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Nearly Lefschetz Fibrations

Updated 7 July 2026
  • Nearly Lefschetz fibrations are controlled generalizations of classical Lefschetz fibrations, allowing additional singular behavior such as connected round folds.
  • They enhance monodromy and section theory by integrating ordinary Lefschetz points with exotic fibers, overcoming classical constraints in near-symplectic 4-manifolds.
  • Recent studies link explicit genus‑1 normal forms, spin structure criteria, and boundary decompositions to classify these fibrations and their symplectic fillings.

Auroux, Donaldson and Katzarkov introduced broken Lefschetz fibrations as a generalization of Lefschetz fibrations in order to describe near-symplectic 4-manifolds (Hayano, 2010). In the literature considered here, nearly Lefschetz fibrations are controlled relaxations of genuine Lefschetz fibrations in which one allows a prescribed additional singular behavior beyond isolated ordinary Lefschetz points. For closed 4-manifolds this appears as the simplified broken Lefschetz fibration, with isolated Lefschetz singularities together with a connected circle of indefinite-fold, or round, singularities (Hayano, 2011). In recent symplectic filling theory, a nearly Lefschetz fibration over the disk is a smooth map on a compact 4-manifold with corners whose singularities consist of ordinary Lefschetz points and finitely many exotic fibers locally modeled on {y2=x}\{y^2=x\}, producing spinal rather than classical open books on the boundary (Plamenevskaya et al., 28 Jul 2025). Across these settings, the extra singularity enlarges the available monodromy, section theory, and filling theory beyond the classical Lefschetz regime.

1. Definitions and local models

A broken Lefschetz fibration f ⁣:MBf\colon M\to B, where MM is an oriented 4-manifold and BB an oriented surface, is a smooth map whose only critical points are Lefschetz singularities and indefinite folds. In compatible complex local coordinates (z1,z2)(z_1,z_2) on MM and ξ\xi on BB, a Lefschetz singularity is modeled by

f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,

while in real coordinates (t,x1,x2,x3)(t,x_1,x_2,x_3) on f ⁣:MBf\colon M\to B0 and f ⁣:MBf\colon M\to B1 on f ⁣:MBf\colon M\to B2, an indefinite fold is modeled by

f ⁣:MBf\colon M\to B3

The isolated Lefschetz points are denoted f ⁣:MBf\colon M\to B4, and the indefinite folds form a connected 1-manifold f ⁣:MBf\colon M\to B5 (Hayano, 2011).

A broken Lefschetz fibration f ⁣:MBf\colon M\to B6 is called simplified when three conditions hold: f ⁣:MBf\colon M\to B7 is injective, f ⁣:MBf\colon M\to B8 is a single embedded circle and all fibers are connected, and all Lefschetz critical points lie on the higher-genus side. Under these hypotheses, f ⁣:MBf\colon M\to B9 is the disjoint union of two disks MM0, the fibers over them differ in genus by one, and the region over a tubular neighborhood of MM1 is the round cobordism (Hayano, 2011). In the genus-1 case, the higher side has genus MM2, the lower side genus MM3, and the round cobordism can be described handle-theoretically as an untwisted or twisted round 1-handle, equivalently a pair of ordinary 1- and 2-handles attached with algebraic intersection zero or two on the belt sphere (Hayano, 2010).

The recent disk-based notion is formulated differently. Let MM4 be a compact 4-manifold with corners and boundary decomposition

MM5

A nearly Lefschetz fibration over MM6 is a smooth map MM7 such that over the interior of MM8 it is a fibration with connected fiber MM9, its restriction to BB0 is exactly this surface bundle, it has finitely many ordinary Lefschetz critical points locally modeled on BB1, and finitely many exotic fibers locally modeled on the branched-cover curve BB2, equivalently by

BB3

Away from the exotic fibers, BB4 carries BB5 to BB6 as a smooth bundle (Plamenevskaya et al., 28 Jul 2025).

These two formalisms are not identical, but both replace the rigidity of genuine Lefschetz fibrations by one additional singular mechanism. This suggests that “nearly Lefschetz” is best understood as a controlled departure from the honest Lefschetz category rather than as a single universally fixed local model.

2. Monodromy and boundary structures

For a simplified broken Lefschetz fibration, the higher-side restriction

BB7

is an honest genus-BB8 Lefschetz fibration with vanishing cycles BB9 and Hurwitz sequence

(z1,z2)(z_1,z_2)0

If (z1,z2)(z_1,z_2)1 is the vanishing cycle of the indefinite fold, then Baykur’s analysis shows that the total monodromy around (z1,z2)(z_1,z_2)2 preserves (z1,z2)(z_1,z_2)3 and lies in the kernel of the cut-along-(z1,z2)(z_1,z_2)4 map

(z1,z2)(z_1,z_2)5

Conversely, any factorization (z1,z2)(z_1,z_2)6 gives a simplified broken Lefschetz fibration with indefinite-fold vanishing cycle (z1,z2)(z_1,z_2)7 (Hayano, 2011). The round cobordism is built by first attaching a fiberwise 2-handle along the nonseparating curve (z1,z2)(z_1,z_2)8 with fiber framing and then a 3-handle, so the monodromy condition and the handle picture are tightly linked.

For nearly Lefschetz fibrations over (z1,z2)(z_1,z_2)9, the monodromy contains two kinds of generators. Ordinary critical values determine vanishing cycles, that is, embedded closed curves in the fiber about which the monodromy is a positive Dehn twist. Exotic fibers determine vanishing arcs, along which the monodromy is a positive boundary-interchange, namely a half-twist swapping two boundary components of the page. As a result, the monodromy lives not in the ordinary mapping class group alone but in the spinal mapping class group generated by Dehn twists and boundary-interchanges (Plamenevskaya et al., 28 Jul 2025).

This distinction is reflected on the boundary. A standard Lefschetz fibration over MM0 induces a classical open book, in which each binding component appears once in the boundary of each page. A nearly Lefschetz fibration induces instead a spinal open book: the 3-manifold decomposes as

MM1

where MM2 is a bundle with page MM3, MM4 is a union of solid tori, and each page can meet a torus in multiple longitudes. The multiplicities of these longitudes are part of the boundary data (Plamenevskaya et al., 28 Jul 2025). In this sense, the passage from standard to nearly Lefschetz fibrations is simultaneously a change in local singularity theory and in the global boundary category.

3. Sections and the failure of classical Lefschetz constraints

For relatively minimal genuine Lefschetz fibrations MM5 of genus MM6, classical constraints are stringent. Smith proved that there are only finitely many homotopy classes of sections MM7, and Smith and Stipsicz independently proved that every section satisfies

MM8

unless the fibration is the trivial product MM9 (Hayano, 2011).

Hayano showed that neither phenomenon survives in the simplified broken setting. For every ξ\xi0, there exists a nontrivial genus-ξ\xi1 simplified broken Lefschetz fibration

ξ\xi2

with no ξ\xi3-sphere in any fiber and with infinitely many pairwise non-homotopic sections ξ\xi4 (Hayano, 2011). The construction chooses a simple closed curve ξ\xi5, takes the Hurwitz system ξ\xi6, and selects the indefinite-fold cycle ξ\xi7 so that ξ\xi8. The resulting Kirby diagram presents

ξ\xi9

The sections BB0 are obtained by trivializing over the lower-genus side the boundary torus of BB1 with winding number BB2 around one fundamental loop in BB3. A computation of BB4 then shows that these section classes are all distinct.

Hayano also proved that for any integer BB5 and any BB6 there exists a nontrivial genus-BB7 simplified broken Lefschetz fibration admitting a section BB8 with

BB9

(Hayano, 2011). The monodromy-based construction works on f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,0, choosing a nonseparating curve f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,1 and curves f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,2 so that

f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,3

where f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,4 is the boundary circle. Kas’s handle-attachment construction gives a Lefschetz fibration over f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,5, after which one attaches the round 2-handle along f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,6 and caps with a trivial f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,7 piece to obtain a closed simplified broken Lefschetz fibration over f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,8. The section is then read off from the handle picture.

These results indicate that the finiteness of section homotopy classes and the negativity of section square are not features of “broken” or “nearly” Lefschetz theory in general; they are genuinely classical Lefschetz phenomena, destroyed by the presence of the round singularity.

4. Spin structures and obstruction theory

Let f(z1,z2)=ξ=z1z2,f(z_1,z_2)=\xi=z_1z_2,9 be a genus-(t,x1,x2,x3)(t,x_1,x_2,x_3)0 simplified broken Lefschetz fibration with Lefschetz vanishing cycles (t,x1,x2,x3)(t,x_1,x_2,x_3)1 and round-vanishing cycle (t,x1,x2,x3)(t,x_1,x_2,x_3)2. Suppose (t,x1,x2,x3)(t,x_1,x_2,x_3)3 admits a dual class (t,x1,x2,x3)(t,x_1,x_2,x_3)4 to a lower-side fiber (t,x1,x2,x3)(t,x_1,x_2,x_3)5, meaning

(t,x1,x2,x3)(t,x_1,x_2,x_3)6

This hypothesis holds, for example, whenever the higher-plus-round region is simply connected, or if the fibration has a section (Hayano, 2011).

Hayano’s spin criterion states that (t,x1,x2,x3)(t,x_1,x_2,x_3)7 admits a spin structure if and only if two conditions hold. First, there exists a (t,x1,x2,x3)(t,x_1,x_2,x_3)8-quadratic form

(t,x1,x2,x3)(t,x_1,x_2,x_3)9

with respect to the intersection pairing on f ⁣:MBf\colon M\to B00 such that

f ⁣:MBf\colon M\to B01

Second, the self-intersection f ⁣:MBf\colon M\to B02 is even (Hayano, 2011).

Equivalently, the monodromy data determine the relevant contribution to the second Stiefel-Whitney class f ⁣:MBf\colon M\to B03 through the quadratic form f ⁣:MBf\colon M\to B04, while the only additional global obstruction is the parity of the dual class f ⁣:MBf\colon M\to B05. In the genuine Lefschetz case, where there is no round singularity, the condition reduces to the usual Stipsicz-Gompf criterion f ⁣:MBf\colon M\to B06. The extra requirement f ⁣:MBf\colon M\to B07 isolates precisely how the round vanishing cycle enters the obstruction theory.

This criterion is structurally significant because it shows that the broken setting retains a mapping-class-group formulation of spin obstructions, but only after incorporating data from the non-Lefschetz singularity. The obstruction theory therefore parallels the classical one without coinciding with it.

5. Genus-f ⁣:MBf\colon M\to B08 normal forms and low-complexity classification

The genus-f ⁣:MBf\colon M\to B09 case admits a particularly explicit description because the mapping class group f ⁣:MBf\colon M\to B10 is identified with f ⁣:MBf\colon M\to B11. Writing

f ⁣:MBf\colon M\to B12

a genus-f ⁣:MBf\colon M\to B13 simplified broken Lefschetz fibration with f ⁣:MBf\colon M\to B14 Lefschetz critical points has a Hurwitz system

f ⁣:MBf\colon M\to B15

where each f ⁣:MBf\colon M\to B16 is a right-handed Dehn twist f ⁣:MBf\colon M\to B17 along a slope f ⁣:MBf\colon M\to B18, and the product

f ⁣:MBf\colon M\to B19

is the boundary monodromy of the higher-side torus bundle (Hayano, 2010). Because that torus bundle has a section, the monodromy fixes one slope, hence

f ⁣:MBf\colon M\to B20

for some integer f ⁣:MBf\colon M\to B21.

Hayano proved that after simultaneous conjugations and elementary Hurwitz moves, the higher-side monodromy can be put in the normal form

f ⁣:MBf\colon M\to B22

that is, a block

f ⁣:MBf\colon M\to B23

followed by a twisted block

f ⁣:MBf\colon M\to B24

(Hayano, 2010). For f ⁣:MBf\colon M\to B25, the allowable twisted blocks are exactly the standard sequences

f ⁣:MBf\colon M\to B26

f ⁣:MBf\colon M\to B27

and for f ⁣:MBf\colon M\to B28,

f ⁣:MBf\colon M\to B29

with

f ⁣:MBf\colon M\to B30

This leads to a complete classification for the low-complexity range f ⁣:MBf\colon M\to B31. When f ⁣:MBf\colon M\to B32, only f ⁣:MBf\colon M\to B33 occurs. When f ⁣:MBf\colon M\to B34, the possibilities are f ⁣:MBf\colon M\to B35 or f ⁣:MBf\colon M\to B36. When f ⁣:MBf\colon M\to B37, the possibilities are f ⁣:MBf\colon M\to B38, f ⁣:MBf\colon M\to B39, or f ⁣:MBf\colon M\to B40; in the purely Lefschetz limit, f ⁣:MBf\colon M\to B41 connects to the elliptic-surface picture, and when the round handle is absent the standard 12f ⁣:MBf\colon M\to B42-term factorization recovers the elliptic surfaces f ⁣:MBf\colon M\to B43 (Hayano, 2010).

The diffeomorphism types of the total spaces are obtained by Kirby calculus. The families f ⁣:MBf\colon M\to B44 realize

f ⁣:MBf\colon M\to B45

while the families f ⁣:MBf\colon M\to B46 realize

f ⁣:MBf\colon M\to B47

where f ⁣:MBf\colon M\to B48 or f ⁣:MBf\colon M\to B49 (Hayano, 2010). The numerical invariants are correspondingly explicit: f ⁣:MBf\colon M\to B50 since the round handle contributes zero to f ⁣:MBf\colon M\to B51, and in the pure f ⁣:MBf\colon M\to B52 case the signature is f ⁣:MBf\colon M\to B53. Hayano further conjectured that the families f ⁣:MBf\colon M\to B54 and f ⁣:MBf\colon M\to B55, together with their possible f ⁣:MBf\colon M\to B56 summands, exhaust all genus-f ⁣:MBf\colon M\to B57 simplified broken Lefschetz fibrations with non-empty round locus (Hayano, 2010).

In the symplectic-topological setting of sandwiched singularities, nearly Lefschetz fibrations over the disk are tied to spinal open books and filling classification. A spinal open book on a 3-manifold f ⁣:MBf\colon M\to B58 is a decomposition

f ⁣:MBf\colon M\to B59

where f ⁣:MBf\colon M\to B60 is a bundle with compact surface pages f ⁣:MBf\colon M\to B61 with boundary, and f ⁣:MBf\colon M\to B62 is the spine, glued so that each page meets each torus in a collection of longitudes, possibly more than one. When the spine is a union of solid tori and the pages are planar, the open book is called planar uniform over f ⁣:MBf\colon M\to B63, and each binding component carries a multiplicity f ⁣:MBf\colon M\to B64 equal to the number of longitudes contributed by a page (Plamenevskaya et al., 28 Jul 2025).

Roy, Min, and Wang, building on work of Lisi, Van Horn-Morris, and Wendl, proved that if f ⁣:MBf\colon M\to B65 is supported by a planar spinal open book uniform over f ⁣:MBf\colon M\to B66, then any minimal strong or Stein filling f ⁣:MBf\colon M\to B67 admits the structure of a positive allowable nearly Lefschetz fibration inducing that spinal open book on f ⁣:MBf\colon M\to B68; moreover, the number of exotic fibers is determined solely by the binding multiplicities (Plamenevskaya et al., 28 Jul 2025). This theorem supplies the passage from contact boundary data to nearly Lefschetz structures.

The corresponding filling constructions are encoded by immersed disk arrangements

f ⁣:MBf\colon M\to B69

subject to three conditions: each f ⁣:MBf\colon M\to B70 is a simple branched cover; all self-intersections and mutual intersections are positive transverse multipoints, with every branch point or intersection marked; and the total number of marked points on f ⁣:MBf\colon M\to B71 equals a prescribed weight f ⁣:MBf\colon M\to B72 (Plamenevskaya et al., 28 Jul 2025). After blowing up the f ⁣:MBf\colon M\to B73 marked points, the strict transforms f ⁣:MBf\colon M\to B74 become a multisection of the blown-up trivial fibration, and the complement

f ⁣:MBf\colon M\to B75

carries a natural positive allowable nearly Lefschetz fibration. Ordinary singular fibers come from blowing down intersections, and exotic fibers come from branch points. The monodromy around an ordinary critical value is a Dehn twist enclosing exactly the holes corresponding to the disks meeting there, while the monodromy around an exotic value is a boundary-interchange of the two adjacent holes.

This framework yields two central existence statements. First, if f ⁣:MBf\colon M\to B76 is compatible with the decorated germ f ⁣:MBf\colon M\to B77 of a sandwiched singularity, then f ⁣:MBf\colon M\to B78 admits a Stein structure filling the canonical contact link. Second, every minimal strong symplectic filling of the contact link of a sandwiched singularity arises, up to deformation, as some f ⁣:MBf\colon M\to B79, equivalently via a positive allowable nearly Lefschetz fibration whose vanishing cycles and arcs can be packaged into a braided wiring diagram, and conversely a wiring diagram produces an immersed-disk arrangement (Plamenevskaya et al., 28 Jul 2025).

The same formalism detects unexpected Stein fillings, namely Stein fillings not diffeomorphic, indeed not homeomorphic, to any Milnor fiber of any analytic smoothing. The incidence matrix

f ⁣:MBf\colon M\to B80

records how many marked points each f ⁣:MBf\colon M\to B81 carries. Akhmedov, Ozbagci, and Popescu-Pampu show topologically that any two fillings with the same boundary marking have the same matrix, while de Jong–van Straten’s algebraic picture deformations impose additional constraints on realizable matrices. For the decorated germ consisting of f ⁣:MBf\colon M\to B82 lines through the origin in f ⁣:MBf\colon M\to B83, each weighted f ⁣:MBf\colon M\to B84, one obtains at least f ⁣:MBf\colon M\to B85 pairwise non-homeomorphic Stein fillings by choosing DJVS arrangements with incidence matrices not realizable by any complex picture deformation; each such filling carries its unique positive allowable nearly Lefschetz fibration, with monodromy factoring as a product of boundary-interchanges followed by Dehn twists (Plamenevskaya et al., 28 Jul 2025).

In this symplectic-filling context, nearly Lefschetz fibrations generalize planar Lefschetz fibrations to the spinal setting, arise naturally from complements of multisections, and parametrize all minimal symplectic fillings of sandwiched contact links, including Stein fillings outside the classical algebraic Milnor-fiber picture.

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