\left(\mathbb{Z}^2/(I-f_*)\mathbb{Z}^2\right)_{\mathrm{tor}}. G ( M t ) ≅ ( Z 2 / ( I − f ∗ ) Z 2 ) tor . Proof. This can be checked for each type of singular fibers using Theorem 2.3 and Theorem 2.4 .
The Holomorphic Mordell–Weil Group
The holomorphic Mordell–Weil group of an elliptic surface π : M → B \pi: M \to B π : M → B with holomorphic zero-section is the group of holomorphic sections of π \pi π . The correspondence between sections and diffeomorphisms that act by translation makes this equivalent to the group of biholomorphic automorphisms of M M M that act by translation on each smooth fiber.
The Néron–Severi lattice NS ( M ) \operatorname{NS}(M) NS ( M ) of a complex surface M M M is defined as the group of divisors of M M M , quotiented by algebraic equivalence. If the base curve B B B is closed, the Lefschetz ( 1 , 1 ) (1,1) ( 1 , 1 ) -theorem implies
NS ( M ) = H 2 ( M ; Z ) ∩ H 1 , 1 ( M ) . \operatorname{NS}(M)=H^2(M;\mathbb{Z})\cap H^{1,1}(M). NS ( M ) = H 2 ( M ; Z ) ∩ H 1 , 1 ( M ) .
The following theorem gives an explicit identification of MW h o l ( π ) \operatorname{MW}^{\mathrm{hol}}(\pi) MW hol ( π ) in terms of the Néron–Severi lattice and the trivial lattice. For a proof, see [12 Theorem 6.5] .
Theorem 2.6 (Shioda–Tate Isomorphism). For any elliptic fibration π : M → B \pi: M \to B π : M → B over closed base B B B with holomorphic zero-section, there is an isomorphism
MW h o l ( π ) → ≅ NS ( M ) / Triv ( π ) , σ ↦ [ σ ] . \begin{aligned}
\operatorname{MW}^{\mathrm{hol}}(\pi) &\xrightarrow{\cong} \operatorname{NS}(M)/\operatorname{Triv}(\pi),\\
\sigma&\mapsto[\sigma].
\end{aligned} MW hol ( π ) σ ≅ NS ( M ) / Triv ( π ) , ↦ [ σ ] .
Computing MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ )
Our computation of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) relies heavily on the methods from [4 ] . We give all details for completeness, expressing MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) in terms of sheaf cohomology and using a spectral sequence argument.
Cohomological Characterization of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ )
Let T ( π ∘ ) \mathcal{T}(\pi^\circ) T ( π ∘ ) be the sheaf of smooth translations of π ∘ \pi^\circ π ∘ : for any open set U ⊆ B ∘ U \subseteq B^\circ U ⊆ B ∘ , let T ( π ∘ ) ( U ) \mathcal{T}(\pi^\circ)(U) T ( π ∘ ) ( U ) be the group of diffeomorphisms of π ∘ − 1 ( U ) \pi^{\circ-1}(U) π ∘− 1 ( U ) which act by translation on each fiber. Let E B ∘ \mathcal{E}_{B^\circ} E B ∘ denote the sheaf of smooth real-valued functions on B ∘ B^\circ B ∘ .
Proposition 3.1. Let π : M → B \pi: M \to B π : M → B be an elliptic surface and π ∘ : M ∘ → B ∘ \pi^\circ: M^\circ\to B^\circ π ∘ : M ∘ → B ∘ the fiber bundle obtained by removing a small neighborhood of each singular fiber. Then there exists a natural isomorphism
δ : MW ( π ∘ ) → ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) , \delta:\operatorname{MW}(\pi^\circ)\xrightarrow{\cong}H^1(B^\circ,R^1(\pi^\circ)_*\mathbb{Z}), δ : MW ( π ∘ ) ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) , induced by the boundary map in the long exact sequence in cohomology induced by the short exact sequence of sheaves
0 → R 1 ( π ∘ ) ∗ Z → R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ → T ( π ∘ ) → 0. (1) 0 \to R^1(\pi^\circ)_*\mathbb{Z}\to R^1(\pi^\circ)_*\mathbb{Z}\otimes_{\mathbb{Z}}\mathcal{E}_{B^\circ}\to\mathcal{T}(\pi^\circ)\to0. \tag*{(1)} 0 → R 1 ( π ∘ ) ∗ Z → R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ → T ( π ∘ ) → 0. (1)
Proof. For each t ∈ B ∘ t \in B^\circ t ∈ B ∘ , translations of M t M_t M t are naturally identified with H 1 ( M t ; R ) / H 1 ( M t ; Z ) H_1(M_t;\mathbb{R})/H_1(M_t;\mathbb{Z}) H 1 ( M t ; R ) / H 1 ( M t ; Z ) . Hence, fiberwise Poincaré duality gives the short exact sequence of sheaves (1). Since E B ∘ \mathcal{E}_{B^\circ} E B ∘ is a fine sheaf, R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ R^1(\pi^\circ)_*\mathbb{Z}\otimes_{\mathbb{Z}}\mathcal{E}_{B^\circ} R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ is also fine, so H i ( B ∘ , R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ) ≅ 0 H^i(B^\circ,R^1(\pi^\circ)_*\mathbb{Z}\otimes_{\mathbb{Z}}\mathcal{E}_{B^\circ})\cong0 H i ( B ∘ , R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ) ≅ 0 , for any i > 0 i>0 i > 0 . Hence, the long exact sequence of topological groups associated with (1) becomes
0 → H 0 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) → H 0 ( B ∘ , R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ) → H 0 ( B ∘ , T ( π ∘ ) ) → δ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) → 0. 0\to H^0(B^\circ,R^1(\pi^\circ)_*\mathbb{Z})\to H^0(B^\circ,R^1(\pi^\circ)_*\mathbb{Z}\otimes_{\mathbb{Z}}\mathcal{E}_{B^\circ})\to H^0(B^\circ,\mathcal{T}(\pi^\circ))\xrightarrow{\delta}H^1(B^\circ,R^1(\pi^\circ)_*\mathbb{Z})\to0. 0 → H 0 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) → H 0 ( B ∘ , R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ) → H 0 ( B ∘ , T ( π ∘ )) δ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) → 0.
The space H 0 ( B ∘ , R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ) H^{0}(B^{\circ}, R^{1}(\pi^{\circ})_{*}\mathbb{Z}\otimes_{\mathbb{Z}} \mathcal{E}_{B^{\circ}}) H 0 ( B ∘ , R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ) is connected, since it is a vector space, and H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) H^{1}(B^{\circ}, R^{1}(\pi^{\circ})_{*}\mathbb{Z}) H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) is discrete, so exactness of the above sequence implies
π 0 ( H 0 ( B ∘ , T ( π ∘ ) ) ) ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) , \pi_{0}\left(H^{0}(B^{\circ}, \mathcal{T}(\pi^{\circ}))\right) \cong H^{1}(B^{\circ}, R^{1}(\pi^{\circ})_{*}\mathbb{Z}), π 0 ( H 0 ( B ∘ , T ( π ∘ )) ) ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ,
which is what we wanted to prove.
MW(π ∘ \pi^{\circ} π ∘ ) as annihilator of the fiber class
For any 4-manifold M M M and class v ∈ H 2 ( M ) v \in H_{2}(M) v ∈ H 2 ( M ) , we denote the annihilator of v v v by H 2 ( M ) v H^{2}(M)^{v} H 2 ( M ) v . We adopt the convention that a diffeomorphism f ∈ Diff ( M ) f \in\operatorname{Diff}(M) f ∈ Diff ( M ) acts on H 2 ( M ) H^{2}(M) H 2 ( M ) by ( f − 1 ) ∗ (f^{-1})^{*} ( f − 1 ) ∗ .
Proposition 3.2. Let π : M → B \pi: M \to B π : M → B be an elliptic fibration over a compact base B B B and let π ∘ : M ∘ → B ∘ \pi^{\circ} : M^{\circ} \to B^{\circ} π ∘ : M ∘ → B ∘ be the fiber bundle obtained by removing an open neighborhood of each singular fiber. Let F ∈ H 2 ( M ∘ ) F \in H_{2}(M^{\circ}) F ∈ H 2 ( M ∘ ) be the fiber class of π ∘ \pi^{\circ} π ∘ .
(i) There exists a natural isomorphism
Φ : MW ( π ∘ ) → ≅ H 2 ( M ∘ ) F . \Phi: \operatorname{MW}(\pi^{\circ}) \xrightarrow{\ \cong\ } H^{2}(M^{\circ})^{F}. Φ : MW ( π ∘ ) ≅ H 2 ( M ∘ ) F . (ii) For each τ ∈ MW ( π ∘ ) \tau\in\operatorname{MW}(\pi^{\circ}) τ ∈ MW ( π ∘ ) , there exists a unique γ τ ∈ H 2 ( M ∘ ) F \gamma_{\tau} \in H^{2}(M^{\circ})^{F} γ τ ∈ H 2 ( M ∘ ) F such that τ \tau τ acts on ξ ∈ H 2 ( M ∘ ) \xi\in H^{2}(M^{\circ}) ξ ∈ H 2 ( M ∘ ) by
τ ( ξ ) = ξ + ⟨ ξ , F ⟩ γ τ . \tau(\xi) = \xi+ \langle\xi,F\rangle\gamma_{\tau}. τ ( ξ ) = ξ + ⟨ ξ , F ⟩ γ τ . (iii) Explicitly, the isomorphism Φ \Phi Φ lifts to the following homomorphism
Γ s m ( B ∘ , M ∘ ) ⟶ H 2 ( M ∘ ) F \Gamma^{\mathrm{sm}}(B^{\circ}, M^{\circ}) \longrightarrow H^{2}(M^{\circ})^{F} Γ sm ( B ∘ , M ∘ ) ⟶ H 2 ( M ∘ ) F σ ⟼ PD ( M ∘ , ∂ M ∘ ) [ σ ] − PD ( M ∘ , ∂ M ∘ ) [ σ 0 ∣ B ∘ ] . \sigma\longmapsto\operatorname{PD}_{(M^{\circ},\partial M^{\circ})}[\sigma] - \operatorname{PD}_{(M^{\circ},\partial M^{\circ})}[\sigma_{0}|_{B^{\circ}}]. σ ⟼ PD ( M ∘ , ∂ M ∘ ) [ σ ] − PD ( M ∘ , ∂ M ∘ ) [ σ 0 ∣ B ∘ ] .
Proof. The Leray spectral sequence for π ∘ \pi^{\circ} π ∘ is
E 2 p , q = H p ( B ∘ , R q ( π ∘ ) ∗ Z ) ⟹ H p + q ( M ∘ ) . E_{2}^{p,q}=H^{p}(B^{\circ}, R^{q}(\pi^{\circ})_{*}\mathbb{Z}) \Longrightarrow H^{p+q}(M^{\circ}). E 2 p , q = H p ( B ∘ , R q ( π ∘ ) ∗ Z ) ⟹ H p + q ( M ∘ ) .
Since B ∘ B^{\circ} B ∘ strong deformation retracts to a wedge of circles, H p ( B ∘ , R q ( π ∘ ) ∗ Z ) H^{p}(B^{\circ}, R^{q}(\pi^{\circ})_{*}\mathbb{Z}) H p ( B ∘ , R q ( π ∘ ) ∗ Z ) vanishes if p ≥ 2 p \ge2 p ≥ 2 or q ≥ 3 q \ge3 q ≥ 3 . Thus, the Leray spectral sequence degenerates on the E 2 E_{2} E 2 page.
Observe that R 2 ( π ∘ ) ∗ Z R^{2}(\pi^{\circ})_{*}\mathbb{Z} R 2 ( π ∘ ) ∗ Z is a trivial local system of rank 1. Indeed, every fiber of π ∘ \pi^{\circ} π ∘ is a torus, so the stalks are all isomorphic to H 2 ( T 2 ) ≅ Z H^{2}(T^{2}) \cong\mathbb{Z} H 2 ( T 2 ) ≅ Z . Because the complex structure induces an orientation, R 2 ( π ∘ ) ∗ Z R^{2}(\pi^{\circ})_{*}\mathbb{Z} R 2 ( π ∘ ) ∗ Z must have trivial monodromy. Thus, a natural isomorphism H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) ≅ Z H^{0}(B^{\circ}, R^{2}(\pi^{\circ})_{*}\mathbb{Z}) \cong\mathbb{Z} H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) ≅ Z is given by integration over the fiber class F ∈ H 2 ( M ∘ ) F \in H_{2}(M^{\circ}) F ∈ H 2 ( M ∘ ) .
Consider the Leray filtration
H 2 ( M ∘ ) = L 2 H 2 ⊃ L 1 H 2 ⊃ L 0 H 2 = 0. H^{2}(M^{\circ}) = L_{2}H^{2} \supset L_{1}H^{2} \supset L_{0}H^{2} = 0. H 2 ( M ∘ ) = L 2 H 2 ⊃ L 1 H 2 ⊃ L 0 H 2 = 0.
Since E 2 = E ∞ E_{2}=E_{\infty} E 2 = E ∞ , it satisfies L 2 H 2 / L 1 H 2 ≅ H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) L_{2}H^{2}/L_{1}H^{2} \cong H^{0}(B^{\circ}, R^{2}(\pi^{\circ})_{*}\mathbb{Z}) L 2 H 2 / L 1 H 2 ≅ H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) and L 1 H 2 / L 0 H 2 ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) L_{1}H^{2}/L_{0}H^{2} \cong H^{1}(B^{\circ}, R^{1}(\pi^{\circ})_{*}\mathbb{Z}) L 1 H 2 / L 0 H 2 ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) . This gives the short exact sequence
0 ⟶ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ⟶ H 2 ( M ∘ ) ⟶ H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) ⟶ 0 , (2) 0 \longrightarrow H^{1}(B^{\circ}, R^{1}(\pi^{\circ})_{*}\mathbb{Z}) \longrightarrow H^{2}(M^{\circ}) \longrightarrow H^{0}(B^{\circ}, R^{2}(\pi^{\circ})_{*}\mathbb{Z}) \longrightarrow0, \tag*{(2)} 0 ⟶ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ⟶ H 2 ( M ∘ ) ⟶ H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) ⟶ 0 , (2)
where H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) ≅ Z H^{0}(B^{\circ}, R^{2}(\pi^{\circ})_{*}\mathbb{Z}) \cong\mathbb{Z} H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) ≅ Z and the second map is given by integrating over the fiber class F ∈ H 2 ( M ∘ ) F \in H_{2}(M^{\circ}) F ∈ H 2 ( M ∘ ) . The last factor is free, so the short exact sequence splits and by Proposition 3.1,
MW ( π ∘ ) ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ≅ H 2 ( M ∘ ) F . \operatorname{MW}(\pi^{\circ}) \cong H^{1}(B^{\circ}, R^{1}(\pi^{\circ})_{*}\mathbb{Z}) \cong H^{2}(M^{\circ})^{F}. MW ( π ∘ ) ≅ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ≅ H 2 ( M ∘ ) F .
Note that any τ ∈ MW ( π ∘ ) \tau\in\operatorname{MW}(\pi^\circ) τ ∈ MW ( π ∘ ) acts on H 2 ( M ∘ ) H^2(M^\circ) H 2 ( M ∘ ) and induces a trivial action on H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) H^1(B^\circ,R^1(\pi^\circ)_*\mathbb{Z}) H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) and H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) H^0(B^\circ,R^2(\pi^\circ)_*\mathbb{Z}) H 0 ( B ∘ , R 2 ( π ∘ ) ∗ Z ) , since it acts by fiberwise translation. Let ξ ∈ H 2 ( M ∘ ) \xi\in H^2(M^\circ) ξ ∈ H 2 ( M ∘ ) . The restriction of the zero-section σ 0 \sigma_0 σ 0 to B ∘ B^\circ B ∘ gives a class [ σ 0 ∣ B ∘ ] ∈ H 2 ( M ∘ , ∂ M ∘ ) [\sigma_0|_{B^\circ}] \in H_2(M^\circ,\partial M^\circ) [ σ 0 ∣ B ∘ ] ∈ H 2 ( M ∘ , ∂ M ∘ ) . Let s ∈ H 2 ( M ∘ ) s \in H^2(M^\circ) s ∈ H 2 ( M ∘ ) denote its image under Poincaré–Lefschetz duality in ( M ∘ , ∂ M ∘ ) (M^\circ,\partial M^\circ) ( M ∘ , ∂ M ∘ ) . Then, ⟨ s , F ⟩ = 1 \langle s,F\rangle=1 ⟨ s , F ⟩ = 1 . Hence, ξ − ⟨ ξ , F ⟩ s \xi-\langle\xi,F\rangle s ξ − ⟨ ξ , F ⟩ s pairs trivially with F F F , so it lies in the first term of the short exact sequence (2). Therefore,
τ ∗ ( ξ ) = τ ∗ ( ξ − ⟨ ξ , F ⟩ s ) + τ ∗ ( ⟨ ξ , F ⟩ s ) = ξ − ⟨ ξ , F ⟩ s + ⟨ ξ , F ⟩ τ ∗ ( s ) . \tau_*(\xi)=\tau_*(\xi-\langle\xi,F\rangle s)+\tau_*(\langle\xi,F\rangle s)=\xi-\langle\xi,F\rangle s+\langle\xi,F\rangle\tau_*(s). τ ∗ ( ξ ) = τ ∗ ( ξ − ⟨ ξ , F ⟩ s ) + τ ∗ (⟨ ξ , F ⟩ s ) = ξ − ⟨ ξ , F ⟩ s + ⟨ ξ , F ⟩ τ ∗ ( s ) .
Set γ τ : = τ ∗ ( s ) − s \gamma_\tau:=\tau_*(s)-s γ τ := τ ∗ ( s ) − s . If τ ∈ MW ( π ∘ ) \tau\in\operatorname{MW}(\pi^\circ) τ ∈ MW ( π ∘ ) is represented by a diffeomorphism that acts by translation by a section σ \sigma σ , then τ ∗ ( s ) = PD ( M ∘ , ∂ M ∘ ) [ σ ] \tau_*(s)=\operatorname{PD}_{(M^\circ,\partial M^\circ)}[\sigma] τ ∗ ( s ) = PD ( M ∘ , ∂ M ∘ ) [ σ ] .
It remains to prove that the isomorphism Φ ′ \Phi' Φ ′ defined as the composition
MW ( π ∘ ) → δ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) → ι H 2 ( M ∘ ) F \operatorname{MW}(\pi^\circ)\xrightarrow{\delta}H^1(B^\circ,R^1(\pi^\circ)_*\mathbb{Z})\xrightarrow{\iota}H^2(M^\circ)^F MW ( π ∘ ) δ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ι H 2 ( M ∘ ) F
is (up to sign) given by
τ ↦ γ τ . \tau\mapsto\gamma_\tau. τ ↦ γ τ .
Let { U i } \{U_i\} { U i } be a good cover of B ∘ B^\circ B ∘ which trivializes π ∘ \pi^\circ π ∘ . Consider a representative τ ^ ∈ H 0 ( B ∘ , T ( π ∘ ) ) \widehat{\tau}\in H^0(B^\circ,\mathcal{T}(\pi^\circ)) τ ∈ H 0 ( B ∘ , T ( π ∘ )) of τ \tau τ corresponding to the section σ : B ∘ → M ∘ \sigma:B^\circ\to M^\circ σ : B ∘ → M ∘ , and let ( τ i ) i (\tau_i)_i ( τ i ) i be a Čech 0-cocycle representing τ ^ \widehat{\tau} τ , so τ i ∈ T ( π ∘ ) ( U i ) \tau_i\in\mathcal{T}(\pi^\circ)(U_i) τ i ∈ T ( π ∘ ) ( U i ) . Let λ i ∈ R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ( U i ) \lambda_i\in R^1(\pi^\circ)_*\mathbb{Z}\otimes_{\mathbb{Z}}\mathcal{E}_{B^\circ}(U_i) λ i ∈ R 1 ( π ∘ ) ∗ Z ⊗ Z E B ∘ ( U i ) be lifts of τ i \tau_i τ i . On intersections, λ j − λ i ∈ R 1 ( π ∘ ) ∗ Z ( U i ∩ U j ) \lambda_j-\lambda_i\in R^1(\pi^\circ)_*\mathbb{Z}(U_i\cap U_j) λ j − λ i ∈ R 1 ( π ∘ ) ∗ Z ( U i ∩ U j ) and δ ( τ ^ ) ∈ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) \delta(\widehat{\tau})\in H^1(B^\circ,R^1(\pi^\circ)_*\mathbb{Z}) δ ( τ ) ∈ H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) is represented by the Čech 1-cocycle ( λ j − λ i ) i , j (\lambda_j-\lambda_i)_{i,j} ( λ j − λ i ) i , j .
We construct b i ∈ C 1 ( π − 1 ( U i ) ; Z ) b_i\in C^1(\pi^{-1}(U_i);\mathbb{Z}) b i ∈ C 1 ( π − 1 ( U i ) ; Z ) , such that for i < j i<j i < j , the equality [ ( λ i − λ j ) i , j ] = [ ( b i − b j ) i , j ] [(\lambda_i-\lambda_j)_{i,j}]=[(b_i-b_j)_{i,j}] [( λ i − λ j ) i , j ] = [( b i − b j ) i , j ] holds in H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) H^1(B^\circ,R^1(\pi^\circ)_*\mathbb{Z}) H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) . Then the inclusion ι : H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ↪ H 2 ( M ∘ ) \iota:H^1(B^\circ,R^1(\pi^\circ)_*\mathbb{Z})\hookrightarrow H^2(M^\circ) ι : H 1 ( B ∘ , R 1 ( π ∘ ) ∗ Z ) ↪ H 2 ( M ∘ ) maps ( b j − b i ) i , j (b_j-b_i)_{i,j} ( b j − b i ) i , j to the class of ( − d b i ) i (-db_i)_i ( − d b i ) i in H 2 ( M ∘ ) H^2(M^\circ) H 2 ( M ∘ ) . Let
q : H 1 ( T 2 ; R ) ⟶ H 1 ( T 2 ; R ) / H 1 ( T 2 ; Z ) q:H^1(T^2;\mathbb{R})\longrightarrow H^1(T^2;\mathbb{R})/H^1(T^2;\mathbb{Z}) q : H 1 ( T 2 ; R ) ⟶ H 1 ( T 2 ; R ) / H 1 ( T 2 ; Z )
denote the natural projection. For each i i i , the map λ i : U i → H 1 ( T 2 ; R ) \lambda_i:U_i\to H^1(T^2;\mathbb{R}) λ i : U i → H 1 ( T 2 ; R ) determines a local isotopy p i p_i p i from σ 0 \sigma_0 σ 0 to σ \sigma σ by setting
p i : U i × [ 0 , 1 ] ⟶ π − 1 ( U i ) , p_i:U_i\times[0,1]\longrightarrow\pi^{-1}(U_i), p i : U i × [ 0 , 1 ] ⟶ π − 1 ( U i ) ,
p i ( x , v ) = q ( v λ i ( x ) ) ( σ 0 ( x ) ) , p_i(x,v)=q(v\lambda_i(x))(\sigma_0(x)), p i ( x , v ) = q ( v λ i ( x )) ( σ 0 ( x )) ,
where H 1 ( T 2 ; R ) / H 1 ( T 2 ; Z ) H^1(T^2;\mathbb{R})/H^1(T^2;\mathbb{Z}) H 1 ( T 2 ; R ) / H 1 ( T 2 ; Z ) is identified with the group of translations on T 2 T^2 T 2 . Let C i : = p i ( U i × [ 0 , 1 ] ) C_i:=p_i(U_i\times[0,1]) C i := p i ( U i × [ 0 , 1 ]) , viewed as a relative locally finite chain in C 1 l f ( π − 1 ( U i ) , ∂ π − 1 ( U i ) ) C^{\mathrm{lf}}_1(\pi^{-1}(U_i),\partial\pi^{-1}(U_i)) C 1 lf ( π − 1 ( U i ) , ∂ π − 1 ( U i )) . Then ∂ C i = [ σ ( U i ) ] − [ σ 0 ( U i ) ] \partial C_i=[\sigma(U_i)]-[\sigma_0(U_i)] ∂ C i = [ σ ( U i )] − [ σ 0 ( U i )] . Let D i : C k l f ( π − 1 ( U i ) , ∂ π − 1 ( U i ) ) → C 4 − k ( π − 1 ( U i ) ) D_i:C^{\mathrm{lf}}_k(\pi^{-1}(U_i),\partial\pi^{-1}(U_i))\to C^{4-k}(\pi^{-1}(U_i)) D i : C k lf ( π − 1 ( U i ) , ∂ π − 1 ( U i )) → C 4 − k ( π − 1 ( U i )) be a chain-level realization of Poincaré–Lefschetz duality such that d D i ( c ) = D i ( ∂ c ) dD_i(c)=D_i(\partial c) d D i ( c ) = D i ( ∂ c ) for any c ∈ C k l f ( π − 1 ( U i ) , ∂ π − 1 ( U i ) ) c\in C^{\mathrm{lf}}_k(\pi^{-1}(U_i),\partial\pi^{-1}(U_i)) c ∈ C k lf ( π − 1 ( U i ) , ∂ π − 1 ( U i )) . Set b i : = D i ( C i ) ∈ C 1 ( π − 1 ( U i ) ; Z ) b_i:=D_i(C_i)\in C^1(\pi^{-1}(U_i);\mathbb{Z}) b i := D i ( C i ) ∈ C 1 ( π − 1 ( U i ) ; Z ) . Then d b i = D i ( [ σ ( U i ) ] − [ σ 0 ( U i ) ] ) db_i=D_i([\sigma(U_i)]-[\sigma_0(U_i)]) d b i = D i ([ σ ( U i )] − [ σ 0 ( U i )]) , so this is a cocycle representing PD ( σ ( U i ) ) − PD ( σ 0 ( U i ) ) \operatorname{PD}(\sigma(U_i))-\operatorname{PD}(\sigma_0(U_i)) PD ( σ ( U i )) − PD ( σ 0 ( U i )) .
Note that C j − C i C_j-C_i C j − C i is the fiberwise concatenation of the paths p j p_j p j and the inverse of p i p_i p i . For each x ∈ U i ∩ U j x\in U_i\cap U_j x ∈ U i ∩ U j , let l x l_x l x be the concatenation of the paths p j ( x , ⋅ ) p_j(x,\cdot) p j ( x , ⋅ ) and p i ( x , ⋅ ) p_i(x,\cdot) p i ( x , ⋅ ) with opposite orientation. This is a cycle in M x M_x M x , based at σ 0 ( x ) \sigma_0(x) σ 0 ( x ) , so by covering space theory, there exists a unique lift l ~ : [ 0 , 1 ] → H 1 ( M x ; R ) \widetilde{l}:[0,1]\to H^1(M_x;\mathbb{R}) l : [ 0 , 1 ] → H 1 ( M x ; R ) with l ~ ( 0 ) = 0 \widetilde{l}(0)=0 l ( 0 ) = 0 . Continuity of l ~ \widetilde{l} l and the construction of p i p_i p i imply
l ~ ( v ) = { 2 v λ j ( x ) , if 0 ≤ v ≤ 1 2 , ( 1 − 2 v ) λ i ( x ) + λ j ( x ) , if 1 2 ≤ v ≤ 1. \widetilde{l}(v)=
\begin{cases}
2v\lambda_j(x), & \text{if }0\leq v\leq\frac{1}{2},\\
(1-2v)\lambda_i(x)+\lambda_j(x), & \text{if }\frac{1}{2}\leq v\leq1.
\end{cases} l ( v ) = { 2 v λ j ( x ) , ( 1 − 2 v ) λ i ( x ) + λ j ( x ) , if 0 ≤ v ≤ 2 1 , if 2 1 ≤ v ≤ 1.
Hence, l ~ ( 1 ) = λ j − λ i \widetilde{l}(1)=\lambda_j-\lambda_i l ( 1 ) = λ j − λ i and l [ ( λ j − λ i ) i , j ] = l [ ( b j − b i ) i , j ] = [ ( − d b i ) i ] l[(\lambda_j-\lambda_i)_{i,j}]=l[(b_j-b_i)_{i,j}]=[(-db_i)_i] l [( λ j − λ i ) i , j ] = l [( b j − b i ) i , j ] = [( − d b i ) i ] , which coincide on intersections and glue to the class − ( PD [ σ ] − PD [ σ 0 ] ) ∈ H 2 ( M ∘ ; Z ) -(\operatorname{PD}[\sigma]-\operatorname{PD}[\sigma_0])\in H^2(M^\circ;\mathbb{Z}) − ( PD [ σ ] − PD [ σ 0 ]) ∈ H 2 ( M ∘ ; Z ) . Hence, setting Φ = − Φ ′ \Phi=-\Phi' Φ = − Φ ′ concludes the proof.
Elliptic Fibrations over a Disk with One Singular Fiber
In this section, we analyze an elliptic fibration over a disk with one singular fiber, explicitly computing MW ( π ) \operatorname{MW}(\pi) MW ( π ) and MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) . We determine a complete obstruction to extending sections locally, in a small neighborhood of a singular fiber. Let D D D be the closed unit disk in C \mathbb{C} C and consider an elliptic fibration π : X → D \pi:X\to D π : X → D with only one singular fiber at the origin. Let D ε ⊂ D D_\varepsilon\subset D D ε ⊂ D be a small open disk around the origin and let D ∘ : = D − D ε D^\circ:=D-D_\varepsilon D ∘ := D − D ε and X ∘ : = π − 1 ( D ∘ ) X^\circ:=\pi^{-1}(D^\circ) X ∘ := π − 1 ( D ∘ ) . We answer the following:
Question 4.1. Given an isotopy class in MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) , when does it have a representative section σ : D ∘ → X ∘ \sigma:D^\circ\to X^\circ σ : D ∘ → X ∘ that extends to a section σ : D → X \sigma:D \to X σ : D → X ?
Since D ∘ D^\circ D ∘ strong deformation retracts onto its boundary, this is equivalent to asking when a section σ : ∂ D → ∂ X \sigma:\partial D \to\partial X σ : ∂ D → ∂ X extends to a section over the entire disk D D D . We construct a map ψ : MW ( π ∘ ) → H 1 ( X 0 ) \psi:\operatorname{MW}(\pi^\circ) \to H_1(X_0) ψ : MW ( π ∘ ) → H 1 ( X 0 ) and show that it captures the obstruction to extending sections: a section σ \sigma σ extends if and only if ψ ( [ σ ] ) = 0 \psi([\sigma])=0 ψ ([ σ ]) = 0 .
Definition of ψ \psi ψ and Local Obstruction Theorem
We define a homomorphism ψ : MW ( π ∘ ) → H 1 ( X 0 ) \psi:\operatorname{MW}(\pi^\circ) \to H_1(X_0) ψ : MW ( π ∘ ) → H 1 ( X 0 ) . Given an element in MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) , pick a representative section σ : D ∘ → X ∘ \sigma:D^\circ\to X^\circ σ : D ∘ → X ∘ . The image of the restriction σ ∣ ∂ D : ∂ D → ∂ X \sigma|_{\partial D}:\partial D \to\partial X σ ∣ ∂ D : ∂ D → ∂ X represents a homology class [ σ ∣ ∂ D ] ∈ H 1 ( ∂ X ) [\sigma|_{\partial D}] \in H_1(\partial X) [ σ ∣ ∂ D ] ∈ H 1 ( ∂ X ) . This class is independent of the choice of isotopy representative. Indeed, if two sections σ , σ ′ : D ∘ → X ∘ \sigma,\sigma':D^\circ\to X^\circ σ , σ ′ : D ∘ → X ∘ are isotopic, the isotopy restricts to ∂ D \partial D ∂ D and traces an annulus in ∂ X \partial X ∂ X . Then, σ ( ∂ D ) \sigma(\partial D) σ ( ∂ D ) and σ ′ ( ∂ D ) \sigma'(\partial D) σ ′ ( ∂ D ) are the two boundary components of the annulus traced out by the isotopy. Thus, the 1-cycle in ∂ X \partial X ∂ X represented by σ ∣ ∂ D − σ ′ ∣ ∂ D \sigma|_{\partial D}-\sigma'|_{\partial D} σ ∣ ∂ D − σ ′ ∣ ∂ D is the boundary of a 2-cycle in ∂ X \partial X ∂ X , meaning [ σ ∣ ∂ D ] = [ σ ′ ∣ ∂ D ] [\sigma|_{\partial D}]=[\sigma'|_{\partial D}] [ σ ∣ ∂ D ] = [ σ ′ ∣ ∂ D ] in H 1 ( ∂ X ) H_1(\partial X) H 1 ( ∂ X ) . Hence, we can define a map
η : MW ( π ∘ ) ⟶ H 1 ( ∂ X ) , [ σ ] ⟼ [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ] . \eta:\operatorname{MW}(\pi^\circ) \longrightarrow H_1(\partial X), \qquad[\sigma]\longmapsto[\sigma|_{\partial D}]-[\sigma_0|_{\partial D}]. η : MW ( π ∘ ) ⟶ H 1 ( ∂ X ) , [ σ ] ⟼ [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ] .
The inclusion ∂ X ↪ X \partial X \hookrightarrow X ∂ X ↪ X induces a map H 1 ( ∂ X ) → H 1 ( X ) H_1(\partial X) \to H_1(X) H 1 ( ∂ X ) → H 1 ( X ) . By Proposition 2.2, X X X strong deformation retracts to X 0 X_0 X 0 , inducing an isomorphism H 1 ( X ) ≅ H 1 ( X 0 ) H_1(X) \cong H_1(X_0) H 1 ( X ) ≅ H 1 ( X 0 ) . We define ψ \psi ψ as the composition of these maps:
MW ( π ∘ ) → η H 1 ( ∂ X ) ⟶ H 1 ( X ) → ≅ H 1 ( X 0 ) . \operatorname{MW}(\pi^\circ) \xrightarrow{\eta} H_1(\partial X) \longrightarrow H_1(X) \xrightarrow{\cong} H_1(X_0). MW ( π ∘ ) η H 1 ( ∂ X ) ⟶ H 1 ( X ) ≅ H 1 ( X 0 ) .
Intuitively, ψ \psi ψ takes a section over D ∘ D^\circ D ∘ and pushes its image over ∂ D \partial D ∂ D into the central fiber X 0 X_0 X 0 , as depicted in Figure 4 .
Figure 4. The map ψ \psi ψ restricts a section σ \sigma σ to the boundary, then shrinks it to X 0 X_0 X 0 .
The following theorem gives a complete characterization of when a section extends to the central fiber up to isotopy. This is crucial in computing the Mordell–Weil group of an arbitrary elliptic surface.
Theorem 4.2 (Local Obstruction Theorem). Let π : X → D \pi:X \to D π : X → D be an elliptic fibration over a disk, with only one singular fiber at the origin. The following is a short exact sequence of groups
0 ⟶ MW ( π ) ⟶ MW ( π ∘ ) → ψ H 1 ( X 0 ) ⟶ 0. 0 \longrightarrow\operatorname{MW}(\pi) \longrightarrow\operatorname{MW}(\pi^\circ) \xrightarrow{\psi} H_1(X_0) \longrightarrow0. 0 ⟶ MW ( π ) ⟶ MW ( π ∘ ) ψ H 1 ( X 0 ) ⟶ 0.
Remark 4.3. We can see immediately that if a section σ : D ∘ → X ∘ \sigma:D^\circ\to X^\circ σ : D ∘ → X ∘ extends to a section σ ˉ : D → X \bar{\sigma}:D \to X σ ˉ : D → X , then ψ ( [ σ ] ) = 0 \psi([\sigma])=0 ψ ([ σ ]) = 0 . Indeed, σ ∣ ∂ D \sigma|_{\partial D} σ ∣ ∂ D represents a trivial class in H 1 ( X ) H_1(X) H 1 ( X ) , since it is the boundary of the 2-cycle σ ˉ ( D ) \bar{\sigma}(D) σ ˉ ( D ) . The same holds for the zero-section σ 0 \sigma_0 σ 0 . Therefore, [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ] [\sigma|_{\partial D}]-[\sigma_0|_{\partial D}] [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ] is zero in H 1 ( X ) ≅ H 1 ( X 0 ) H_1(X) \cong H_1(X_0) H 1 ( X ) ≅ H 1 ( X 0 ) . The main point of Theorem 4.2 is that this condition is sufficient: if ψ ( [ σ ] ) = 0 \psi([\sigma])=0 ψ ([ σ ]) = 0 , then [ σ ] [\sigma] [ σ ] has a representative which extends to D D D .
Remark 4.4. Recall that by Kodaira’s classification, additive fibers are simply-connected. Hence, if X 0 X_0 X 0 is additive, H 1 ( X 0 ) ≅ 0 H_1(X_0) \cong0 H 1 ( X 0 ) ≅ 0 and Theorem 4.2 implies that all section classes of π ∘ \pi^\circ π ∘ extend to sections of π \pi π .
Example 4.5 (A section that does not extend). Let D ⊂ C D \subset\mathbb{C} D ⊂ C be a disk centered at the origin and let π : X → D \pi: X \to D π : X → D be a proper holomorphic map such that for t ≠ 0 t \ne0 t = 0 , the fibers X t X_t X t are smooth tori and the fiber at the origin is of type I n ∗ I_n^* I n ∗ (see Figure 5 a for the case n = 1 n=1 n = 1 ). The restriction π : ∂ X → ∂ D \pi: \partial X \to\partial D π : ∂ X → ∂ D is a torus-bundle over a circle. Pick a basepoint t t t on ∂ D \partial D ∂ D and fix an identification of X t X_t X t with the standard torus T 2 T^2 T 2 . Choose a parametrization γ : [ 0 , 1 ] → ∂ D \gamma: [0,1] \to\partial D γ : [ 0 , 1 ] → ∂ D with γ ( 0 ) = γ ( 1 ) = t \gamma(0) = \gamma(1) = t γ ( 0 ) = γ ( 1 ) = t . Let f ∈ Mod ( T 2 ) f \in\operatorname{Mod}(T^2) f ∈ Mod ( T 2 ) be the monodromy transformation corresponding to γ \gamma γ . By Kodaira’s classification, we can pick curves α , β \alpha, \beta α , β on T 2 T^2 T 2 , representing a basis of H 1 ( T 2 ) H_1(T^2) H 1 ( T 2 ) such that f f f acts on H 1 ( T 2 ) H_1(T^2) H 1 ( T 2 ) as
Figure 5. Example of a section that does not extend.
f ∗ = ( 1 n 0 1 ) . f_* = \begin{pmatrix} 1 & n \\ 0 & 1 \end{pmatrix}. f ∗ = ( 1 0 n 1 ) .
This means that f f f is the n n n -th power of a Dehn twist about α \alpha α . By Picard-Lefschetz theory, this implies that α \alpha α is the vanishing cycle of the fibration, i.e. its homology class vanishes in H 1 ( X 0 ) H_1(X_0) H 1 ( X 0 ) . Let φ ∈ Diff + ( T 2 ) \varphi\in\operatorname{Diff}^+(T^2) φ ∈ Diff + ( T 2 ) be a representative of f f f that acts as the identity on T 2 − R T^2 - R T 2 − R for a regular neighborhood R R R of α \alpha α . Then ∂ X \partial X ∂ X is diffeomorphic to the mapping torus
M φ = ( T 2 × [ 0 , 1 ] ) / ( x , 0 ) ∼ ( φ ( x ) , 1 ) , M_\varphi= (T^2 \times[0,1])/(x,0) \sim(\varphi(x),1), M φ = ( T 2 × [ 0 , 1 ]) / ( x , 0 ) ∼ ( φ ( x ) , 1 ) ,
see Figure 5 b.
In order to obtain an elliptic fibration, we fix a zero-section σ 0 : D → X \sigma_0: D \to X σ 0 : D → X . Using the mapping torus description of ∂ X \partial X ∂ X , we define σ 0 \sigma_0 σ 0 over ∂ D \partial D ∂ D , then find an explicit extension. Pick x ∈ T 2 − R x \in T^2 - R x ∈ T 2 − R . Define σ 0 ′ : [ 0 , 1 ] → M φ \sigma'_0: [0,1] \to M_\varphi σ 0 ′ : [ 0 , 1 ] → M φ by σ 0 ′ ( s ) = [ ( x , s ) ] \sigma'_0(s) = [(x,s)] σ 0 ′ ( s ) = [( x , s )] . Since x ∈ T 2 − R x \in T^2 - R x ∈ T 2 − R , it follows φ ( x ) = x \varphi(x) = x φ ( x ) = x and thus σ 0 ′ ( 0 ) = σ 0 ′ ( 1 ) \sigma'_0(0) = \sigma'_0(1) σ 0 ′ ( 0 ) = σ 0 ′ ( 1 ) . Hence, σ 0 ′ \sigma'_0 σ 0 ′ induces a map σ 0 ′ : ∂ D → M φ \sigma_0': \partial D \to M_\varphi σ 0 ′ : ∂ D → M φ . Composing with the diffeomorphism M φ → ∂ X M_\varphi\to\partial X M φ → ∂ X gives a section σ 0 : ∂ D → ∂ X \sigma_0: \partial D \to\partial X σ 0 : ∂ D → ∂ X . This section picks out “the same” point in each fiber, which is away from the vanishing cycle. Thus, we can extend it radially to D D D . Since σ 0 ∣ ∂ D \sigma_0|_{\partial D} σ 0 ∣ ∂ D never meets the vanishing cycle, σ 0 ( 0 ) \sigma_0(0) σ 0 ( 0 ) will not meet the node of X 0 X_0 X 0 . Hence, σ 0 ( 0 ) ∈ X 0 # \sigma_0(0) \in X_0^\# σ 0 ( 0 ) ∈ X 0 # .3 Thus, σ 0 : D → X \sigma_0: D \to X σ 0 : D → X is a section of π \pi π .
We define a section σ : ∂ D → ∂ X \sigma: \partial D \to\partial X σ : ∂ D → ∂ X and show it does not extend to D D D (see Figure 5 ). Choose a parametrization β : [ 0 , 1 ] → T 2 \beta: [0,1] \to T^2 β : [ 0 , 1 ] → T 2 such that β ( 0 ) = β ( 1 ) ∈ T 2 − R \beta(0) = \beta(1) \in T^2 - R β ( 0 ) = β ( 1 ) ∈ T 2 − R . Define σ : [ 0 , 1 ] → M φ \sigma: [0,1] \to M_\varphi σ : [ 0 , 1 ] → M φ , σ ( s ) = [ ( β ( s ) , s ) ] \sigma(s) = [(\beta(s),s)] σ ( s ) = [( β ( s ) , s )] . Since β ( 0 ) ∈ T 2 − R \beta(0) \in T^2 - R β ( 0 ) ∈ T 2 − R , it is fixed by φ \varphi φ . Thus,
σ ( 0 ) = [ ( β ( 0 ) , 0 ) ] = [ ( φ ( β ( 0 ) ) , 1 ) ] = [ ( β ( 0 ) , 1 ) ] = [ ( β ( 1 ) , 1 ) ] = σ ( 1 ) . \sigma(0) = [(\beta(0),0)] = [(\varphi(\beta(0)),1)] = [(\beta(0),1)] = [(\beta(1),1)] = \sigma(1). σ ( 0 ) = [( β ( 0 ) , 0 )] = [( φ ( β ( 0 )) , 1 )] = [( β ( 0 ) , 1 )] = [( β ( 1 ) , 1 )] = σ ( 1 ) .
Hence, this induces a map σ : ∂ D → M φ \sigma: \partial D \to M_\varphi σ : ∂ D → M φ . Composing it with the diffeomorphism M φ → ∂ X M_\varphi\to\partial X M φ → ∂ X defines a section of π : ∂ X → ∂ D \pi: \partial X \to\partial D π : ∂ X → ∂ D .
The map ψ \psi ψ takes [ σ ] [\sigma] [ σ ] to the loop [ β ] ∈ H 1 ( X 0 ) [\beta] \in H_1(X_0) [ β ] ∈ H 1 ( X 0 ) . Recall that α \alpha α is the vanishing cycle, so [ β ] [\beta] [ β ] is the generator of H 1 ( X 0 ) ≅ Z H_1(X_0) \cong\mathbb{Z} H 1 ( X 0 ) ≅ Z . By Remark 4.3, σ \sigma σ cannot extend over the whole disk, since [ β ] [\beta] [ β ] is non-trivial in H 1 ( X 0 ) H_1(X_0) H 1 ( X 0 ) .
Computation of MW()
In the setup of an elliptic fibration over a disk with only one singular fiber, choosing the isotopy class of a section is equivalent to choosing a multiplicity one component of the singular fiber. We make this more explicit in the following proposition.
Proposition 4.6 (Computation of MW(π \pi π )). Let π : X → D \pi: X \to D π : X → D be an elliptic fibration over a disk with only one singular fiber at 0 0 0 . Let X 0 # X_0^{\#} X 0 # be the smooth locus of X 0 X_0 X 0 and let G ( X 0 ) : = π 0 ( X 0 # ) G(X_0) := \pi_0(X_0^{\#}) G ( X 0 ) := π 0 ( X 0 # ) be the group of components of the regular part of the singular fiber X 0 X_0 X 0 and let Γ s m ( π ) \Gamma^{\mathrm{sm}}(\pi) Γ sm ( π ) denote the group of smooth sections of π \pi π , where we choose σ 0 \sigma_0 σ 0 to be the identity element. There is a homomorphism φ : Γ s m ( π ) → G ( X 0 ) \varphi: \Gamma^{\mathrm{sm}}(\pi) \to G(X_0) φ : Γ sm ( π ) → G ( X 0 ) defined as the composition
Γ s m ( π ) ⟶ X 0 # ⟶ G ( X 0 ) \Gamma^{\mathrm{sm}}(\pi) \longrightarrow X_0^{\#} \longrightarrow G(X_0) Γ sm ( π ) ⟶ X 0 # ⟶ G ( X 0 ) where the first map evaluates a section σ : D → X \sigma: D \to X σ : D → X at 0 0 0 and the second is projection X 0 # → π 0 ( X 0 # ) X_0^{\#} \to\pi_0(X_0^{\#}) X 0 # → π 0 ( X 0 # ) .
Furthermore, φ \varphi φ induces an isomorphism
φ ‾ : MW ( π ) → ≅ G ( X 0 ) . \overline{\varphi} : \operatorname{MW}(\pi) \xrightarrow{\cong} G(X_0). φ : MW ( π ) ≅ G ( X 0 ) .
Proof. φ \varphi φ is well-defined. Consider a section σ : D → X \sigma: D \to X σ : D → X . By definition, π ∘ σ = id D \pi\circ\sigma= \operatorname{id}_D π ∘ σ = id D , so the chain rule implies that d π 0 \mathrm{d}\pi_0 d π 0 has full rank. Thus, σ ( 0 ) ∈ X 0 # \sigma(0) \in X_0^{\#} σ ( 0 ) ∈ X 0 # , so φ \varphi φ is well-defined. Furthermore, φ \varphi φ is a group homomorphism, as a composition of group homomorphisms.
φ \varphi φ does not depend on the isotopy representative. Given two isotopic sections σ , σ 1 : D → X \sigma,\sigma^1 : D \to X σ , σ 1 : D → X , there exists a one-parameter family of sections σ t : D → X \sigma^t : D \to X σ t : D → X with σ 0 = σ \sigma^0 = \sigma σ 0 = σ , for t ∈ [ 0 , 1 ] t \in[0,1] t ∈ [ 0 , 1 ] . As we showed above, σ t ( 0 ) ∈ X 0 # \sigma^t(0) \in X_0^{\#} σ t ( 0 ) ∈ X 0 # . By continuity in t t t , it follows that σ t ( 0 ) \sigma^t(0) σ t ( 0 ) lies in the same connected component of X 0 # X_0^{\#} X 0 # for all t t t . In particular, σ \sigma σ and σ 1 \sigma^1 σ 1 intersect the same irreducible component of X 0 X_0 X 0 , inducing a homomorphism MW ( π ) → G ( X 0 ) \operatorname{MW}(\pi) \to G(X_0) MW ( π ) → G ( X 0 ) .
φ \varphi φ is surjective. Let C i ∈ G ( X 0 ) C_i \in G(X_0) C i ∈ G ( X 0 ) be a component of X 0 X_0 X 0 of multiplicity 1 1 1 and pick a regular point x ∈ C i x \in C_i x ∈ C i . Since π \pi π is a submersion at x x x there exist local coordinates around x ∈ X x \in X x ∈ X and 0 ∈ D 0 \in D 0 ∈ D such that π \pi π is the projection ( z , w ) ↦ z (z,w) \mapsto z ( z , w ) ↦ z . In these coordinates, define a section σ ( z ) = ( z , 0 ) \sigma(z) = (z,0) σ ( z ) = ( z , 0 ) . Let D ε ⊂ D D_\varepsilon\subset D D ε ⊂ D be an open disk centered at the origin, completely contained in the coordinate chart on D D D chosen above. Let X ε : = π − 1 ( D ε ) X_\varepsilon:= \pi^{-1}(D_\varepsilon) X ε := π − 1 ( D ε ) . Then π : X − X ε → D − D ε \pi: X-X_\varepsilon\to D-D_\varepsilon π : X − X ε → D − D ε is a torus-bundle and σ ∣ ∂ D ε \sigma|_{\partial D_\varepsilon} σ ∣ ∂ D ε is a well-defined section over ∂ D ε \partial D_\varepsilon ∂ D ε . Since the annulus D − D ε D-D_\varepsilon D − D ε strong deformation retracts to ∂ D ε \partial D_\varepsilon ∂ D ε , the bundle X − X ε → D − D ε X-X_\varepsilon\to D-D_\varepsilon X − X ε → D − D ε is isomorphic to the pullback of π − 1 ( ∂ D ε ) → ∂ D ε \pi^{-1}(\partial D_\varepsilon) \to\partial D_\varepsilon π − 1 ( ∂ D ε ) → ∂ D ε along the retraction. Therefore, σ ∣ ∂ D ε \sigma|_{\partial D_\varepsilon} σ ∣ ∂ D ε can be extended to a section over the entire annulus, yielding a section σ : D → X \sigma: D \to X σ : D → X .
φ \varphi φ is injective. Let σ : D → X \sigma: D \to X σ : D → X be a section intersecting the zero-component C 0 C_0 C 0 of X 0 X_0 X 0 . We first use a flow argument to isotope σ \sigma σ to a section that meets X 0 X_0 X 0 at σ 0 ( 0 ) \sigma_0(0) σ 0 ( 0 ) . Then we use the fact that π \pi π is a submersion on the smooth locus of X X X to conclude.
Let C 0 # C_0^{\#} C 0 # denote the zero-component with singular points removed. By Kodaira’s classification, the fact that X 0 X_0 X 0 is singular implies that C 0 # C_0^{\#} C 0 # is diffeomorphic to C \mathbb{C} C or C × \mathbb{C}^{\times} C × . In particular, it is path-connected, so there exists a path γ : [ 0 , 1 ] → C 0 # \gamma: [0,1] \to C_0^{\#} γ : [ 0 , 1 ] → C 0 # with γ ( 0 ) = σ ( 0 ) \gamma(0)=\sigma(0) γ ( 0 ) = σ ( 0 ) and γ ( 1 ) = σ 0 ( 0 ) \gamma(1)=\sigma_0(0) γ ( 1 ) = σ 0 ( 0 ) . Assume that γ \gamma γ is an embedding and choose a compactly supported vector field v v v on C 0 # C_0^{\#} C 0 # such that γ ′ ( t ) = v γ ( t ) \gamma'(t)=v_{\gamma(t)} γ ′ ( t ) = v γ ( t ) , for all t ∈ [ 0 , 1 ] t \in[0,1] t ∈ [ 0 , 1 ] . The vector field v v v can be smoothly extended to a compactly supported vector field V ~ \widetilde{V} V on an open neighborhood W ⊂ X # W \subset X^{\#} W ⊂ X # . We extend V V V to the entire X # X^{\#} X # by setting it equal to $0 everywhere outside W W W . Let T V X # : = ker ( d π ) T_VX^{\#}:=\ker(\mathrm{d}\pi) T V X # := ker ( d π ) be the vertical tangent bundle. Fix a Riemannian metric on the manifold X # X^{\#} X # and let V ~ x \widetilde{V}_x V x denote the orthogonal projection of V x V_x V x to T x V X # T_xV X^{\#} T x V X # . Recall that we defined v v v as a vector field on C 0 # ⊂ X 0 # C_0^{\#} \subset X_0^{\#} C 0 # ⊂ X 0 # , so d π ( v ) = 0 \mathrm{d}\pi(v)=0 d π ( v ) = 0 , meaning v ∈ T v X # v \in T_vX^{\#} v ∈ T v X # . Thus, V ~ ∣ C 0 # = v \widetilde{V}|_{C_0^{\#}}=v V ∣ C 0 # = v .
Integrating the compactly supported vector field V ~ \widetilde{V} V gives a global flow Φ t : X # → X # \Phi_t:X^{\#}\to X^{\#} Φ t : X # → X # . For arbitrary t ∈ [ 0 , 1 ] t \in[0,1] t ∈ [ 0 , 1 ] , we have
d d t ( π ∘ Φ t ( x ) ) = d π Φ t ( x ) ( d d t Φ t ( x ) ) = d π Φ t ( x ) ( V ~ Φ t ( x ) ) = 0. \frac{d}{dt}\left(\pi\circ\Phi_t(x)\right)
=\mathrm{d}\pi_{\Phi_t(x)}\left(\frac{d}{dt}\Phi_t(x)\right)
=\mathrm{d}\pi_{\Phi_t(x)}\left(\widetilde{V}_{\Phi_t(x)}\right)=0. d t d ( π ∘ Φ t ( x ) ) = d π Φ t ( x ) ( d t d Φ t ( x ) ) = d π Φ t ( x ) ( V Φ t ( x ) ) = 0.
Thus, π ∘ Φ t ( x ) \pi\circ\Phi_t(x) π ∘ Φ t ( x ) is constant in t t t , meaning π ∘ Φ t ( x ) = π ∘ Φ 0 ( x ) = π ( x ) \pi\circ\Phi_t(x) = \pi\circ\Phi_0(x) = \pi(x) π ∘ Φ t ( x ) = π ∘ Φ 0 ( x ) = π ( x ) . Hence, Φ t \Phi_t Φ t maps each fiber to itself. In particular, it maps sections to sections. Let σ ~ : D → X \widetilde{\sigma}: D \to X σ : D → X be defined by σ ~ : = Φ 1 ∘ σ \widetilde{\sigma} := \Phi_1 \circ\sigma σ := Φ 1 ∘ σ . This is a section of π \pi π with σ ~ ( 0 ) = Φ 1 ( σ ( 0 ) ) = σ 0 ( 0 ) \widetilde{\sigma}(0) = \Phi_1(\sigma(0)) = \sigma_0(0) σ ( 0 ) = Φ 1 ( σ ( 0 )) = σ 0 ( 0 ) , by definition of the vector field v v v . Define an isotopy H : D × [ 0 , 1 ] → X H : D \times[0,1] \to X H : D × [ 0 , 1 ] → X by setting H ( s , t ) = Φ t ( σ ( s ) ) H(s,t) = \Phi_t(\sigma(s)) H ( s , t ) = Φ t ( σ ( s )) . Thus, σ \sigma σ and σ ~ \widetilde{\sigma} σ are isotopic sections.
It remains to show that σ ~ \widetilde{\sigma} σ and σ 0 \sigma_0 σ 0 are isotopic. Let p : = σ 0 ( 0 ) = σ ~ ( 0 ) p := \sigma_0(0) = \widetilde{\sigma}(0) p := σ 0 ( 0 ) = σ ( 0 ) . This is a regular point, so by the local submersion theorem, there exists a chart U U U on X X X around p p p and D ε D_\varepsilon D ε on D D D around 0 0 0 , such that in this chart, π \pi π is just a projection. We can define an isotopy over D ε D_\varepsilon D ε using a straight-line homotopy in the local chart. Now observe that the obstruction to extending an isotopy over the annulus D − D ε D-D_\varepsilon D − D ε lies in H k ( D − D ε , ∂ D ε ; π k ( T 2 ) ) H^k(D-D_\varepsilon,\partial D_\varepsilon;\pi_k(T^2)) H k ( D − D ε , ∂ D ε ; π k ( T 2 )) , which is trivial since the annulus D − D ε D-D_\varepsilon D − D ε strong deformation retracts to ∂ D ε \partial D_\varepsilon ∂ D ε . By [13 Theorem 34.6] , the isotopy over ∂ D ε \partial D_\varepsilon ∂ D ε extends over the entire annulus D − D ε D-D_\varepsilon D − D ε .
Corollary 4.7. If π : X → D \pi: X \to D π : X → D is an elliptic fibration with only one singular fiber, then MW ( π ) \operatorname{MW}(\pi) MW ( π ) is finite.
Proof. By Proposition 4.6, MW ( π ) ≅ G ( X 0 ) \operatorname{MW}(\pi) \cong G(X_0) MW ( π ) ≅ G ( X 0 ) , which is finite by Kodaira’s classification.
Explicit Computation of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ )
We give a homological characterization of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) , identifying it with the group of monodromy coinvariants.
Fix a basepoint t ∈ ∂ D t \in\partial D t ∈ ∂ D . Let γ \gamma γ be a counterclockwise generator for π 1 ( ∂ D , t ) \pi_1(\partial D,t) π 1 ( ∂ D , t ) . Let f ∈ Mod ( X t ) f \in\operatorname{Mod}(X_t) f ∈ Mod ( X t ) be the monodromy transformation corresponding to the loop γ \gamma γ . We show that the homomorphism
η : MW ( π ∘ ) ⟶ H 1 ( ∂ X ) , \eta: \operatorname{MW}(\pi^\circ) \longrightarrow H_1(\partial X), η : MW ( π ∘ ) ⟶ H 1 ( ∂ X ) ,
[ σ ] ⟼ [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ] [\sigma] \longmapsto[\sigma|_{\partial D}] - [\sigma_0|_{\partial D}] [ σ ] ⟼ [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ]
is injective, identifying MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) with a specific subgroup of H 1 ( ∂ X ) H_1(\partial X) H 1 ( ∂ X ) . The following lemma also shows that H 1 ( ∂ X ) H_1(\partial X) H 1 ( ∂ X ) consists of “vertical elements” (elements in MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) ) and “horizontal elements” (elements of H 1 ( S 1 ) H_1(S^1) H 1 ( S 1 ) ).
Lemma 4.8 (Computation of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) ). ** Let π : X → D \pi: X \to D π : X → D be an elliptic fibration over a disk with only one singular fiber at 0 0 0 and monodromy f ∈ Mod ( X t ) f \in\operatorname{Mod}(X_t) f ∈ Mod ( X t ) . The Mordell–Weil group of π ∘ \pi^\circ π ∘ fits into the following short exact sequence
0 ⟶ MW ( π ∘ ) → η H 1 ( ∂ X ) → π ∗ H 1 ( ∂ D ) ⟶ 0. (3) 0 \longrightarrow\operatorname{MW}(\pi^\circ) \xrightarrow{\eta} H_1(\partial X) \xrightarrow{\pi_*} H_1(\partial D) \longrightarrow0. \tag*{(3)} 0 ⟶ MW ( π ∘ ) η H 1 ( ∂ X ) π ∗ H 1 ( ∂ D ) ⟶ 0. (3) Furthermore,
MW ( π ∘ ) ≅ H 1 ( X t ) ( I − f ∗ ) H 1 ( X t ) ≅ Z 2 / ( I − f ∗ ) Z 2 . \operatorname{MW}(\pi^\circ) \cong\frac{H_1(X_t)}{(I-f_*)H_1(X_t)} \cong\mathbb{Z}^2/(I-f_*)\mathbb{Z}^2. MW ( π ∘ ) ≅ ( I − f ∗ ) H 1 ( X t ) H 1 ( X t ) ≅ Z 2 / ( I − f ∗ ) Z 2 .
Proof. Let F : = [ X t ] ∈ H 2 ( X ∘ ) F := [X_t] \in H_2(X^\circ) F := [ X t ] ∈ H 2 ( X ∘ ) denote the fiber class of π ∘ \pi^\circ π ∘ and let H 2 ( X ∘ ) F H^2(X^\circ)^F H 2 ( X ∘ ) F denote the annihilator of F F F . By Proposition 3.2, there exists an isomorphism MW ( π ∘ ) → H 2 ( X ∘ ) F \operatorname{MW}(\pi^\circ) \to H^2(X^\circ)^F MW ( π ∘ ) → H 2 ( X ∘ ) F , given by [ σ ] ↦ PD [ σ ] − PD [ σ 0 ] [\sigma] \mapsto\operatorname{PD}[\sigma] - \operatorname{PD}[\sigma_0] [ σ ] ↦ PD [ σ ] − PD [ σ 0 ] . Since X ∘ X^\circ X ∘ strong deformation retracts onto ∂ X \partial X ∂ X , restriction gives an isomorphism H 2 ( X ∘ ) F → H 2 ( ∂ X ) F H^2(X^\circ)^F \to H^2(\partial X)^F H 2 ( X ∘ ) F → H 2 ( ∂ X ) F . Poincaré duality on the closed oriented three-manifold ∂ X \partial X ∂ X gives an isomorphism PD ∂ X : H 2 ( ∂ X ) → H 1 ( ∂ X ) \operatorname{PD}_{\partial X} : H^2(\partial X) \to H_1(\partial X) PD ∂ X : H 2 ( ∂ X ) → H 1 ( ∂ X ) . Thus, composing these maps gives an inclusion
MW ( π ∘ ) ↪ H 1 ( ∂ X ) , \operatorname{MW}(\pi^\circ) \hookrightarrow H_1(\partial X), MW ( π ∘ ) ↪ H 1 ( ∂ X ) ,
[ σ ] ⟼ [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ] . [\sigma] \longmapsto[\sigma|_{\partial D}] - [\sigma_0|_{\partial D}]. [ σ ] ⟼ [ σ ∣ ∂ D ] − [ σ 0 ∣ ∂ D ] .
The image of this inclusion is equal to the image of H 2 ( ∂ X ) F H^2(\partial X)^F H 2 ( ∂ X ) F under Poincaré duality. A cohomology class α ∈ H 2 ( ∂ X ) \alpha\in H^2(\partial X) α ∈ H 2 ( ∂ X ) lies in the annihilator of the fiber class F F F if and only if 0 = ⟨ α , F ⟩ = PD ∂ X ( α ) ⋅ F 0 = \langle\alpha,F\rangle= \operatorname{PD}_{\partial X}(\alpha)\cdot F 0 = ⟨ α , F ⟩ = PD ∂ X ( α ) ⋅ F , where ⋅ \cdot ⋅ denotes the algebraic intersection number. Hence,
PD ∂ X ( H 2 ( ∂ X ) F ) = { a ∈ H 1 ( ∂ X ) ∣ a ⋅ F = 0 } . \operatorname{PD}_{\partial X}\bigl(H^2(\partial X)^F\bigr) = \{a \in H_1(\partial X) \mid a \cdot F = 0\}. PD ∂ X ( H 2 ( ∂ X ) F ) = { a ∈ H 1 ( ∂ X ) ∣ a ⋅ F = 0 } .
Consider the Wang exact sequence for the fiber bundle X t → ∂ X → S 1 X_t \to\partial X \to S^1 X t → ∂ X → S 1
⋯ ⟶ H 1 ( X t ) → I − f ∗ H 1 ( X t ) ⟶ H 1 ( ∂ X ) → ∂ H 0 ( X t ) → I − f ∗ H 0 ( X t ) ⟶ ⋯ (4) \cdots\longrightarrow H_1(X_t) \xrightarrow{I-f_*} H_1(X_t) \longrightarrow H_1(\partial X) \xrightarrow{\partial} H_0(X_t) \xrightarrow{I-f_*} H_0(X_t) \longrightarrow\cdots \tag*{(4)} ⋯ ⟶ H 1 ( X t ) I − f ∗ H 1 ( X t ) ⟶ H 1 ( ∂ X ) ∂ H 0 ( X t ) I − f ∗ H 0 ( X t ) ⟶ ⋯ (4)
The monodromy f f f acts as the identity on H 0 ( X t ) H_0(X_t) H 0 ( X t ) , so the map H 0 ( X t ) → I − f ∗ H 0 ( X t ) H_0(X_t) \xrightarrow{I-f_*} H_0(X_t) H 0 ( X t ) I − f ∗ H 0 ( X t ) in the long exact sequence (4) is zero. Thus, we obtain a short exact sequence
0 → H 1 ( X t ) ( I − f ∗ ) H 1 ( X t ) → H 1 ( ∂ X ) → ∂ H 0 ( X t ) → 0. (5) 0 \to\frac{H_1(X_t)}{(I-f_*)H_1(X_t)} \to H_1(\partial X) \xrightarrow{\partial} H_0(X_t) \to0. \tag*{(5)} 0 → ( I − f ∗ ) H 1 ( X t ) H 1 ( X t ) → H 1 ( ∂ X ) ∂ H 0 ( X t ) → 0. (5)
The boundary map H 1 ( ∂ X ) → ∂ H 0 ( X t ) H_1(\partial X) \xrightarrow{\partial} H_0(X_t) H 1 ( ∂ X ) ∂ H 0 ( X t ) is precisely the algebraic intersection number with the class [ X t ] ∈ H 2 ( ∂ X ) [X_t] \in H_2(\partial X) [ X t ] ∈ H 2 ( ∂ X ) . Hence, the image of H 2 ( ∂ X ) F H^2(\partial X)^F H 2 ( ∂ X ) F under Poincaré duality in ∂ X \partial X ∂ X is equal to the kernel of H 1 ( ∂ X ) → ∂ H 0 ( X t ) H_1(\partial X) \xrightarrow{\partial} H_0(X_t) H 1 ( ∂ X ) ∂ H 0 ( X t ) . Therefore,
MW ( π ∘ ) ≅ H 2 ( X ∘ ) F ≅ PD ∂ X ( H 2 ( ∂ X ) F ) = = ker ( H 1 ( ∂ X ) → ∂ H 0 ( X t ) ) ≅ H 1 ( X t ) ( I − f ∗ ) H 1 ( X t ) ≅ Z 2 / ( I − f ∗ ) Z 2 . \begin{aligned}
\operatorname{MW}(\pi^\circ) \cong H^2(X^\circ)^F \cong\operatorname{PD}_{\partial X}(H^2(\partial X)^F) = \\
&= \ker(H_1(\partial X) \xrightarrow{\partial} H_0(X_t)) \cong\frac{H_1(X_t)}{(I-f_*)H_1(X_t)} \cong\mathbb{Z}^2/(I-f_*)\mathbb{Z}^2.
\end{aligned} MW ( π ∘ ) ≅ H 2 ( X ∘ ) F ≅ PD ∂ X ( H 2 ( ∂ X ) F ) = = ker ( H 1 ( ∂ X ) ∂ H 0 ( X t )) ≅ ( I − f ∗ ) H 1 ( X t ) H 1 ( X t ) ≅ Z 2 / ( I − f ∗ ) Z 2 .
We finish the proof by showing that the short exact sequence (5) implies exactness of the short exact sequence (3) . As explained before, the map ∂ : H 1 ( ∂ X ) → H 0 ( X t ) ≅ Z \partial: H_1(\partial X) \to H_0(X_t) \cong\mathbb{Z} ∂ : H 1 ( ∂ X ) → H 0 ( X t ) ≅ Z is the algebraic intersection number with the class [ X t ] ∈ H 2 ( ∂ X ) [X_t] \in H_2(\partial X) [ X t ] ∈ H 2 ( ∂ X ) . This is equivalent to saying that ∂ \partial ∂ measures how many times a homology class winds around the circle ∂ D \partial D ∂ D . Hence, under the canonical identifications H 0 ( X t ) ≅ Z H_0(X_t) \cong\mathbb{Z} H 0 ( X t ) ≅ Z and H 1 ( ∂ D ) ≅ Z H_1(\partial D) \cong\mathbb{Z} H 1 ( ∂ D ) ≅ Z , we get ∀ c ∈ H 1 ( ∂ X ) \forall c \in H_1(\partial X) ∀ c ∈ H 1 ( ∂ X ) , ∂ c = c ⋅ [ X t ] = ( π ∣ ∂ X ) ∗ ( c ) \partial c = c \cdot[X_t] = (\pi|_{\partial X})_*(c) ∂ c = c ⋅ [ X t ] = ( π ∣ ∂ X ) ∗ ( c ) . Hence, ∂ \partial ∂ can be replaced with ( π ∣ ∂ X ) ∗ : H 1 ( ∂ X ) → H 1 ( ∂ D ) ≅ Z (\pi|_{\partial X})_* : H_1(\partial X) \to H_1(\partial D) \cong\mathbb{Z} ( π ∣ ∂ X ) ∗ : H 1 ( ∂ X ) → H 1 ( ∂ D ) ≅ Z .
Corollary 4.9. Let π : X → D \pi: X \to D π : X → D be an elliptic fibration with only one singular fiber at the origin. The singular fiber X 0 X_0 X 0 is additive if and only if MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) is finite.
Proof. By Lemma 4.8, MW ( π ∘ ) ≅ Z 2 / ( I − f ∗ ) Z 2 \operatorname{MW}(\pi^\circ) \cong\mathbb{Z}^2/(I-f_*)\mathbb{Z}^2 MW ( π ∘ ) ≅ Z 2 / ( I − f ∗ ) Z 2 . This group is finite if and only if det ( I − f ∗ ) ≠ 0 \det(I-f_*) \ne0 det ( I − f ∗ ) = 0 . Thus, it suffices to show that 1 1 1 is an eigenvalue of f ∗ : H 1 ( X t ) → H 1 ( X t ) f_* : H_1(X_t) \to H_1(X_t) f ∗ : H 1 ( X t ) → H 1 ( X t ) if and only if X 0 X_0 X 0 is not additive. The determinant of f ∗ f_* f ∗ is 1 1 1 , so if 1 1 1 is an eigenvalue of f ∗ f_* f ∗ , then both eigenvalues must equal 1 1 1 . Therefore, tr ( f ∗ ) = 2 \operatorname{tr}(f_*) = 2 tr ( f ∗ ) = 2 . By Kodaira’s classification, the trace of the monodromy is 2 2 2 if and only if X 0 X_0 X 0 is smooth or multiplicative.
Injectivity of the restriction map MW ( π ) → MW ( π ∘ ) \operatorname{MW}(\pi) \to\operatorname{MW}(\pi^\circ) MW ( π ) → MW ( π ∘ )
We show that, if two sections of π \pi π are isotopic over ∂ D \partial D ∂ D , then they must be isotopic over D D D .
Proposition 4.10. Let π : X → D \pi: X \to D π : X → D be an elliptic fibration over a disk D D D with only one singular fiber at the origin. Then the homomorphism MW ( π ) → MW ( π ∘ ) \operatorname{MW}(\pi) \to\operatorname{MW}(\pi^\circ) MW ( π ) → MW ( π ∘ ) given by restricting sections to D ∘ D^\circ D ∘ is injective.
Proof. Let σ : D → X \sigma: D \to X σ : D → X be a section of π \pi π such that σ ∣ ∂ D ≃ σ 0 ∣ ∂ D \sigma|_{\partial D} \simeq\sigma_0|_{\partial D} σ ∣ ∂ D ≃ σ 0 ∣ ∂ D . By Proposition 4.6, σ \sigma σ and σ 0 \sigma_0 σ 0 are isotopic over D D D if and only if they intersect the same component of X 0 X_0 X 0 . Let us assume that they intersect different components of X 0 X_0 X 0 . Denote the irreducible components of X 0 X_0 X 0 by C 0 , … , C r C_0, \ldots, C_r C 0 , … , C r and assume that σ 0 \sigma_0 σ 0 intersects C 0 C_0 C 0 and σ \sigma σ intersects C a C_a C a for a ≠ 0 a \ne0 a = 0 . Since sections intersect each fiber with multiplicity 1 1 1 , C a C_a C a must be a multiplicity 1 1 1 component of X 0 X_0 X 0 . Let − σ ( D ) -\sigma(D) − σ ( D ) be σ ( D ) \sigma(D) σ ( D ) with reversed orientation. The algebraic intersection number satisfies − σ ( D ) ⋅ [ X 0 ] = − 1 -\sigma(D) \cdot[X_0] = -1 − σ ( D ) ⋅ [ X 0 ] = − 1 . The isotopy between σ ∣ ∂ D \sigma|_{\partial D} σ ∣ ∂ D and σ 0 ∣ ∂ D \sigma_0|_{\partial D} σ 0 ∣ ∂ D traces out an annulus Y Y Y in ∂ X \partial X ∂ X , see Figure 6 . Since ∂ σ 0 ( D ) \partial\sigma_0(D) ∂ σ 0 ( D ) and ∂ ( − σ ( D ) ) \partial(-\sigma(D)) ∂ ( − σ ( D )) have opposite orientation in ∂ X \partial X ∂ X , they can be glued to the respective boundaries of Y Y Y , yielding the closed surface S : = σ 0 ( D ) ∪ ( − σ ( D ) ) ∪ Y S := \sigma_0(D)\cup(-\sigma(D))\cup Y S := σ 0 ( D ) ∪ ( − σ ( D )) ∪ Y . This defines a homology class [ S ] ∈ H 2 ( X ) [S] \in H_2(X) [ S ] ∈ H 2 ( X ) . Since H 2 ( X ) ≅ H 2 ( X 0 ) H_2(X) \cong H_2(X_0) H 2 ( X ) ≅ H 2 ( X 0 ) , which is freely generated by the irreducible components of X 0 X_0 X 0 , there exist x i ∈ Z x_i \in\mathbb{Z} x i ∈ Z such that [ S ] = ∑ x i [ C i ] [S] = \sum x_i[C_i] [ S ] = ∑ x i [ C i ] . Since Y ⊂ ∂ X Y \subset\partial X Y ⊂ ∂ X , it does not intersect X 0 X_0 X 0 . This gives the following system of equations:
Figure 6. Two isotopic sections σ \sigma σ , σ 0 \sigma_0 σ 0 trace out an annulus Y Y Y in ∂ X \partial X ∂ X .
1 = [ S ] ⋅ [ C 0 ] = ∑ x i [ C i ] [ C 0 ] − 1 = [ S ] ⋅ [ C a ] = ∑ x i [ C i ] [ C a ] 0 = [ S ] ⋅ [ C j ] = ∑ x i [ C i ] [ C j ] , for j ≠ 0 , a . \begin{aligned}
1 &= [S]\cdot[C_0] = \sum x_i[C_i][C_0]\\
-1 &= [S]\cdot[C_a] = \sum x_i[C_i][C_a]\\
0 &= [S]\cdot[C_j] = \sum x_i[C_i][C_j],\quad\text{for }j\ne0,a.
\end{aligned} 1 − 1 0 = [ S ] ⋅ [ C 0 ] = ∑ x i [ C i ] [ C 0 ] = [ S ] ⋅ [ C a ] = ∑ x i [ C i ] [ C a ] = [ S ] ⋅ [ C j ] = ∑ x i [ C i ] [ C j ] , for j = 0 , a .
Let A ~ ∈ M ( r + 1 ) × ( r + 1 ) ( Z ) \widetilde{A}\in M_{(r+1)\times(r+1)}(\mathbb{Z}) A ∈ M ( r + 1 ) × ( r + 1 ) ( Z ) be the extended Cartan matrix associated with the singular fiber X 0 X_0 X 0 .5 The system of equations is equivalent to the matrix equation − A ~ x = e 0 − e a -\widetilde{A}x=e_0-e_a − A x = e 0 − e a , where x = ( x 0 , … , x r ) T x=(x_0,\ldots,x_r)^T x = ( x 0 , … , x r ) T and e 0 e_0 e 0 and e a e_a e a denote the zeroth and a a a -th standard basis vector in R r + 1 \mathbb{R}^{r+1} R r + 1 , respectively. Let A A A be the Cartan matrix obtained by removing the component C 0 C_0 C 0 . We can write
A ~ = ( 2 v T v A ) , \widetilde{A} =
\begin{pmatrix}
2 & v^T\\
v & A
\end{pmatrix}, A = ( 2 v v T A ) ,
where v ∈ Z r v\in\mathbb{Z}^r v ∈ Z r . Let m ~ ∈ Z r + 1 \widetilde{m}\in\mathbb{Z}^{r+1} m ∈ Z r + 1 be the vector of multiplicities of the irreducible components of X 0 X_0 X 0 . By Kodaira’s classification, this vector spans the kernel of A ~ \widetilde{A} A . Since C 0 C_0 C 0 has multiplicity 1, we can write m ~ = ( 1 m ) T \widetilde{m}=(1\quad m)^T m = ( 1 m ) T for m ∈ Z r m\in\mathbb{Z}^r m ∈ Z r . Now, A ~ m ~ = 0 \widetilde{A}\widetilde{m}=0 A m = 0 implies v + A m = 0 v+Am=0 v + A m = 0 . Also, writing x = ( x 0 x ′ ) T x=(x_0\quad x')^T x = ( x 0 x ′ ) T with x ′ ∈ Z r x'\in\mathbb{Z}^r x ′ ∈ Z r in the equation A ~ x = − e 0 + e a \widetilde{A}x=-e_0+e_a A x = − e 0 + e a yields
x 0 v + A x ′ = e ˉ a , x_0v+Ax'=\bar e_a, x 0 v + A x ′ = e ˉ a ,
where e ˉ a \bar e_a e ˉ a denotes the a a a -th standard basis vector in Z r \mathbb{Z}^r Z r . Using v + A m = 0 v+Am=0 v + A m = 0 , this implies
A ( x ′ − x 0 m ) = e ˉ a . (6) A(x'-x_0m)=\bar e_a. \tag*{(6)} A ( x ′ − x 0 m ) = e ˉ a . (6)
The Cartan matrix A A A is invertible, so (6) is equivalent to
x ′ − x 0 m = A − 1 e ˉ a . (7) x'-x_0m=A^{-1}\bar e_a. \tag*{(7)} x ′ − x 0 m = A − 1 e ˉ a . (7)
In what follows, we show that the a a a -th column of the inverse of a Cartan matrix of type ADE cannot be integral. Since x ′ , m ∈ Z r x',m\in\mathbb{Z}^r x ′ , m ∈ Z r and x 0 ∈ Z x_0\in\mathbb{Z} x 0 ∈ Z , this implies that (7) is impossible and gives the desired contradiction.
Recall that a a a corresponds to a non-zero component of multiplicity one, so we only need to check such columns. We do this explicitly, by considering the inverses of Cartan matrices of each type. We check that the columns corresponding to multiplicity 1 components are not integral. All formulas for inverses of Cartan matrices we use below are from [16 ] .
A i , j = { 2 , if i = j , − 1 , if ∣ i − j ∣ = 1 , 0 , otherwise. A_{i,j}=
\begin{cases}
2, & \text{if }i=j,\\
-1, & \text{if }|i-j|=1,\\
0, & \text{otherwise.}
\end{cases} A i , j = ⎩ ⎨ ⎧ 2 , − 1 , 0 , if i = j , if ∣ i − j ∣ = 1 , otherwise.
Its inverse has entries
( A − 1 ) i , j = min ( i , j ) − i j n + 1 , for 1 ≤ i , j ≤ n . (A^{-1})_{i,j}=\min(i,j)-\frac{ij}{n+1},\quad\text{for }1\le i,j\le n. ( A − 1 ) i , j = min ( i , j ) − n + 1 ij , for 1 ≤ i , j ≤ n .
For each 1 ≤ j ≤ n 1\le j\le n 1 ≤ j ≤ n , the first entry of the j j j -th column is 1 − j n + 1 ∉ Z 1-\frac{j}{n+1}\notin\mathbb{Z} 1 − n + 1 j ∈ / Z .
Type D n D_n D n : In this case we assume n ≥ 4 n \ge4 n ≥ 4 . We order the vertices as in Figure 7 . Only the first and the last two components have multiplicity 1 1 1 , so a ∈ { 1 , n − 1 , n } a \in\{1,n-1,n\} a ∈ { 1 , n − 1 , n } . The corresponding Cartan matrix is
Figure 7. Labelling of vertices for Dynkin diagrams.
A = ( 2 − 1 − 1 ⋱ ⋱ ⋱ 2 − 1 − 1 − 1 2 0 − 1 0 2 ) A =
\begin{pmatrix}
2 & -1 & & & & \\
-1 & \ddots& \ddots& & & \\
& \ddots& 2 & -1 & -1 & \\
& & -1 & 2 & 0 & \\
& & -1 & 0 & 2 &
\end{pmatrix} A = 2 − 1 − 1 ⋱ ⋱ ⋱ 2 − 1 − 1 − 1 2 0 − 1 0 2
The matrix is symmetric and so is its inverse, so it suffices to give the entries of the inverse for i ≤ j i \le j i ≤ j :
( A − 1 ) i , j = { i , if 1 ≤ i ≤ j ≤ n − 2 i / 2 , if i < n − 1 , j = n − 1 or n n − 2 4 , if i = n − 1 , j = n n 4 , if i = j = n − 1 or n . (A^{-1})_{i,j} =
\begin{cases}
i, & \text{if } 1 \le i \le j \le n-2 \\
i/2, & \text{if } i < n-1, j=n-1 \text{ or } n \\
\frac{n-2}{4}, & \text{if } i=n-1,j=n \\
\frac{n}{4}, & \text{if } i=j=n-1 \text{ or } n.
\end{cases} ( A − 1 ) i , j = ⎩ ⎨ ⎧ i , i /2 , 4 n − 2 , 4 n , if 1 ≤ i ≤ j ≤ n − 2 if i < n − 1 , j = n − 1 or n if i = n − 1 , j = n if i = j = n − 1 or n .
We start with the column given by j = 1 j=1 j = 1 . By symmetry, we have ( A − 1 ) n , 1 = ( A − 1 ) 1 , n = 1 / 2 (A^{-1})_{n,1}=(A^{-1})_{1,n}=1/2 ( A − 1 ) n , 1 = ( A − 1 ) 1 , n = 1/2 , so this column is not integral. For the columns j = n − 1 j=n-1 j = n − 1 and j = n j=n j = n , the fact that n ≥ 4 n \ge4 n ≥ 4 implies that ( A − 1 ) 1 , n − 1 = ( A − 1 ) 1 , n = 1 / 2 (A^{-1})_{1,n-1}=(A^{-1})_{1,n}=1/2 ( A − 1 ) 1 , n − 1 = ( A − 1 ) 1 , n = 1/2 , so these cannot be integral.
Type E E E :
E 6 E_6 E 6 : If we order the vertices as in Figure 7 , then only the first and sixth component have multiplicity 1 1 1 , so a ∈ { 1 , 6 } a \in\{1,6\} a ∈ { 1 , 6 } . The corresponding Cartan matrix is
A = ( 2 0 − 1 0 0 0 0 2 0 − 1 0 0 − 1 0 2 − 1 0 0 0 − 1 − 1 2 − 1 0 0 0 0 − 1 2 − 1 0 0 0 0 − 1 2 ) . A =
\begin{pmatrix}
2 & 0 & -1 & 0 & 0 & 0 \\
0 & 2 & 0 & -1 & 0 & 0 \\
-1 & 0 & 2 & -1 & 0 & 0 \\
0 & -1 & -1 & 2 & -1 & 0 \\
0 & 0 & 0 & -1 & 2 & -1 \\
0 & 0 & 0 & 0 & -1 & 2
\end{pmatrix}. A = 2 0 − 1 0 0 0 0 2 0 − 1 0 0 − 1 0 2 − 1 0 0 0 − 1 − 1 2 − 1 0 0 0 0 − 1 2 − 1 0 0 0 0 − 1 2 .
We only need to give a non-integral entry in the first column of the inverse and one in the last column of the inverse. ( A − 1 ) 1 , 1 = 4 / 3 (A^{-1})_{1,1}=4/3 ( A − 1 ) 1 , 1 = 4/3 and ( A − 1 ) 1 , 6 = 2 / 3 (A^{-1})_{1,6}=2/3 ( A − 1 ) 1 , 6 = 2/3 , so we are done.
E 7 E_7 E 7 : If we order the vertices as in Figure 7 , only the seventh component has multiplicity 1 1 1 , so a = 7 a=7 a = 7 . Hence, we need to check only the last column of the inverse of the Cartan matrix. ( A − 1 ) 2 , 7 = 3 / 2 (A^{-1})_{2,7}=3/2 ( A − 1 ) 2 , 7 = 3/2 , so we are done.
Section classes extend if and only if they are torsion
Using the description of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) in terms of monodromy coinvariants, we show that a section over ∂ D \partial D ∂ D extends to a section over D D D if and only if it is torsion in MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) .
Lemma 4.11. Let π : X → D \pi:X\to D π : X → D be an elliptic fibration over a disk with one singular fiber at the origin. The image of the restriction map MW ( π ) → MW ( π ∘ ) \operatorname{MW}(\pi)\to\operatorname{MW}(\pi^\circ) MW ( π ) → MW ( π ∘ ) equals MW ( π ∘ ) t o r \operatorname{MW}(\pi^\circ)_{\mathrm{tor}} MW ( π ∘ ) tor .
Proof. By Proposition 4.6, MW ( π ) ≅ G ( X 0 ) \operatorname{MW}(\pi)\cong G(X_0) MW ( π ) ≅ G ( X 0 ) . By Corollary 4.7, MW ( π ) \operatorname{MW}(\pi) MW ( π ) is torsion. Thus, the image of the inclusion must be contained in the torsion part of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) . Furthermore, Lemma 2.5 implies that G ( X 0 ) G(X_0) G ( X 0 ) is isomorphic to the torsion part of the monodromy coinvariants, i.e. G ( X 0 ) ≅ ( Z 2 / ( f ∗ − I ) Z 2 ) t o r G(X_0)\cong\left(\mathbb{Z}^2/(f_*-I)\mathbb{Z}^2\right)_{\mathrm{tor}} G ( X 0 ) ≅ ( Z 2 / ( f ∗ − I ) Z 2 ) tor . Thus, the injection MW ( π ) ↪ MW ( π ∘ ) \operatorname{MW}(\pi)\hookrightarrow\operatorname{MW}(\pi^\circ) MW ( π ) ↪ MW ( π ∘ ) given by Proposition 4.10 becomes an injection ( Z 2 / ( f ∗ − I ) Z 2 ) t o r ↪ MW ( π ∘ ) t o r \left(\mathbb{Z}^2/(f_*-I)\mathbb{Z}^2\right)_{\mathrm{tor}}\hookrightarrow\operatorname{MW}(\pi^\circ)_{\mathrm{tor}} ( Z 2 / ( f ∗ − I ) Z 2 ) tor ↪ MW ( π ∘ ) tor . By Lemma 4.8, the codomain is equal to the domain and since both are finite, the map MW ( π ) → MW ( π ∘ ) t o r \operatorname{MW}(\pi)\to\operatorname{MW}(\pi^\circ)_{\mathrm{tor}} MW ( π ) → MW ( π ∘ ) tor must be a bijection.
Proof of thm: extend sections locally
Proof of Theorem 4.2. Injectivity of the restriction map MW ( π ) → MW ( π ∘ ) \operatorname{MW}(\pi)\to\operatorname{MW}(\pi^\circ) MW ( π ) → MW ( π ∘ ) follows from Proposition 4.10. We distinguish cases based on whether X 0 X_0 X 0 is additive or multiplicative.
Assume X 0 X_0 X 0 is additive. By definition, π 1 ( X 0 ) = 0 \pi_1(X_0)=0 π 1 ( X 0 ) = 0 . Thus, H 1 ( X 0 ) ≅ 0 H_1(X_0)\cong0 H 1 ( X 0 ) ≅ 0 and to prove exactness of the sequence, it suffices to show surjectivity of MW ( π ) → MW ( π ∘ ) \operatorname{MW}(\pi)\to\operatorname{MW}(\pi^\circ) MW ( π ) → MW ( π ∘ ) . By Corollary 4.9, MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) is a finite group. By Lemma 4.11, this implies MW ( π ) → MW ( π ∘ ) \operatorname{MW}(\pi)\to\operatorname{MW}(\pi^\circ) MW ( π ) → MW ( π ∘ ) is surjective, so the sequence is exact.
Assume X 0 X_0 X 0 is multiplicative. By Kodaira’s classification, there exists a basis { α , β } \{\alpha,\beta\} { α , β } of H 1 ( X t ) H_1(X_t) H 1 ( X t ) such that the monodromy f ∈ Mod ( X t ) f\in\operatorname{Mod}(X_t) f ∈ Mod ( X t ) acts on H 1 ( X t ) H_1(X_t) H 1 ( X t ) as f ∗ = ( 1 n 0 1 ) f_*=\begin{pmatrix}1&n\\0&1\end{pmatrix} f ∗ = ( 1 0 n 1 ) .
By Lemma 4.8, η : MW ( π ∘ ) → H 1 ( ∂ X ) \eta:\operatorname{MW}(\pi^\circ)\to H_1(\partial X) η : MW ( π ∘ ) → H 1 ( ∂ X ) is an injection. The zero-section σ 0 ∣ ∂ D : ∂ D → ∂ X \sigma_0|_{\partial D}:\partial D\to\partial X σ 0 ∣ ∂ D : ∂ D → ∂ X induces a splitting of the short exact sequence (3). Hence,
H 1 ( ∂ X ) = η ( MW ( π ∘ ) ) ⊕ ( σ 0 ∣ ∂ D ) ∗ ( H 1 ( ∂ D ) ) . H_1(\partial X)=\eta\left(\operatorname{MW}(\pi^\circ)\right)\oplus(\sigma_0|_{\partial D})_*\left(H_1(\partial D)\right). H 1 ( ∂ X ) = η ( MW ( π ∘ ) ) ⊕ ( σ 0 ∣ ∂ D ) ∗ ( H 1 ( ∂ D ) ) .
Also by Lemma 4.8, it follows
MW ( π ∘ ) ≅ η ( MW ( π ∘ ) ) ≅ H 1 ( X t ) ( I − f ∗ ) H 1 ( X t ) ≅ ( Z / n Z ) ⊕ Z , \operatorname{MW}(\pi^\circ)\cong\eta\left(\operatorname{MW}(\pi^\circ)\right)\cong\frac{H_1(X_t)}{(I-f_*)H_1(X_t)}\cong(\mathbb{Z}/n\mathbb{Z})\oplus\mathbb{Z}, MW ( π ∘ ) ≅ η ( MW ( π ∘ ) ) ≅ ( I − f ∗ ) H 1 ( X t ) H 1 ( X t ) ≅ ( Z / n Z ) ⊕ Z ,
with the ( Z / n Z ) (\mathbb{Z}/n\mathbb{Z}) ( Z / n Z ) -factor generated by α \alpha α and the Z \mathbb{Z} Z -factor generated by β \beta β . (See Figure 8 ). Thus,
Figure 8. Explicit degeneration for a multiplicative fiber of type I 2 I_2 I 2 .
H 1 ( ∂ X ) = ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ ⊕ Z ⟨ γ ⟩ , H_1(\partial X)=(\mathbb{Z}/n\mathbb{Z})\langle\alpha\rangle\oplus\mathbb{Z}\langle\beta\rangle\oplus\mathbb{Z}\langle\gamma\rangle, H 1 ( ∂ X ) = ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ ⊕ Z ⟨ γ ⟩ ,
where γ = σ 0 ( ∂ D ) \gamma=\sigma_0(\partial D) γ = σ 0 ( ∂ D ) . Restricting the codomain to the image of η \eta η gives an isomorphism
η : MW ( π ∘ ) → ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ < H 1 ( ∂ X ) . \eta:\operatorname{MW}(\pi^\circ)\to(\mathbb{Z}/n\mathbb{Z})\langle\alpha\rangle\oplus\mathbb{Z}\langle\beta\rangle<H_1(\partial X). η : MW ( π ∘ ) → ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ < H 1 ( ∂ X ) .
Recall that we defined ψ : MW ( π ∘ ) → H 1 ( X 0 ) \psi:\operatorname{MW}(\pi^\circ)\to H_1(X_0) ψ : MW ( π ∘ ) → H 1 ( X 0 ) as the composition of η \eta η and the map H 1 ( ∂ X ) → H 1 ( X 0 ) H_1(\partial X)\to H_1(X_0) H 1 ( ∂ X ) → H 1 ( X 0 ) . By Picard-Lefschetz theory, α \alpha α is the vanishing cycle of the fibration and thus its homology class vanishes in H 1 ( X 0 ) H_1(X_0) H 1 ( X 0 ) . The loop β \beta β is mapped to a loop on X 0 X_0 X 0 going around the cycle of spheres precisely once, so H 1 ( X 0 ) ≅ Z ⟨ β ⟩ H_1(X_0)\cong\mathbb{Z}\langle\beta\rangle H 1 ( X 0 ) ≅ Z ⟨ β ⟩ . Therefore, the restriction of the map H 1 ( ∂ X ) → H 1 ( X 0 ) H_1(\partial X)\to H_1(X_0) H 1 ( ∂ X ) → H 1 ( X 0 ) to ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ (\mathbb{Z}/n\mathbb{Z})\langle\alpha\rangle\oplus\mathbb{Z}\langle\beta\rangle ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ takes α ↦ 0 \alpha\mapsto0 α ↦ 0 , β ↦ β \beta\mapsto\beta β ↦ β . Therefore, the kernel of this restriction is ( Z / n Z ) ⟨ α ⟩ (\mathbb{Z}/n\mathbb{Z})\langle\alpha\rangle ( Z / n Z ) ⟨ α ⟩ . Hence, ker ( ψ ) = η − 1 ( ( Z / n Z ) ⟨ α ⟩ ) \ker(\psi)=\eta^{-1}((\mathbb{Z}/n\mathbb{Z})\langle\alpha\rangle) ker ( ψ ) = η − 1 (( Z / n Z ) ⟨ α ⟩) .
By Lemma 4.11, a section σ : D ∘ → X ∘ \sigma:D^\circ\to X^\circ σ : D ∘ → X ∘ extends to a section over D D D up to isotopy if and only if it is torsion in MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) . Since η \eta η is injective, [ σ ] ∈ MW ( π ∘ ) [\sigma]\in\operatorname{MW}(\pi^\circ) [ σ ] ∈ MW ( π ∘ ) is torsion if and only if η ( [ σ ] ) ∈ ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ \eta([\sigma])\in(\mathbb{Z}/n\mathbb{Z})\langle\alpha\rangle\oplus\mathbb{Z}\langle\beta\rangle η ([ σ ]) ∈ ( Z / n Z ) ⟨ α ⟩ ⊕ Z ⟨ β ⟩ is torsion. The last statement holds if and only if η ( [ σ ] ) ∈ ( Z / n Z ) ⟨ α ⟩ \eta([\sigma])\in(\mathbb{Z}/n\mathbb{Z})\langle\alpha\rangle η ([ σ ]) ∈ ( Z / n Z ) ⟨ α ⟩ . Thus MW ( π ) = ker ( ψ ) \operatorname{MW}(\pi)=\ker(\psi) MW ( π ) = ker ( ψ ) . Surjectivity of ψ \psi ψ follows since the isotopy class of the section σ : ∂ D → ∂ X \sigma:\partial D\to\partial X σ : ∂ D → ∂ X defined in Example 4.5 is mapped to the generator [ β ] ∈ H 1 ( X 0 ) [\beta]\in H_1(X_0) [ β ] ∈ H 1 ( X 0 ) .
The Smooth Shioda–Tate Isomorphism
In this section, we compute the Mordell–Weil group of an arbitrary elliptic fibration π \pi π over closed base. We start by showing that MW ( π ) \operatorname{MW}(\pi) MW ( π ) can be viewed as a subgroup of MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) .
Proposition 5.1. Let π : M → B \pi: M \to B π : M → B be an elliptic fibration. Then the natural map MW ( π ) → MW ( π ∘ ) \operatorname{MW}(\pi) \to\operatorname{MW}(\pi^\circ) MW ( π ) → MW ( π ∘ ) given by restriction is injective.
Proof. If [ σ ] ∈ MW ( π ) [\sigma] \in\operatorname{MW}(\pi) [ σ ] ∈ MW ( π ) and σ ∣ B ∘ \sigma|_{B^\circ} σ ∣ B ∘ is isotopic to σ 0 ∣ B ∘ \sigma_0|_{B^\circ} σ 0 ∣ B ∘ , applying Proposition 4.10 in a small neighborhood of each critical value gives a local isotopy between the two sections, which can be adjusted to coincide with the original isotopy over B ∘ B^\circ B ∘ , yielding a global isotopy between σ \sigma σ and σ 0 \sigma_0 σ 0 .
A Global Obstruction to Extending Sections
In order to relate MW ( π ) \operatorname{MW}(\pi) MW ( π ) and MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) , we extend the local obstruction from Theorem 4.2 to a global one. Consider an elliptic fibration π : M → B \pi: M \to B π : M → B with critical value set Σ ⊂ B \Sigma\subset B Σ ⊂ B . For t ∈ B t \in B t ∈ B , denote M t : = π − 1 ( t ) M_t := \pi^{-1}(t) M t := π − 1 ( t ) . Let N N N be the closure of M − M ∘ M - M^\circ M − M ∘ in M M M . Define the map Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \Psi: \operatorname{MW}(\pi^\circ) \to\bigoplus_{t\in\Sigma} H_1(M_t) Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) , as the composition of the following maps, which we explain below.
MW ( π ∘ ) → ι H 2 ( M ∘ , ∂ M ∘ ) → ∂ H 1 ( ∂ M ∘ ) → ≅ H 1 ( ∂ N ) → incl ∗ H 1 ( N ) → ≅ H 1 ( ⋃ t ∈ Σ M t ) → ≅ ⨁ t ∈ Σ H 1 ( M t ) . \operatorname{MW}(\pi^\circ) \xrightarrow{\iota} H_2(M^\circ,\partial M^\circ) \xrightarrow{\partial} H_1(\partial M^\circ) \xrightarrow{\cong} H_1(\partial N) \xrightarrow{\operatorname{incl}_*} H_1(N) \xrightarrow{\cong} H_1\left(\bigcup_{t\in\Sigma} M_t\right) \xrightarrow{\cong} \bigoplus_{t\in\Sigma} H_1(M_t). MW ( π ∘ ) ι H 2 ( M ∘ , ∂ M ∘ ) ∂ H 1 ( ∂ M ∘ ) ≅ H 1 ( ∂ N ) incl ∗ H 1 ( N ) ≅ H 1 ( t ∈ Σ ⋃ M t ) ≅ t ∈ Σ ⨁ H 1 ( M t ) .
The homomorphism ι \iota ι takes the isotopy class of a section σ \sigma σ to [ σ ] − [ σ 0 ∣ B ∘ ] ∈ H 2 ( M ∘ , ∂ M ∘ ) [\sigma]-[\sigma_0|_{B^\circ}] \in H_2(M^\circ,\partial M^\circ) [ σ ] − [ σ 0 ∣ B ∘ ] ∈ H 2 ( M ∘ , ∂ M ∘ ) . The map ∂ : H 2 ( M ∘ , ∂ M ∘ ) → H 1 ( ∂ M ∘ ) \partial: H_2(M^\circ,\partial M^\circ) \to H_1(\partial M^\circ) ∂ : H 2 ( M ∘ , ∂ M ∘ ) → H 1 ( ∂ M ∘ ) is the boundary map in the long exact sequence in homology of the pair ( M ∘ , ∂ M ∘ ) (M^\circ,\partial M^\circ) ( M ∘ , ∂ M ∘ ) . It acts on a homology class in H 2 ( M ∘ , ∂ M ∘ ) H_2(M^\circ,\partial M^\circ) H 2 ( M ∘ , ∂ M ∘ ) by restricting it to the boundary ∂ M ∘ \partial M^\circ ∂ M ∘ . Observe that ∂ M ∘ \partial M^\circ ∂ M ∘ and ∂ N \partial N ∂ N are equal as sets, so the map H 1 ( ∂ M ∘ ) ≅ H 1 ( ∂ N ) H_1(\partial M^\circ) \cong H_1(\partial N) H 1 ( ∂ M ∘ ) ≅ H 1 ( ∂ N ) is induced by the identity. Inclusion ∂ N ↪ N \partial N \hookrightarrow N ∂ N ↪ N induces the map H 1 ( ∂ N ) → incl ∗ H 1 ( N ) H_1(\partial N) \xrightarrow{\operatorname{incl}_*} H_1(N) H 1 ( ∂ N ) incl ∗ H 1 ( N ) . Since N N N strong deformation-retracts to ⋃ t ∈ Σ M t \bigcup_{t\in\Sigma} M_t ⋃ t ∈ Σ M t , we obtain an isomorphism in homology H 1 ( N ) ≅ H 1 ( ⋃ t ∈ Σ M t ) H_1(N) \cong H_1\left(\bigcup_{t\in\Sigma} M_t\right) H 1 ( N ) ≅ H 1 ( ⋃ t ∈ Σ M t ) . Finally, since the spaces M t M_t M t are disjoint, homology of their union is isomorphic to the direct sum of their homology groups, yielding an isomorphism H 1 ( ⋃ t ∈ Σ M t ) ≅ ⨁ t ∈ Σ H 1 ( M t ) H_1\left(\bigcup_{t\in\Sigma} M_t\right) \cong\bigoplus_{t\in\Sigma} H_1(M_t) H 1 ( ⋃ t ∈ Σ M t ) ≅ ⨁ t ∈ Σ H 1 ( M t ) .
Effectively, given an isotopy class [ σ ] ∈ MW ( π ∘ ) [\sigma] \in\operatorname{MW}(\pi^\circ) [ σ ] ∈ MW ( π ∘ ) , the map Ψ \Psi Ψ restricts σ \sigma σ to the boundary of a neighborhood of each singular fiber, obtaining a homology class in ∂ N \partial N ∂ N . Inclusion ∂ N ↪ N \partial N \hookrightarrow N ∂ N ↪ N gives a homology class in N N N , which deformation retracts to the union of the singular fibers.
For each singular value t ∈ B t \in B t ∈ B , let D t D_t D t be a disk around t t t containing no other critical values of π \pi π . Define the map ψ t : MW ( π ∣ π − 1 ( D t ∘ ) ) → H 1 ( X t ) \psi_t : \operatorname{MW}(\pi|_{\pi^{-1}(D_t^\circ)}) \to H_1(X_t) ψ t : MW ( π ∣ π − 1 ( D t ∘ ) ) → H 1 ( X t ) by ψ t ( [ σ ] ) = [ σ ∣ ∂ D t ] − [ σ 0 ∣ ∂ D t ] \psi_t([\sigma]) = [\sigma|_{\partial D_t}] - [\sigma_0|_{\partial D_t}] ψ t ([ σ ]) = [ σ ∣ ∂ D t ] − [ σ 0 ∣ ∂ D t ] . This is the map ψ \psi ψ from § 4 . We can use it to prove the following proposition.
Proposition 5.2 (A Global Obstruction to Extending Sections). Let π : M → B \pi: M \to B π : M → B be an elliptic fibration. The Mordell–Weil group MW ( π ) \operatorname{MW}(\pi) MW ( π ) is the kernel of the map Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \Psi: \operatorname{MW}(\pi^\circ) \to\bigoplus_{t\in\Sigma} H_1(M_t) Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) .
Proof. A section σ : B ∘ → M ∘ \sigma:B^\circ\to M^\circ σ : B ∘ → M ∘ extends to a section of π \pi π if and only if it extends in a neighborhood of each fiber. We rewrite Ψ \Psi Ψ in a way that lets us use Theorem 4.2.
For t ∈ Σ t \in\Sigma t ∈ Σ , let i t : M t ↪ π − 1 ( D ‾ t ) i_t:M_t \hookrightarrow\pi^{-1}(\overline{D}_t) i t : M t ↪ π − 1 ( D t ) be the natural inclusion map. Homology of a union of disjoint union of spaces is naturally isomorphic to the direct sum of the homology groups of the spaces. Thus, there exists the following commutative diagram:
H 1 ( ∂ N ) → ≅ ⨁ t ∈ Σ H 1 ( π − 1 ( ∂ D t ) ) incl ∗ ↓ ↓ incl ∗ H 1 ( N ) → ≅ ⨁ t ∈ Σ H 1 ( π − 1 ( D ‾ t ) ) incl ∗ − 1 ↓ ≅ ↓ ⨁ t ∈ Σ ( i t ) ∗ − 1 H 1 ( ⋃ t ∈ Σ M t ) → ≅ ⨁ t ∈ Σ H 1 ( M t ) \begin{CD}
H_1(\partial N) @>{\cong}>> \bigoplus_{t\in\Sigma} H_1\left(\pi^{-1}(\partial D_t)\right) \\
@V{\operatorname{incl}_*}VV @VV{\operatorname{incl}_*}V \\
H_1(N) @>{\cong}>> \bigoplus_{t\in\Sigma} H_1\left(\pi^{-1}(\overline{D}_t)\right) \\
@V{\operatorname{incl}_*^{-1}}V{\cong}V @VV{\bigoplus_{t\in\Sigma}(i_t)_*^{-1}}V{\cong} \\
H_1\left(\bigcup_{t\in\Sigma}M_t\right) @>{\cong}>> \bigoplus_{t\in\Sigma}H_1(M_t)
\end{CD} H 1 ( ∂ N ) incl ∗ ↓ ⏐ H 1 ( N ) incl ∗ − 1 ↓ ⏐ ≅ H 1 ( t ∈ Σ ⋃ M t ) ≅ ≅ ≅ t ∈ Σ ⨁ H 1 ( π − 1 ( ∂ D t ) ) ↓ ⏐ incl ∗ t ∈ Σ ⨁ H 1 ( π − 1 ( D t ) ) ↓ ⏐ ⨁ t ∈ Σ ( i t ) ∗ − 1 t ∈ Σ ⨁ H 1 ( M t )
where the first vertical map is induced by inclusion ∂ N ↪ N \partial N \hookrightarrow N ∂ N ↪ N and the second vertical map is the inverse of the isomorphism induced by the inclusion ⋃ t ∈ Σ M t ↪ N \bigcup_{t\in\Sigma} M_t \hookrightarrow N ⋃ t ∈ Σ M t ↪ N . Hence, the composition of Ψ \Psi Ψ with the projection ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( M t ) \bigoplus_{t\in\Sigma} H_1(M_t) \to H_1(M_t) ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( M t ) is equal to the map − ψ t -\psi_t − ψ t . By Theorem 4.2, σ \sigma σ is isotopic to a section σ t : B ∘ → M ∘ \sigma_t:B^\circ\to M^\circ σ t : B ∘ → M ∘ that is equal to σ \sigma σ away from a neighborhood of t t t and extends in a neighborhood of the critical value t ∈ B t \in B t ∈ B if and only if ψ t ( [ σ ] ) = 0 \psi_t([\sigma])=0 ψ t ([ σ ]) = 0 . Hence, σ \sigma σ is isotopic over B ∘ B^\circ B ∘ to a section σ ′ : B ∘ → M ∘ \sigma':B^\circ\to M^\circ σ ′ : B ∘ → M ∘ , which extends to a global section σ ′ : B → M \sigma':B \to M σ ′ : B → M if and only if Ψ ( [ σ ] ) = 0 \Psi([\sigma])=0 Ψ ([ σ ]) = 0 .
Remark 5.3. We will later see that the map MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \operatorname{MW}(\pi^\circ) \to\bigoplus_{t\in\Sigma} H_1(M_t) MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) is in fact surjective and the two Mordell–Weil groups fit in the following short exact sequence:
0 → MW ( π ) → MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) → 0. 0 \to\operatorname{MW}(\pi) \to\operatorname{MW}(\pi^\circ) \to\bigoplus_{t\in\Sigma} H_1(M_t) \to0. 0 → MW ( π ) → MW ( π ∘ ) → t ∈ Σ ⨁ H 1 ( M t ) → 0.
Remark 5.4. In Proposition 5.2, we can explicitly compute ⨁ t ∈ Σ H 1 ( M t ) \bigoplus_{t\in\Sigma} H_1(M_t) ⨁ t ∈ Σ H 1 ( M t ) . Indeed, the M t M_t M t are simply connected if and only if they are additive fibers in Kodaira’s classification. Each multiplicative fiber is a cycle of n n n spheres and thus satisfies H 1 ( M t ) ≅ Z H_1(M_t)\cong\mathbb{Z} H 1 ( M t ) ≅ Z . Hence, if m m m denotes the number of multiplicative fibers of π \pi π , it follows ⨁ t ∈ Σ H 1 ( M t ) ≅ Z m \bigoplus_{t\in\Sigma} H_1(M_t)\cong\mathbb{Z}^m ⨁ t ∈ Σ H 1 ( M t ) ≅ Z m . In particular, the Mordell–Weil groups of π \pi π and π ∘ \pi^\circ π ∘ differ by a finitely generated free group.
Proof of thm: full MW
We are finally ready to compute MW ( π ) \operatorname{MW}(\pi) MW ( π ) in the general case where π : M → B \pi:M \to B π : M → B is an elliptic fibration over a closed complex curve B B B .
Assume that the critical values of π \pi π are Σ = { t 1 , … , t n } ⊂ B \Sigma=\{t_1,\ldots,t_n\}\subset B Σ = { t 1 , … , t n } ⊂ B . Denote the irreducible components of the fiber M t i M_{t_i} M t i by C i , 0 , … , C i , r i C_{i,0},\ldots,C_{i,r_i} C i , 0 , … , C i , r i , where we assume that C i , 0 C_{i,0} C i , 0 is the component intersecting the zero-section σ 0 \sigma_0 σ 0 . These represent classes [ C i , j ] ∈ H 2 ( M ) [C_{i,j}]\in H_2(M) [ C i , j ] ∈ H 2 ( M ) . Let c i , j ∈ H 2 ( M ) c_{i,j}\in H^2(M) c i , j ∈ H 2 ( M ) denote the Poincaré dual of [ C i , j ] [C_{i,j}] [ C i , j ] in M M M . Let e ∈ H 2 ( M ) e\in H^2(M) e ∈ H 2 ( M ) denote the Poincaré dual of the fiber class F F F of π \pi π and let s ∈ H 2 ( M ) s\in H^2(M) s ∈ H 2 ( M ) denote the Poincaré dual of [ σ 0 ( B ) ] ∈ H 2 ( M ) [\sigma_0(B)]\in H_2(M) [ σ 0 ( B )] ∈ H 2 ( M ) . Recalled that the trivial lattice is defined by
Triv ( M ) : = ⟨ e , s , c i , j : j > 0 ⟩ ⊂ H 2 ( M ) . \operatorname{Triv}(M):=\langle e,s,c_{i,j}:j>0\rangle\subset H^2(M). Triv ( M ) := ⟨ e , s , c i , j : j > 0 ⟩ ⊂ H 2 ( M ) .
We are now ready to prove Theorem 1.1.
Proof of Theorem 1.1. Step 1. Construct an exact sequence relating H 2 ( M ) H^2(M) H 2 ( M ) , H 2 ( M ∘ ) H^2(M^\circ) H 2 ( M ∘ ) and ⨁ t ∈ Σ H 1 ( M t ) \bigoplus_{t\in\Sigma} H_1(M_t) ⨁ t ∈ Σ H 1 ( M t ) . Consider the long exact sequence in cohomology corresponding to the pair ( M , M ∘ ) (M,M^\circ) ( M , M ∘ ) .
⋯ ⟶ H 1 ( M ∘ ) ⟶ H 2 ( M , M ∘ ) → j ∗ H 2 ( M ) ⟶ H 2 ( M ∘ ) → δ H 3 ( M , M ∘ ) → j ∗ H 3 ( M ) ⟶ ⋯ (8) \cdots\longrightarrow H^1(M^\circ) \longrightarrow H^2(M,M^\circ) \xrightarrow{j^*} H^2(M) \longrightarrow H^2(M^\circ) \xrightarrow{\delta} H^3(M,M^\circ) \xrightarrow{j^*} H^3(M) \longrightarrow\cdots \tag*{(8)} ⋯ ⟶ H 1 ( M ∘ ) ⟶ H 2 ( M , M ∘ ) j ∗ H 2 ( M ) ⟶ H 2 ( M ∘ ) δ H 3 ( M , M ∘ ) j ∗ H 3 ( M ) ⟶ ⋯ (8)
Let N N N denote the closure of M − M ∘ M-M^\circ M − M ∘ . Observe that N N N strong deformation retracts to ⋃ t ∈ Σ M t \bigcup_{t\in\Sigma}M_t ⋃ t ∈ Σ M t , so inclusion incl : ⋃ t ∈ Σ M t ↪ N \operatorname{incl}\colon\bigcup_{t\in\Sigma}M_t\hookrightarrow N incl : ⋃ t ∈ Σ M t ↪ N induces an isomorphism in homology. Let l : ( N , ∂ N ) ↪ ( M , M ∘ ) l\colon(N,\partial N)\hookrightarrow(M,M^\circ) l : ( N , ∂ N ) ↪ ( M , M ∘ ) be inclusion. By excision, l l l induces an isomorphism l ∗ : H k ( M , M ∘ ) → H k ( N , ∂ N ) l^*\colon H^k(M,M^\circ)\to H^k(N,\partial N) l ∗ : H k ( M , M ∘ ) → H k ( N , ∂ N ) for k = 0 , 1 , 2 , 3 , 4 k=0,1,2,3,4 k = 0 , 1 , 2 , 3 , 4 . Define τ k \tau_k τ k as the composition
H k ( M , M ∘ ) → ≅ l ∗ H k ( N , ∂ N ) → ≅ PD [ N , ∂ N ] H 4 − k ( N ) → ≅ ( incl ∗ ) − 1 H 4 − k ( ⋃ t ∈ Σ M t ) → ≅ ⨁ t ∈ Σ H 4 − k ( M t ) . \begin{aligned}
H^k(M,M^\circ)&\xrightarrow[\cong]{l^*}H^k(N,\partial N)
\xrightarrow[\cong]{\operatorname{PD}_{[N,\partial N]}}H_{4-k}(N)
\xrightarrow[\cong]{(\operatorname{incl}_*)^{-1}}H_{4-k}\left(\bigcup_{t\in\Sigma}M_t\right)\\
&\xrightarrow[\cong]{}\bigoplus_{t\in\Sigma}H_{4-k}(M_t).
\end{aligned} H k ( M , M ∘ ) l ∗ ≅ H k ( N , ∂ N ) PD [ N , ∂ N ] ≅ H 4 − k ( N ) ( incl ∗ ) − 1 ≅ H 4 − k ( t ∈ Σ ⋃ M t ) ≅ t ∈ Σ ⨁ H 4 − k ( M t ) .
where the last map is given by the fact that M t M_t M t are disjoint sets. Using the isomorphisms τ k \tau_k τ k and Poincaré duality in M M M , the long exact sequence (8) gives
⟶ H 1 ( M ∘ ) ⟶ ⨁ t ∈ Σ H 2 ( M t ) → j ∗ ∘ τ 2 − 1 H 2 ( M ) ⟶ H 2 ( M ∘ ) → τ 3 ∘ δ ⨁ t ∈ Σ H 1 ( M t ) → PD M ∘ j ∗ ∘ τ 3 − 1 H 1 ( M ) ⟶ ⋯ (9) \longrightarrow H^1(M^\circ)\longrightarrow\bigoplus_{t\in\Sigma}H_2(M_t)\xrightarrow{j^*\circ\tau_2^{-1}}H^2(M)\longrightarrow H^2(M^\circ)\xrightarrow{\tau_3\circ\delta}\bigoplus_{t\in\Sigma}H_1(M_t)\xrightarrow{\operatorname{PD}_M\circ j^*\circ\tau_3^{-1}}H_1(M)\longrightarrow\cdots \tag*{(9)} ⟶ H 1 ( M ∘ ) ⟶ t ∈ Σ ⨁ H 2 ( M t ) j ∗ ∘ τ 2 − 1 H 2 ( M ) ⟶ H 2 ( M ∘ ) τ 3 ∘ δ t ∈ Σ ⨁ H 1 ( M t ) PD M ∘ j ∗ ∘ τ 3 − 1 H 1 ( M ) ⟶ ⋯ (9)
Step 2. The map PD M ∘ j ∗ ∘ ( τ 4 − k ) − 1 : ⨁ t ∈ Σ H k ( M t ) → H k ( M ) \operatorname{PD}_M\circ j^*\circ(\tau_{4-k})^{-1}\colon\bigoplus_{t\in\Sigma}H_k(M_t)\to H_k(M) PD M ∘ j ∗ ∘ ( τ 4 − k ) − 1 : ⨁ t ∈ Σ H k ( M t ) → H k ( M ) is induced by the inclusion i t : M t ↪ M i_t\colon M_t\hookrightarrow M i t : M t ↪ M on each summand, for k = 0 , 1 , 2 , 3 , 4 k=0,1,2,3,4 k = 0 , 1 , 2 , 3 , 4 . By definition of τ 4 − k \tau_{4-k} τ 4 − k , the claim is equivalent to showing that the rectangle in the diagram below commutes.
H 4 − k ( M , M ∘ ) → j ∗ H 4 − k ( M ) l ∗ ↓ ≅ ↓ PD M H 4 − k ( N , ∂ N ) → PD ( N , ∂ N ) H k ( N ) PD ( N , ∂ N ) ↓ ≅ ↓ l ∗ H k ( N ) ← incl ∗ H k ( ⋃ t ∈ Σ M t ) ≅ ↓ ↓ ⨁ t ∈ Σ ( i t ) ∗ ⨁ t ∈ Σ H k ( M t ) → H k ( M ) \begin{CD}
H^{4-k}(M,M^\circ) @>{j^*}>> H^{4-k}(M)\\
@V{l^*}V{\cong}V @VV{\operatorname{PD}_M}V\\
H^{4-k}(N,\partial N) @>{\operatorname{PD}_{(N,\partial N)}}>> H_k(N)\\
@V{\operatorname{PD}_{(N,\partial N)}}V{\cong}V @VV{l_*}V\\
H_k(N) @<{\operatorname{incl}_*}<< H_k\left(\bigcup_{t\in\Sigma}M_t\right)\\
@V{\cong}V{}V @VV{\bigoplus_{t\in\Sigma}(i_t)_*}V\\
\bigoplus_{t\in\Sigma}H_k(M_t) @>{}>> H_k(M)
\end{CD} H 4 − k ( M , M ∘ ) l ∗ ↓ ⏐ ≅ H 4 − k ( N , ∂ N ) PD ( N , ∂ N ) ↓ ⏐ ≅ H k ( N ) ≅ ↓ ⏐ t ∈ Σ ⨁ H k ( M t ) j ∗ PD ( N , ∂ N ) incl ∗ H 4 − k ( M ) ↓ ⏐ PD M H k ( N ) ↓ ⏐ l ∗ H k ( t ∈ Σ ⋃ M t ) ↓ ⏐ ⨁ t ∈ Σ ( i t ) ∗ H k ( M )
As a composition of inclusions, triangle (2) commutes. Clearly, triangle (3) also commutes. Subdiagram (1) is commutative if and only if for any α ∈ H 4 − k ( M , M ∘ ) \alpha\in H^{4-k}(M,M^\circ) α ∈ H 4 − k ( M , M ∘ ) , the following identity holds in H k ( M ) H_k(M) H k ( M )
l ∗ ( l ∗ α ⌢ [ N , ∂ N ] ) = j ∗ α ⌢ [ M ] . (10) l_*\left(l^*\alpha\mathbin{\frown}[N,\partial N]\right)=j^*\alpha\mathbin{\frown}[M]. \tag*{(10)} l ∗ ( l ∗ α ⌢ [ N , ∂ N ] ) = j ∗ α ⌢ [ M ] . (10)
By naturality of the cap product, the left-hand side is equal to α ⌢ l ∗ [ N , ∂ N ] \alpha\mathbin{\frown} l_*[N,\partial N] α ⌢ l ∗ [ N , ∂ N ] . Since l ∗ [ N , ∂ N ] = j ∗ [ M ] ∈ H 4 ( M , M ∘ ) l_*[N,\partial N]=j_*[M]\in H_4(M,M^\circ) l ∗ [ N , ∂ N ] = j ∗ [ M ] ∈ H 4 ( M , M ∘ ) , the left hand side of (10) equals α ⌢ j ∗ [ M ] \alpha\mathbin{\frown} j_*[M] α ⌢ j ∗ [ M ] , so (10) holds for all α ∈ H 4 − k ( M , M ∘ ) \alpha\in H^{4-k}(M,M^\circ) α ∈ H 4 − k ( M , M ∘ ) .
Step 3. The map PD M ∘ j ∗ ∘ ( τ 3 ) − 1 : ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( M ) \operatorname{PD}_M\circ j^*\circ(\tau_3)^{-1}\colon\bigoplus_{t\in\Sigma}H_1(M_t)\to H_1(M) PD M ∘ j ∗ ∘ ( τ 3 ) − 1 : ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( M ) in the long exact sequence (9) is zero. By Step 2, this map is ⨁ t ∈ Σ ( i t ) ∗ \bigoplus_{t\in\Sigma}(i_t)_* ⨁ t ∈ Σ ( i t ) ∗ . The map π ∗ : H 1 ( M ) → H 1 ( B ) \pi_*\colon H_1(M)\to H_1(B) π ∗ : H 1 ( M ) → H 1 ( B ) is an isomorphism by Proposition 2.1. Thus, it suffices to show that π ∗ ∘ ( ⨁ t ∈ Σ ( i t ) ∗ ) : ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( B ) \pi_*\circ\bigl(\bigoplus_{t\in\Sigma}(i_t)_*\bigr)\colon\bigoplus_{t\in\Sigma}H_1(M_t)\to H_1(B) π ∗ ∘ ( ⨁ t ∈ Σ ( i t ) ∗ ) : ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( B ) is zero. But for each t ∈ Σ t\in\Sigma t ∈ Σ , the map π ∘ i t \pi\circ i_t π ∘ i t is constant on M t M_t M t , so π ∗ ∘ ( i t ) ∗ \pi_*\circ(i_t)_* π ∗ ∘ ( i t ) ∗ is zero on H 1 ( M t ) H_1(M_t) H 1 ( M t ) . Hence, the map PD M ∘ j ∗ ∘ ( τ 3 ) − 1 : ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( M ) \operatorname{PD}_M\circ j^*\circ(\tau_3)^{-1}\colon\bigoplus_{t\in\Sigma}H_1(M_t)\to H_1(M) PD M ∘ j ∗ ∘ ( τ 3 ) − 1 : ⨁ t ∈ Σ H 1 ( M t ) → H 1 ( M ) is trivial.
Step 4. The image of the map j ∗ ∘ ( τ 2 ) − 1 : ⨁ t ∈ Σ H 2 ( M t ) → H 2 ( M ) j^*\circ(\tau_2)^{-1}\colon\bigoplus_{t\in\Sigma}H_2(M_t)\to H^2(M) j ∗ ∘ ( τ 2 ) − 1 : ⨁ t ∈ Σ H 2 ( M t ) → H 2 ( M ) is ⟨ c i , j : i = { 1 , … , n } , j ≥ 0 ⟩ \langle c_{i,j}:i=\{1,\ldots,n\},j\geq0\rangle ⟨ c i , j : i = { 1 , … , n } , j ≥ 0 ⟩ . Observe that ⨁ t ∈ Σ H 2 ( M t ) \bigoplus_{t\in\Sigma}H_2(M_t) ⨁ t ∈ Σ H 2 ( M t ) is the free abelian group with generators [ C i , j ] [C_{i,j}] [ C i , j ] . By Step 2, the following diagram commutes:
H 2 ( M , M ∘ ) → j ∗ H 2 ( M ) τ 2 ↓ ≅ ≅ ↑ PD M H 2 ( ⋃ t ∈ Σ M t ) → incl ∗ H 2 ( M ) ≅ ↑ τ 2 ⨁ t ∈ Σ H 2 ( M t ) \begin{CD}
H^2(M,M^\circ) @>{j^*}>> H^2(M) \\
@V{\tau_2}V{\cong}V @A{\cong}A{\operatorname{PD}_M}A \\
H_2\left(\bigcup_{t\in\Sigma}M_t\right) @>{\operatorname{incl}_*}>> H_2(M) \\
@A{\cong}A{\tau_2}A \\
\bigoplus_{t\in\Sigma}H_2(M_t)
\end{CD} H 2 ( M , M ∘ ) τ 2 ↓ ⏐ ≅ H 2 ( t ∈ Σ ⋃ M t ) ≅ ⏐ ↑ τ 2 t ∈ Σ ⨁ H 2 ( M t ) j ∗ incl ∗ H 2 ( M ) ≅ ⏐ ↑ PD M H 2 ( M )
Hence, j ∗ ∘ ( τ 2 ) − 1 ( [ C i , j ] ) = PD M − 1 [ C i , j ] = c i , j j^*\circ(\tau_2)^{-1}([C_{i,j}])=\operatorname{PD}_M^{-1}[C_{i,j}]=c_{i,j} j ∗ ∘ ( τ 2 ) − 1 ([ C i , j ]) = PD M − 1 [ C i , j ] = c i , j . Thus, the image of the map j ∗ ∘ τ 2 − 1 j^*\circ\tau_2^{-1} j ∗ ∘ τ 2 − 1 is precisely ⟨ c i , j ⟩ ⊂ H 2 ( M ) \langle c_{i,j}\rangle\subset H^2(M) ⟨ c i , j ⟩ ⊂ H 2 ( M ) .
Step 5. Deduce a short exact sequence relating the annihilators and replace H 2 ( M ∘ ) F H^2(M^\circ)^F H 2 ( M ∘ ) F with MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) . By Step 3 and Step 4, the long exact sequence (9) becomes
0 ⟶ ⟨ c i , j : i = { 1 , … , n } , j ≥ 0 ⟩ ⟶ H 2 ( M ) ⟶ H 2 ( M ∘ ) → τ 3 ∘ δ ⨁ t ∈ Σ H 1 ( M t ) ⟶ 0. 0\longrightarrow\langle c_{i,j}:i=\{1,\ldots,n\},j\geq0\rangle\longrightarrow H^2(M)\longrightarrow H^2(M^\circ)\xrightarrow{\tau_3\circ\delta}\bigoplus_{t\in\Sigma}H_1(M_t)\longrightarrow0. 0 ⟶ ⟨ c i , j : i = { 1 , … , n } , j ≥ 0 ⟩ ⟶ H 2 ( M ) ⟶ H 2 ( M ∘ ) τ 3 ∘ δ t ∈ Σ ⨁ H 1 ( M t ) ⟶ 0.
The components C i , j C_{i,j} C i , j do not intersect the generic fiber, so all c i , j c_{i,j} c i , j annihilate F F F . Restricting the exact sequence to the annihilators of F F F induces the following exact sequence
0 ⟶ ⟨ c i , j : i = { 1 , … , n } , j ≥ 0 ⟩ ⟶ H 2 ( M ) F ⟶ H 2 ( M ∘ ) F → τ 3 ∘ δ ⨁ t ∈ Σ H 1 ( M t ) ⟶ 0. 0\longrightarrow\langle c_{i,j}:i=\{1,\ldots,n\},j\geq0\rangle\longrightarrow H^2(M)^F\longrightarrow H^2(M^\circ)^F\xrightarrow{\tau_3\circ\delta}\bigoplus_{t\in\Sigma}H_1(M_t)\longrightarrow0. 0 ⟶ ⟨ c i , j : i = { 1 , … , n } , j ≥ 0 ⟩ ⟶ H 2 ( M ) F ⟶ H 2 ( M ∘ ) F τ 3 ∘ δ t ∈ Σ ⨁ H 1 ( M t ) ⟶ 0.
Surjectivity follows since for any x ∈ H 2 ( M ∘ ) x\in H^2(M^\circ) x ∈ H 2 ( M ∘ ) , it holds x − ⟨ x , F ⟩ s ∣ M ∘ ∈ H 2 ( M ∘ ) F x-\langle x,F\rangle s|_{M^\circ}\in H^2(M^\circ)^F x − ⟨ x , F ⟩ s ∣ M ∘ ∈ H 2 ( M ∘ ) F , which maps to the same element in ⨁ t ∈ Σ H 1 ( M t ) \bigoplus_{t\in\Sigma}H_1(M_t) ⨁ t ∈ Σ H 1 ( M t ) as x x x . This induces the short exact sequence
0 ⟶ H 2 ( M ) F / ⟨ c i , j ⟩ ⟶ H 2 ( M ∘ ) F → τ 3 ∘ δ ⨁ t ∈ Σ H 1 ( M t ) ⟶ 0. (11) 0\longrightarrow H^2(M)^F/\langle c_{i,j}\rangle\longrightarrow H^2(M^\circ)^F\xrightarrow{\tau_3\circ\delta}\bigoplus_{t\in\Sigma}H_1(M_t)\longrightarrow0. \tag*{(11)} 0 ⟶ H 2 ( M ) F / ⟨ c i , j ⟩ ⟶ H 2 ( M ∘ ) F τ 3 ∘ δ t ∈ Σ ⨁ H 1 ( M t ) ⟶ 0. (11)
By Proposition 3.2, there exists an isomorphism Φ : MW ( π ∘ ) → ≅ H 2 ( M ∘ ) F \Phi\colon\operatorname{MW}(\pi^\circ)\xrightarrow{\cong}H^2(M^\circ)^F Φ : MW ( π ∘ ) ≅ H 2 ( M ∘ ) F , which takes the isotopy class of a section σ \sigma σ to PD [ σ ] − PD [ σ 0 ] ∈ H 2 ( M ∘ ) F \operatorname{PD}[\sigma]-\operatorname{PD}[\sigma_0]\in H^2(M^\circ)^F PD [ σ ] − PD [ σ 0 ] ∈ H 2 ( M ∘ ) F . Thus, the short exact sequence (11) induces the short exact sequence
0 ⟶ H 2 ( M ) F / ⟨ c i , j ⟩ ⟶ MW ( π ∘ ) → τ 3 ∘ δ ∘ Φ ⨁ t ∈ Σ H 1 ( M t ) ⟶ 0. (12) 0\longrightarrow H^2(M)^F/\langle c_{i,j}\rangle\longrightarrow\operatorname{MW}(\pi^\circ)\xrightarrow{\tau_3\circ\delta\circ\Phi}\bigoplus_{t\in\Sigma}H_1(M_t)\longrightarrow0. \tag*{(12)} 0 ⟶ H 2 ( M ) F / ⟨ c i , j ⟩ ⟶ MW ( π ∘ ) τ 3 ∘ δ ∘ Φ t ∈ Σ ⨁ H 1 ( M t ) ⟶ 0. (12)
By Proposition 5.2, MW ( π ) \operatorname{MW}(\pi) MW ( π ) is the kernel of the map Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \Psi\colon\operatorname{MW}(\pi^\circ)\to\bigoplus_{t\in\Sigma}H_1(M_t) Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) . Thus, to compute MW ( π ) \operatorname{MW}(\pi) MW ( π ) , it suffices to show that the two maps between MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) and ⨁ t ∈ Σ H 1 ( M t ) \bigoplus_{t\in\Sigma}H_1(M_t) ⨁ t ∈ Σ H 1 ( M t ) are equal.
Step 6. The maps Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \Psi\colon\operatorname{MW}(\pi^\circ)\to\bigoplus_{t\in\Sigma}H_1(M_t) Ψ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) and τ 3 ∘ δ ∘ Φ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \tau_3\circ\delta\circ\Phi\colon\operatorname{MW}(\pi^\circ)\to\bigoplus_{t\in\Sigma}H_1(M_t) τ 3 ∘ δ ∘ Φ : MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) are equal. By the definitions of Φ \Phi Φ and τ 3 \tau_3 τ 3 , this is equivalent to showing commutativity of the following diagram:
H 2 ( M ∘ ) → δ H 3 ( M , M ∘ ) ≅ P D ( M ∘ , ∂ M ∘ ) − 1 ↑ ≅ ι ∗ ↓ H 2 ( M ∘ , ∂ M ∘ ) H 3 ( N , ∂ N ) Φ ↑ ≅ P D ( N , ∂ N ) ↓ M W ( π ∘ ) H 1 ( N ) ≅ ↓ H 1 ( ⋃ t ∈ Σ M t ) ≅ ↓ ⨁ t ∈ Σ H 1 ( M t ) \begin{CD}
H^2(M^\circ) @>{\delta}>> H^3(M,M^\circ) \\
@A{\cong\,\mathrm{PD}^{-1}_{(M^\circ,\partial M^\circ)}}AA @V{\cong\,\iota^*}VV \\
H_2(M^\circ,\partial M^\circ) @. H^3(N,\partial N) \\
@A{\Phi}AA @V{\cong\,\mathrm{PD}_{(N,\partial N)}}VV \\
\mathrm{MW}(\pi^\circ) @. H_1(N) \\
@. @V{\cong}VV \\
@. H_1\left(\bigcup_{t\in\Sigma}M_t\right) \\
@. @V{\cong}VV \\
@. \bigoplus_{t\in\Sigma}H_1(M_t)
\end{CD} H 2 ( M ∘ ) ≅ PD ( M ∘ , ∂ M ∘ ) − 1 ⏐ ↑ H 2 ( M ∘ , ∂ M ∘ ) Φ ⏐ ↑ MW ( π ∘ ) δ H 3 ( M , M ∘ ) ≅ ι ∗ ↓ ⏐ H 3 ( N , ∂ N ) ≅ PD ( N , ∂ N ) ↓ ⏐ H 1 ( N ) ≅ ↓ ⏐ H 1 ( t ∈ Σ ⋃ M t ) ≅ ↓ ⏐ t ∈ Σ ⨁ H 1 ( M t )
We expand this diagram by writing out the maps in the definition of Ψ \Psi Ψ : M W ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) \mathrm{MW}(\pi^\circ)\to\bigoplus_{t\in\Sigma}H_1(M_t) MW ( π ∘ ) → ⨁ t ∈ Σ H 1 ( M t ) . We add some intermediary maps, which allow us to use naturality of the long exact sequence of a pair and of Poincaré–Lefschetz duality.
H 2 ( M ∘ ) = H 2 ( M ∘ ) → δ H 3 ( M , M ∘ ) r e s t r ↓ r e s t r ↓ ι ∗ ↓ H 2 ( ∂ M ∘ ) → i d ∗ H 2 ( ∂ N ) → δ H 3 ( N , ∂ N ) ≅ ⟨ [ ∂ M ∘ ] ⟩ ↓ ≅ ⟨ [ ∂ N ] ⟩ ↓ ≅ ⟨ [ N , ∂ N ] ⟩ ↓ H 2 ( M ∘ , ∂ M ∘ ) → ∂ H 1 ( ∂ M ∘ ) → i d ∗ ≅ H 1 ( ∂ N ) → i n c l ∗ H 1 ( N ) ↑ ≅ ↓ M W ( π ∘ ) H 1 ( ⋃ t ∈ Σ M t ) Ψ ↓ ≅ ↓ ⨁ t ∈ Σ H 1 ( M t ) \begin{CD}
H^2(M^\circ) @= H^2(M^\circ) @>{\delta}>> H^3(M,M^\circ) \\
@V{\mathrm{restr}}VV @V{\mathrm{restr}}VV @V{\iota^*}VV \\
H^2(\partial M^\circ) @>{\mathrm{id}^*}>> H^2(\partial N) @>{\delta}>> H^3(N,\partial N) \\
@V{\cong\,\langle[\partial M^\circ]\rangle}VV @V{\cong\,\langle[\partial N]\rangle}VV @V{\cong\,\langle[N,\partial N]\rangle}VV \\
H_2(M^\circ,\partial M^\circ) @>{\partial}>> H_1(\partial M^\circ) @>{\mathrm{id}_*\,\cong}>> H_1(\partial N) @>{\mathrm{incl}_*}>> H_1(N) \\
@A{}AA @. @. @V{\cong}VV \\
\mathrm{MW}(\pi^\circ) @. @. @. H_1\left(\bigcup_{t\in\Sigma}M_t\right) \\
@V{\Psi}VV @. @. @V{\cong}VV \\
@. @. @. \bigoplus_{t\in\Sigma}H_1(M_t)
\end{CD} H 2 ( M ∘ ) restr ↓ ⏐ H 2 ( ∂ M ∘ ) ≅ ⟨[ ∂ M ∘ ]⟩ ↓ ⏐ H 2 ( M ∘ , ∂ M ∘ ) ⏐ ↑ MW ( π ∘ ) Ψ ↓ ⏐ id ∗ ∂ H 2 ( M ∘ ) restr ↓ ⏐ H 2 ( ∂ N ) ≅ ⟨[ ∂ N ]⟩ ↓ ⏐ H 1 ( ∂ M ∘ ) δ δ id ∗ ≅ H 3 ( M , M ∘ ) ι ∗ ↓ ⏐ H 3 ( N , ∂ N ) ≅ ⟨[ N , ∂ N ]⟩ ↓ ⏐ H 1 ( ∂ N ) incl ∗ H 1 ( N ) ≅ ↓ ⏐ H 1 ( t ∈ Σ ⋃ M t ) ≅ ↓ ⏐ t ∈ Σ ⨁ H 1 ( M t )
The first row is the identity, followed by the boundary map δ : H 2 ( M ∘ ) → H 3 ( M , M ∘ ) \delta:H^2(M^\circ)\to H^3(M,M^\circ) δ : H 2 ( M ∘ ) → H 3 ( M , M ∘ ) from the long exact sequence of the pair ( M , M ∘ ) (M,M^\circ) ( M , M ∘ ) . The second row consists of the map induced by the identity i d : ∂ M ∘ → ∂ N \mathrm{id}:\partial M^\circ\to\partial N id : ∂ M ∘ → ∂ N and the boundary map δ : H 2 ( ∂ N ) → H 3 ( N , ∂ N ) \delta:H^2(\partial N)\to H^3(N,\partial N) δ : H 2 ( ∂ N ) → H 3 ( N , ∂ N ) from the long exact sequence in cohomology of the pair ( N , ∂ N ) (N,\partial N) ( N , ∂ N ) . The third row is the boundary map ∂ : H 2 ( M ∘ , ∂ M ∘ ) → H 1 ( ∂ M ∘ ) \partial:H_2(M^\circ,\partial M^\circ)\to H_1(\partial M^\circ) ∂ : H 2 ( M ∘ , ∂ M ∘ ) → H 1 ( ∂ M ∘ ) , followed by the map on H 1 H_1 H 1 induced by the identity i d : ∂ M ∘ → ∂ N \mathrm{id}:\partial M^\circ\to\partial N id : ∂ M ∘ → ∂ N , followed by the map H 1 ( ∂ N ) → H 1 ( N ) H_1(\partial N)\to H_1(N) H 1 ( ∂ N ) → H 1 ( N ) induced by inclusion.
We consider each square in the last diagram and show that it (anti-)commutes. Square (1) commutes, since both horizontal maps are the identity. The horizontal maps in square (2) are the boundary maps from the long exact sequences of the pairs ( M , M ∘ ) (M,M^\circ) ( M , M ∘ ) , respectively ( N , ∂ N ) (N,\partial N) ( N , ∂ N ) and the vertical maps are induced by the inclusion ( N , ∂ N ) ↪ ( M , M ∘ ) (N,\partial N)\hookrightarrow(M,M^\circ) ( N , ∂ N ) ↪ ( M , M ∘ ) . Thus, square (2) commutes by naturality of the long exact sequence of a pair. Square (3) commutes and square (5) anticommutes by naturality of Poincaré–Lefschetz duality with respect to the long exact sequences in homology and cohomology of a pair (see [2 Theorem 9.2] ). Square (4) anticommutes, by naturality of the cap product and the fact that ∂ M ∘ \partial M^\circ ∂ M ∘ and ∂ N \partial N ∂ N have opposite orientation, so [ ∂ M ∘ ] = − [ ∂ N ] [\partial M^\circ]=-[\partial N] [ ∂ M ∘ ] = − [ ∂ N ] . Square (6) commutes, by definition of Ψ \Psi Ψ .
Since (1), (2), (4), (5) commute up to sign, with precisely 2 of them reversing sign, it follows that going from H 2 ( M ∘ ) H^2(M^\circ) H 2 ( M ∘ ) to H 1 ( N ) H_1(N) H 1 ( N ) by first going right and then down is the same as going down and then to the right. Since squares (3) and (6) commute, this shows that Ψ = τ ∘ δ ∘ Φ \Psi=\tau\circ\delta\circ\Phi Ψ = τ ∘ δ ∘ Φ .
Step 7. Show that H 2 ( M ) F ≅ H 2 ( M ) / Z s H^2(M)^F\cong H^2(M)/\mathbb{Z}s H 2 ( M ) F ≅ H 2 ( M ) / Z s , where s = PD M [ σ 0 ( B ) ] s=\operatorname{PD}_M[\sigma_0(B)] s = PD M [ σ 0 ( B )] . Pairing with the fiber class induces the following short exact sequence:
0 ⟶ H 2 ( M ) F ⟶ H 2 ( M ) ⟶ Z ⟶ 0 , (13) 0\longrightarrow H^2(M)^F\longrightarrow H^2(M)\longrightarrow\mathbb{Z}\longrightarrow0, \tag*{(13)} 0 ⟶ H 2 ( M ) F ⟶ H 2 ( M ) ⟶ Z ⟶ 0 , (13)
and since ⟨ s , F ⟩ = 1 \langle s,F\rangle=1 ⟨ s , F ⟩ = 1 , the homomorphism φ : Z ⟶ H 2 ( M ) \varphi:\mathbb{Z}\longrightarrow H^2(M) φ : Z ⟶ H 2 ( M ) , φ ( k ) = k s \varphi(k)=ks φ ( k ) = k s induces a splitting of (13). Hence,
H 2 ( M ) ≅ H 2 ( M ) F ⊕ Z s H^2(M)\cong H^2(M)^F\oplus\mathbb{Z}s H 2 ( M ) ≅ H 2 ( M ) F ⊕ Z s
and thus
H 2 ( M ) F ≅ H 2 ( M ) / Z s . H^2(M)^F\cong H^2(M)/\mathbb{Z}s. H 2 ( M ) F ≅ H 2 ( M ) / Z s .
Step 8. Conclusion. By applying in order Proposition 5.2, Step 6, (12) and Step 7, we conclude
MW ( π ) = ker ( Ψ ) = ker ( τ 3 ∘ δ ∘ Φ ) ≅ H 2 ( X ) F / ⟨ c i , j ⟩ ≅ H 2 ( X ) / Triv ( π ) . \operatorname{MW}(\pi)=\ker(\Psi)=\ker(\tau_3\circ\delta\circ\Phi)\cong H^2(X)^F/\langle c_{i,j}\rangle\cong H^2(X)/\operatorname{Triv}(\pi). MW ( π ) = ker ( Ψ ) = ker ( τ 3 ∘ δ ∘ Φ ) ≅ H 2 ( X ) F / ⟨ c i , j ⟩ ≅ H 2 ( X ) / Triv ( π ) .
The isomorphism can be given explicitly as follows. Consider the commutative diagram
0 ⟶ H 2 ( M ) / Triv ( π ) ⟶ H 2 ( M ∘ ) F ⟶ ⨁ t ∈ Σ H 1 ( M t ) ⟶ 0 Φ 1 ↑ Φ ↑ id ↑ 0 ⟶ MW ( π ) ⟶ MW ( π ∘ ) ⟶ ⨁ t ∈ Σ H 1 ( M t ) ⟶ 0 , \begin{aligned}
0&\longrightarrow H^2(M)/\operatorname{Triv}(\pi)\longrightarrow H^2(M^\circ)^F\longrightarrow\bigoplus_{t\in\Sigma}H_1(M_t)\longrightarrow0\\
&\hspace{4.5cm}\Phi_1\uparrow\hspace{2.2cm}\Phi\uparrow\hspace{2.1cm}\operatorname{id}\uparrow\\
0&\longrightarrow\operatorname{MW}(\pi)\longrightarrow\operatorname{MW}(\pi^\circ)\longrightarrow\bigoplus_{t\in\Sigma}H_1(M_t)\longrightarrow0,
\end{aligned} 0 0 ⟶ H 2 ( M ) / Triv ( π ) ⟶ H 2 ( M ∘ ) F ⟶ t ∈ Σ ⨁ H 1 ( M t ) ⟶ 0 Φ 1 ↑ Φ ↑ id ↑ ⟶ MW ( π ) ⟶ MW ( π ∘ ) ⟶ t ∈ Σ ⨁ H 1 ( M t ) ⟶ 0 ,
where
Φ ( [ σ ] ) = PD ( M ∘ , ∂ M ∘ ) ( [ σ ] ) − PD ( M ∘ , ∂ M ∘ ) ( [ σ 0 ∣ B ∘ ] ) \Phi([\sigma])=\operatorname{PD}_{(M^\circ,\partial M^\circ)}([\sigma])-\operatorname{PD}_{(M^\circ,\partial M^\circ)}([\sigma_0|_{B^\circ}]) Φ ([ σ ]) = PD ( M ∘ , ∂ M ∘ ) ([ σ ]) − PD ( M ∘ , ∂ M ∘ ) ([ σ 0 ∣ B ∘ ])
for any [ σ ] ∈ MW ( π ∘ ) [\sigma]\in\operatorname{MW}(\pi^\circ) [ σ ] ∈ MW ( π ∘ ) , and
Φ 1 ( [ σ ] ) = [ PD M ( σ ) − PD M ( σ 0 ) ] ∈ H 2 ( M ) / Triv ( π ) \Phi_1([\sigma])=[\operatorname{PD}_M(\sigma)-\operatorname{PD}_M(\sigma_0)]\in H^2(M)/\operatorname{Triv}(\pi) Φ 1 ([ σ ]) = [ PD M ( σ ) − PD M ( σ 0 )] ∈ H 2 ( M ) / Triv ( π )
for any [ σ ] ∈ MW ( π ) [\sigma]\in\operatorname{MW}(\pi) [ σ ] ∈ MW ( π ) . By Proposition 3.2, Φ \Phi Φ is an isomorphism, so the short five-Lemma implies that Φ 1 \Phi_1 Φ 1 is also an isomorphism.
Proof of Theorem 1.6. Theorem 2.6 and Theorem 1.1 give the following commutative diagram
MW h o l ( π ) ⟶ MW ( π ) ↓ ≀ ↓ ≀ NS ( M ) / Triv ( π ) ⟶ H 2 ( M ) / Triv ( π ) . \begin{aligned}
\operatorname{MW}^{\mathrm{hol}}(\pi)&\longrightarrow\operatorname{MW}(\pi)\\
\downarrow\wr\hspace{1.3cm}&\hspace{1.3cm}\downarrow\wr\\
\operatorname{NS}(M)/\operatorname{Triv}(\pi)&\longrightarrow H^2(M)/\operatorname{Triv}(\pi).
\end{aligned} MW hol ( π ) ↓ ≀ NS ( M ) / Triv ( π ) ⟶ MW ( π ) ↓ ≀ ⟶ H 2 ( M ) / Triv ( π ) .
Since H 2 ( M ) / NS ( M ) H^2(M)/\operatorname{NS}(M) H 2 ( M ) / NS ( M ) is torsion-free, the bottom arrow induces the identity on the torsion part, yielding the conclusion.
Proof of Theorem 1.5. By Proposition 5.1, MW ( π ) \operatorname{MW}(\pi) MW ( π ) injects into MW ( π ∘ ) \operatorname{MW}(\pi^\circ) MW ( π ∘ ) . By Proposition 5.2, MW ( π ) = ker ( Ψ ) \operatorname{MW}(\pi)=\ker(\Psi) MW ( π ) = ker ( Ψ ) . Surjectivity of Ψ \Psi Ψ follows immediately from exactness of the short exact sequence (12) and the fact that Ψ = τ 3 ∘ δ ∘ Φ \Psi=\tau_3\circ\delta\circ\Phi Ψ = τ 3 ∘ δ ∘ Φ .
Applications
We give some explicit applications of Theorem 1.1 .
Proof of Corollary 1.2. If M M M is not a rational elliptic surface, [10 Corollary 1.10] implies that the rank of MW ( π ) \operatorname{MW}(\pi) MW ( π ) is strictly larger than that of MW h o l ( π ) \operatorname{MW}^{\mathrm{hol}}(\pi) MW hol ( π ) . If M M M is a rational elliptic surface, then NS ( M ) = H 2 ( M ) \operatorname{NS}(M)=H^{2}(M) NS ( M ) = H 2 ( M ) , so Theorem 2.6 and Theorem 1.1 yield the conclusion. □
We conclude by elaborating on Example 1.4 and Example 1.3 from the introduction, thus providing a complete computation of the Mordell–Weil group of these K3 surfaces as a direct application of Theorem 1.1 .
Example 5.5 (Mordell–Weil group of a Kummer surface). Consider two non-isogenous elliptic curves E 1 , E 2 E_{1}, E_{2} E 1 , E 2 with hyperelliptic involutions ι 1 , ι 2 \iota_{1},\iota_{2} ι 1 , ι 2 . Let M : = Km ( E 1 × E 2 ) M:=\operatorname{Km}(E_{1}\times E_{2}) M := Km ( E 1 × E 2 ) be the minimal resolution of ( E 1 × E 2 ) / ( ι 1 × ι 2 ) (E_{1}\times E_{2})/(\iota_{1}\times\iota_{2}) ( E 1 × E 2 ) / ( ι 1 × ι 2 ) . This can be viewed as an elliptic surface π : M → P 1 \pi\colon M\to\mathbb{P}^{1} π : M → P 1 with 4 singular fibers of type I 0 ∗ I_{0}^{*} I 0 ∗ , by considering projection p 1 : E 1 × E 2 → E 1 p_{1}\colon E_{1}\times E_{2}\to E_{1} p 1 : E 1 × E 2 → E 1 and the diagram
E 1 × E 2 → / ( ι 1 × ι 2 ) M p 1 ↓ ↓ π E 1 → / ι 1 P 1 \begin{CD}
E_{1}\times E_{2} @>{/(\iota_{1}\times\iota_{2})}>> M \\
@V{p_{1}}VV @VV{\pi}V \\
E_{1} @>{/\iota_{1}}>> \mathbb{P}^{1}
\end{CD} E 1 × E 2 p 1 ↓ ⏐ E 1 / ( ι 1 × ι 2 ) / ι 1 M ↓ ⏐ π P 1 where the horizontal arrows are rational maps. For 1 ≤ i ≤ 4 1\leq i\leq4 1 ≤ i ≤ 4 , let a i a_{i} a i and b i b_{i} b i denote the fixed points of ι 1 \iota_{1} ι 1 , respectively ι 2 \iota_{2} ι 2 . A section of p 1 p_{1} p 1 is s : E 1 → E 1 × E 2 s\colon E_{1}\to E_{1}\times E_{2} s : E 1 → E 1 × E 2 , given by s ( x ) = ( x , b 1 ) s(x)=(x,b_{1}) s ( x ) = ( x , b 1 ) . Assume that the zero-section σ 0 : P 1 → M \sigma_{0}\colon\mathbb{P}^{1}\to M σ 0 : P 1 → M is induced by s s s . We construct an explicit presentation for H 2 ( M ; Z ) H_{2}(M;\mathbb{Z}) H 2 ( M ; Z ) . For more details see [1 Chapter VIII, Section 5] and [15 Section 2.2] .
Let A i : = ( E 1 × { b i } ) / ( ι 1 × 1 ) A_{i}:=(E_{1}\times\{b_{i}\})/(\iota_{1}\times1) A i := ( E 1 × { b i }) / ( ι 1 × 1 ) and B i : = ( { a i } × E 2 ) / ( 1 × ι 2 ) B_{i}:=(\{a_{i}\}\times E_{2})/(1\times\iota_{2}) B i := ({ a i } × E 2 ) / ( 1 × ι 2 ) . The minimal resolution of ( E 1 × E 2 ) / ( ι 1 × ι 2 ) (E_{1}\times E_{2})/(\iota_{1}\times\iota_{2}) ( E 1 × E 2 ) / ( ι 1 × ι 2 ) is obtained by replacing a neighborhood of the image of ( a i , b j ) ∈ E 1 × E 2 (a_{i},b_{j})\in E_{1}\times E_{2} ( a i , b j ) ∈ E 1 × E 2 by the normal bundle of a sphere C i , j C_{i,j} C i , j of self-intersection − 2 -2 − 2 . For i = 1 , 2 i=1,2 i = 1 , 2 let α i \alpha_{i} α i and β i \beta_{i} β i be simple loops, such that α i \alpha_{i} α i are setwise invariant under the involution ι 1 \iota_{1} ι 1 and β i \beta_{i} β i are setwise invariant under ι 2 \iota_{2} ι 2 . Assume that α 1 ⋅ α 2 = 1 \alpha_{1}\cdot\alpha_{2}=1 α 1 ⋅ α 2 = 1 and β 1 ⋅ β 2 = 1 \beta_{1}\cdot\beta_{2}=1 β 1 ⋅ β 2 = 1 and the homology classes of α i \alpha_{i} α i and β i \beta_{i} β i are generators of H 1 ( E 1 ) H_{1}(E_{1}) H 1 ( E 1 ) and H 1 ( E 2 ) H_{1}(E_{2}) H 1 ( E 2 ) respectively. The product α i × β j \alpha_{i}\times\beta_{j} α i × β j is a torus in E 1 × E 2 E_{1}\times E_{2} E 1 × E 2 containing 4 fixed points of ι 1 × ι 2 \iota_{1}\times\iota_{2} ι 1 × ι 2 . Let D i , j ′ D'_{i,j} D i , j ′ denote the image of α i × β j − { fixed points } \alpha_{i}\times\beta_{j}-\{\text{fixed points}\} α i × β j − { fixed points } in M M M . By construction, D i , j ′ D'_{i,j} D i , j ′ is a 4 times punctured sphere. Let D i , j D_{i,j} D i , j be the closed surface in M M M obtained by capping the four punctures of D i , j ′ D'_{i,j} D i , j ′ .
As divisors, the singular fibers of π \pi π are 2 B i + ∑ j = 1 4 C i , j 2B_{i}+\sum_{j=1}^{4}C_{i,j} 2 B i + ∑ j = 1 4 C i , j for 1 ≤ i ≤ 4 1\leq i\leq4 1 ≤ i ≤ 4 and the zero-section is σ 0 = A 1 \sigma_{0}=A_{1} σ 0 = A 1 . Let F F F denote the fiber class of π \pi π . Thus,
PD M ( Triv ( π ) ) = Z ⟨ A 1 , F ⟩ ⊕ Z ⟨ B i : 1 ≤ i ≤ 4 ⟩ ⊕ Z ⟨ C i , j : 1 ≤ i ≤ 4 and 2 ≤ j ≤ 4 ⟩ . \operatorname{PD}_{M}(\operatorname{Triv}(\pi))=\mathbb{Z}\langle A_{1},F\rangle\oplus\mathbb{Z}\langle B_{i}:1\leq i\leq4\rangle\oplus\mathbb{Z}\langle C_{i,j}:1\leq i\leq4\text{ and }2\leq j\leq4\rangle. PD M ( Triv ( π )) = Z ⟨ A 1 , F ⟩ ⊕ Z ⟨ B i : 1 ≤ i ≤ 4 ⟩ ⊕ Z ⟨ C i , j : 1 ≤ i ≤ 4 and 2 ≤ j ≤ 4 ⟩ . All fibers are equal in homology, yielding the equation
2 B i + ∑ j = 1 4 C i , j = F for 1 ≤ i ≤ 4. (14) 2B_{i}+\sum_{j=1}^{4}C_{i,j}=F\text{ for }1\leq i\leq4. \tag*{(14)} 2 B i + j = 1 ∑ 4 C i , j = F for 1 ≤ i ≤ 4. (14) Let G G G be the fiber class of the fibration we would obtain from the projection E 1 × E 2 → E 2 E_{1}\times E_{2}\to E_{2} E 1 × E 2 → E 2 . Again, fibers are equal in homology, yielding the equation
2 A j + ∑ i = 1 4 C i , j = G for 1 ≤ j ≤ 4. (15) 2A_{j}+\sum_{i=1}^{4}C_{i,j}=G\text{ for }1\leq j\leq4. \tag*{(15)} 2 A j + i = 1 ∑ 4 C i , j = G for 1 ≤ j ≤ 4. (15) Summing the equations in (14) over i i i and the ones in (15) over j j j yields the equation
2 ∑ i = 1 4 A i + 2 ∑ i = 1 4 B i + 2 ∑ i , j = 1 4 C i , j = 4 F + 4 G . 2\sum_{i=1}^{4}A_{i}+2\sum_{i=1}^{4}B_{i}+2\sum_{i,j=1}^{4}C_{i,j}=4F+4G. 2 i = 1 ∑ 4 A i + 2 i = 1 ∑ 4 B i + 2 i , j = 1 ∑ 4 C i , j = 4 F + 4 G .
Since H 2 ( M ; Z ) H_{2}(M;\mathbb{Z}) H 2 ( M ; Z ) is torsion-free, this simplifies to
∑ i = 1 4 A i + ∑ i = 1 4 B i + ∑ i , j = 1 4 C i , j − 2 F − 2 G = 0. (16) \sum_{i=1}^{4} A_i+\sum_{i=1}^{4} B_i+\sum_{i,j=1}^{4} C_{i,j}-2F-2G=0. \tag*{(16)} i = 1 ∑ 4 A i + i = 1 ∑ 4 B i + i , j = 1 ∑ 4 C i , j − 2 F − 2 G = 0. (16)
Let L L L be the abelian group generated by
A i , B i , C i , j , D k , l , F , G for 1 ≤ i , j ≤ 4 , 1 ≤ k , l ≤ 2 A_i,B_i,C_{i,j},D_{k,l},F,G\text{ for }1\leq i,j\leq4,1\leq k,l\leq2 A i , B i , C i , j , D k , l , F , G for 1 ≤ i , j ≤ 4 , 1 ≤ k , l ≤ 2
with relations (14) , (15) and (16) . By construction, L L L is a sublattice of H 2 ( M ; Z ) H_{2}(M;\mathbb{Z}) H 2 ( M ; Z ) . It can be checked that L ≅ Z 22 L\cong\mathbb{Z}^{22} L ≅ Z 22 and together with the intersection form, L L L is unimodular. Hence L = H 2 ( M ; Z ) L=H_{2}(M;\mathbb{Z}) L = H 2 ( M ; Z ) .
By Theorem 1.1 and Poincaré duality,
MW ( π ) ≅ H 2 ( M ) / Triv ( π ) ≅ H 2 ( M ) / PD M ( Triv ( π ) ) . \operatorname{MW}(\pi)\cong H^{2}(M)/\operatorname{Triv}(\pi)\cong H_{2}(M)/\operatorname{PD}_{M}(\operatorname{Triv}(\pi)). MW ( π ) ≅ H 2 ( M ) / Triv ( π ) ≅ H 2 ( M ) / PD M ( Triv ( π )) .
The explicit presentations above imply that MW ( π ) \operatorname{MW}(\pi) MW ( π ) is isomorphic to the group generated by
A 2 , A 3 , D k , l for 1 ≤ k , l ≤ 2 A_{2},A_{3},D_{k,l}\text{ for }1\leq k,l\leq2 A 2 , A 3 , D k , l for 1 ≤ k , l ≤ 2
with relations
2 A 2 = 2 A 3 = 0. 2A_{2}=2A_{3}=0. 2 A 2 = 2 A 3 = 0.
Hence,
MW ( π ) ≅ Z 4 × Z / 2 × Z / 2. \operatorname{MW}(\pi)\cong\mathbb{Z}^{4}\times\mathbb{Z}/2\times\mathbb{Z}/2. MW ( π ) ≅ Z 4 × Z /2 × Z /2.
This highlights the difference to the holomorphic case, where MW h o l ( π ) ≅ Z / 2 × Z / 2 \operatorname{MW}^{\mathrm{hol}}(\pi)\cong\mathbb{Z}/2\times\mathbb{Z}/2 MW hol ( π ) ≅ Z /2 × Z /2 .
Example 5.6 (Mordell–Weil group of an Inose surface). Let p : R → P s 1 p:R\to\mathbb{P}^{1}_{s} p : R → P s 1 be the elliptic surface given as the minimal resolution of y 2 = x 3 − 3 x + s − 6 y^{2}=x^{3}-3x+s^{-6} y 2 = x 3 − 3 x + s − 6 with zero-section σ 0 \sigma_{0} σ 0 at infinity. This is a rational elliptic surface with critical values 4 , 8 , ∞ 4,8,\infty 4 , 8 , ∞ and singular fibers of type I 1 , I 1 I_{1},I_{1} I 1 , I 1 , respectively I I ∗ II^{*} I I ∗ . Consider the branched double cover f : P t 1 → P s 1 f:\mathbb{P}^{1}_{t}\to\mathbb{P}^{1}_{s} f : P t 1 → P s 1 given by f ( t ) = t + t − 1 f(t)=t+t^{-1} f ( t ) = t + t − 1 . The branch values are s = ± 2 s=\pm2 s = ± 2 , neither of which is a singular value of p p p , so pulling the elliptic fibration p p p back over f f f yields an elliptically fibered K3 surface π : M → P t 1 \pi:M\to\mathbb{P}^{1}_{t} π : M → P t 1 with two singular fibers of type I I ∗ II^{*} I I ∗ and four singular fibers of type I 1 I_{1} I 1 , see Figure 9 .
Let C 0 , 1 , … , C 0 , 8 C_{0,1},\ldots,C_{0,8} C 0 , 1 , … , C 0 , 8 and C ∞ , 1 , … , C ∞ , 8 C_{\infty,1},\ldots,C_{\infty,8} C ∞ , 1 , … , C ∞ , 8 denote the irreducible components of the two fibers of type I I ∗ II^{*} I I ∗ which do not intersect σ 0 \sigma_{0} σ 0 . Let F F F denote a generic fiber. Then C 0 , i , C ∞ , i , F C_{0,i},C_{\infty,i},F C 0 , i , C ∞ , i , F and σ 0 \sigma_{0} σ 0 span the unimodular lattice
E 8 ( − 1 ) ⊕ E 8 ( − 1 ) ⊕ ( 0 1 1 − 2 ) E_{8}(-1)\oplus E_{8}(-1)\oplus
\begin{pmatrix}
0 & 1\\
1 & -2
\end{pmatrix} E 8 ( − 1 ) ⊕ E 8 ( − 1 ) ⊕ ( 0 1 1 − 2 ) in H 2 ( M ) H_{2}(M) H 2 ( M ) .
In order to determine the remaining 4 generators, let D D D be a disk in P s 1 \mathbb{P}^{1}_{s} P s 1 containing the branch values of f f f but none of the critical values of p p p , as in Figure 9 . The preimage A : = f − 1 ( D ) ⊂ P t 1 A:=f^{-1}(D)\subset\mathbb{P}^{1}_{t} A := f − 1 ( D ) ⊂ P t 1 is an annulus containing no critical values of π \pi π . Pick a point c ∈ ∂ D c\in\partial D c ∈ ∂ D and fix paths in P s 1 − D \mathbb{P}^{1}_{s}-D P s 1 − D from c c c to the critical values 4 , 8 , ∞ 4,8,\infty 4 , 8 , ∞ of p p p with mutually disjoint interiors, containing no other critical values of p p p . Let α , β ⊂ p − 1 ( c ) \alpha,\beta\subset p^{-1}(c) α , β ⊂ p − 1 ( c ) be the vanishing cycles corresponding to the two nodal fibers of p p p . These have algebraic intersection number 1. Let Δ α , Δ β \Delta_{\alpha},\Delta_{\beta} Δ α , Δ β be their vanishing thimbles in R R R and assume that α , β , Δ α , Δ β \alpha,\beta,\Delta_{\alpha},\Delta_{\beta} α , β , Δ α , Δ β are disjoint from σ 0 \sigma_{0} σ 0 . Pick a trivialization of the torus-bundle p : p − 1 ( D ) → D p:p^{-1}(D)\to D p : p − 1 ( D ) → D that preserves the zero-section. This induces a trivialization of π \pi π over A A A .
Let γ \gamma γ be the central circle in the annulus A A A . Two further generators of H 2 ( M ) H_{2}(M) H 2 ( M ) are given by the embedded tori T α : = α × γ T_{\alpha}:=\alpha\times\gamma T α := α × γ and T β : = β × γ T_{\beta}:=\beta\times\gamma T β := β × γ . Let f − 1 ( c ) = { b − , b + } f^{-1}(c)=\{b_{-},b_{+}\} f − 1 ( c ) = { b − , b + } . The pullback of Δ α \Delta_{\alpha} Δ α to M M M consists of two thimbles Δ + \Delta_{+} Δ + and Δ − \Delta_{-} Δ − with boundaries corresponding to the loop α \alpha α in M b + M_{b_{+}} M b + , respectively M b − M_{b_{-}} M b − . The points b + b_{+} b + and b − b_{-} b − lie on different boundary components of A A A . Let η \eta η be a properly embedded arc joining them, which intersects γ \gamma γ transversely. The trivialization of π \pi π over the annulus A A A gives a cylinder α × η \alpha\times\eta α × η in M M M . Together with this cylinder, the two thimbles glue to a continuously embedded sphere S α S_{\alpha} S α in M M M , which can be smoothed. An analogous construction can be done for the preimage of Δ β \Delta_{\beta} Δ β , yielding a sphere S β S_{\beta} S β .
Figure 9. The Inose surface π : M → P s 1 \pi:M\to\mathbb{P}^{1}_{s} π : M → P s 1 is obtained by pulling back the rational elliptic surface p : R → P s 1 p:R\to\mathbb{P}^{1}_{s} p : R → P s 1 with 2 nodal fibers and one fiber of type I I ∗ II^{*} I I ∗ . The branch values of f : P t 1 → P s 1 f:\mathbb{P}^{1}_{t}\to\mathbb{P}^{1}_{s} f : P t 1 → P s 1 are regular points of p p p , so the singular fibers are doubled in M M M : there are four nodal fibers and two fibers of type I I ∗ II^{*} I I ∗ . The two pullbacks of a Lefschetz thimble of a nodal fiber of p p p together with a cylinder in π − 1 ( A ) \pi^{-1}(A) π − 1 ( A ) glue together to the embedded sphere S α S_{\alpha} S α .
By construction T α , T β , S α , S β T_{\alpha},T_{\beta},S_{\alpha},S_{\beta} T α , T β , S α , S β do not intersect the first 18 generators we gave, so it suffices to show that these four homology classes generate a unimodular lattice in H 2 ( M ) H_{2}(M) H 2 ( M ) . Choosing a circle γ ′ \gamma' γ ′ parallel to γ \gamma γ in A A A gives [ T α ] = [ α × γ ′ ] [T_{\alpha}]=[\alpha\times\gamma'] [ T α ] = [ α × γ ′ ] , showing that the algebraic intersection numbers satisfy T α ⋅ T β = 0 T_{\alpha}\cdot T_{\beta}=0 T α ⋅ T β = 0 , T α ⋅ T α = 0 T_{\alpha}\cdot T_{\alpha}=0 T α ⋅ T α = 0 and T β ⋅ T β = 0 T_{\beta}\cdot T_{\beta}=0 T β ⋅ T β = 0 . Observe that the algebraic intersection number of one of the tori with one of the spheres is equal to the algebraic intersection number of the vanishing cycles used in their respective construction. Hence, the intersection form on the lattice spanned by T α , T β , S α , S β T_{\alpha},T_{\beta},S_{\alpha},S_{\beta} T α , T β , S α , S β is
( 0 0 0 1 0 0 − 1 ∗ 0 1 ∗ ∗ − 1 ∗ ∗ ∗ ) \begin{pmatrix}
0 & 0 & 0 & 1 \\
0 & 0 & -1 & * \\
0 & 1 & * & * \\
-1 & * & * & *
\end{pmatrix} 0 0 0 − 1 0 0 1 ∗ 0 − 1 ∗ ∗ 1 ∗ ∗ ∗
so this lattice is unimodular.
The homology classes C 0 , 1 , … , C 0 , 8 , C ∞ , 1 , … , C ∞ , 8 , F , σ 0 , T α , T β , S α , S β C_{0,1},\ldots,C_{0,8},C_{\infty,1},\ldots,C_{\infty,8},F,\sigma_{0},T_{\alpha},T_{\beta},S_{\alpha},S_{\beta} C 0 , 1 , … , C 0 , 8 , C ∞ , 1 , … , C ∞ , 8 , F , σ 0 , T α , T β , S α , S β span a full rank unimodular sublattice of the unimodular lattice H 2 ( M ) H_{2}(M) H 2 ( M ) , so they span the entire H 2 ( M ) H_{2}(M) H 2 ( M ) . The trivial lattice is spanned by the Poincaré duals of C 0 , 1 , … , C 0 , 8 , C ∞ , 1 , … , C ∞ , 8 , F , σ 0 C_{0,1},\ldots,C_{0,8},C_{\infty,1},\ldots,C_{\infty,8},F,\sigma_{0} C 0 , 1 , … , C 0 , 8 , C ∞ , 1 , … , C ∞ , 8 , F , σ 0 , so Theorem 1.1 implies
MW ( π ) ≅ Z 4 \operatorname{MW}(\pi)\cong\mathbb{Z}^{4} MW ( π ) ≅ Z 4
and is generated by the Poincaré duals of T α , T β , S α , S β T_{\alpha},T_{\beta},S_{\alpha},S_{\beta} T α , T β , S α , S β .