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Invariant Subvarieties of Minimal Homological Dimension, Zero Lyapunov Exponents, and Monodromy

Paul Apisa

1. Introduction

Over a finite cover of the moduli space, g\mathcal{M}_{g}, of genus gg Riemann surfaces there are two well-studied vector bundles. One, denoted Ωg\Omega\mathcal{M}_{g}, is a gg-dimensional complex vector bundle whose fiber over a Riemann surface XgX\in\mathcal{M}_{g} is the vector space of holomorphic one-forms on XX. The other, which we denote HH, is the 2g2g-dimensional real vector bundle whose fiber over XX is H1(X,)H^{1}(X,\mathbb{R}). This bundle is equipped with the Gauss-Manin connection. Let H1H_{\mathbb{R}}^{1} denote the pullback of HH to Ωg\Omega\mathcal{M}_{g}.

The space Ωg\Omega\mathcal{M}_{g} is equipped with a GL(2,)\mathrm{GL}(2,\mathbb{R}) action induced from complex scalar multiplication and Teichmüller geodesic flow and admits an invariant stratification by specifying the number and order of zeros of the holomorphic one-forms.

Parallel transport by the Gauss-Manin connection over Teichmüller geodesics induces a cocycle on H1H_{\mathbb{R}}^{1} called the Kontsevich-Zorich cocycle. Zorich [Zor99] and Forni [For02] demonstrated that the Lyapunov exponents of this cocycle govern the deviations of ergodic averages along straight line flow on flat surfaces and Forni [For02] connected these exponents to the geometry of g\mathcal{M}_{g}, a topic elaborated upon in Forni-Matheus-Zorich [FMZ14a].

Homological Dimension of an Invariant Subvariety

Given an SL(2,)\mathrm{SL}(2,\mathbb{R}) invariant measure on a stratum of Ωg\Omega\mathcal{M}_{g}, one could ask for the Lyapunov exponents of the Kontsevich-Zorich cocycle.

By work of Eskin and Mirzakhani [EM18], every SL(2,)\mathrm{SL}(2,\mathbb{R}) ergodic invariant measure is Lebesgue measure restricted to invariant subvarieties (the fact that the support of such a measures is a subvariety and not simply a sub-orbifold is due to Filip [Fil16]). Forni’s criterion (see [For02] and [For11]) states that for such measures the number of nonzero Lyapunov exponents of the Kontsevich-Zorich cocycle is bounded below by twice the homological dimension.

Definition 1.1.

Given an invariant subvariety \mathcal{M}, its homological dimension is the maximum, taken over all horizontally periodic surfaces (X,ω)(X,\omega)\in\mathcal{M}, of the dimension of the span in H1(X,)H^{1}(X,\mathbb{R}) of the core curves of horizontal cylinders on (X,ω)(X,\omega).

While the homological dimension of an invariant subvariety \mathcal{M} is often difficult to compute, it is bounded below by a more tractable quantity, called the rank of \mathcal{M}, which we define now. The tangent space of an invariant subvariety \mathcal{M} at a point (X,ω)(X,\omega), where XX is a Riemann surface and ω\omega a holomorphic one-form on it, can be identified with a subspace of H1(X,Σ;)H^{1}\left(X,\Sigma;\mathbb{C}\right) where Σ\Sigma is the collection of zeros of ω\omega. Letting p:H1(X,Σ;)H1(X;)p:H^{1}\left(X,\Sigma;\mathbb{C}\right)\operatorname{\rightarrow}H^{1}(X;\mathbb{C}) be the projection to absolute cohomology, work of Avila-Eskin-Möller [AEM17] states that p(T(X,ω))p\left(T_{(X,\omega)}\mathcal{M}\right) is a complex symplectic subspace.

Definition 1.2.

The rank of an invariant subvariety \mathcal{M} is half the dimension of p(T(X,ω))p\left(T_{(X,\omega)}\mathcal{M}\right), where (X,ω)(X,\omega)\in\mathcal{M}. The rel of \mathcal{M} is the dimension of the kernel of pT(X,ω)p\restriction_{T_{(X,\omega)}\mathcal{M}}. The definitions are independent of the choice of point in \mathcal{M}.

Building on work of Eskin, Mirzakhani, and Mohammadi [EMM15] and Smillie-Weiss [SW04], Wright [Wri15] showed that the homological dimension of an invariant subvariety is always bounded below by its rank. This observation inspires the following definition.

Definition 1.3.

An invariant subvariety \mathcal{M} is said to have minimal homological dimension if its rank and homological dimension coincide.

Remark 1.4.

In Apisa-Wright [AWa, Example 2.5], it was shown that there are infinitely many examples of invariant subvarieties of every rank and every dimension that have minimal homological dimension, although this terminology is not used there. These examples include the infinite sequence of square-tiled surfaces studied by Matheus-Yoccoz [MY10]. Moreover, these examples are nontrivial in the sense that if \mathcal{M} is one such example, then it is not full rank, i.e. it is not the case that Ωg\mathcal{M}\subseteq\Omega\mathcal{M}_{g} and rank()=g\mathrm{rank}(\mathcal{M})=g. If \mathcal{M} is full rank then it automatically has minimal homological dimension and, by Mirzakhani-Wright [MW18], it is a component of a stratum of Abelian differentials or a hyperelliptic loci therein.

Our first theorem is a characterization of invariant subvarieties of minimal homological dimension.

Theorem 1.5.

If \mathcal{M} has minimal homological dimension then it is either a component of a stratum of Abelian differentials or a full locus of covers of the hyperelliptic locus in a stratum of Abelian differentials.

Moreover, if rank()>1\mathrm{rank}(\mathcal{M})>1, then after marking all periodic points, \mathcal{M} is hh-geminal.

Remark 1.6.

The definition of hh-geminal first appeared in Apisa-Wright [AWa, Definition 4.3] and will be recalled in Section 6. Knowing that \mathcal{M} is hh-geminal places strong constraints on the covers of which the surfaces in \mathcal{M} are the domain.

The definition of periodic point best adapted to our purposes here is the one in Apisa-Wright [AWc]. Note that, in Theorem 1.5, when periodic points are marked, this only requires marking finitely many points by Eskin-Filip-Wright [EFW18, Theorem 1.5] (see Apisa-Wright [AWc, Section 4.2] for a discussion).

Finally, when \mathcal{M} has rank one, Theorem 1.5 is equivalent to the statement that \mathcal{M} is a locus of torus covers. This is a consequence of Wright [Wri15, Theorem 1.9] and the fact that loci of torus covers are precisely rank one invariant subvarieties with field of definition \mathbb{Q}. This enables us to exclusively consider invariant subvarieties of rank at least two in the proof of Theorem 1.5.

A tool used in the proof of Theorem 1.5 is the following (note that the definition of \mathcal{M}-parallelism is recalled in Definition 2.1).

Theorem 1.7.

\mathcal{M} has minimal homological dimension if and only if any two \mathcal{M}-parallel cylinders have homologous core curves.

Theorems 1.5 and 1.7 answer a question of Mirzakhani-Wright [MW18, Question 1.7] which asks what invariant subvarieties \mathcal{M} of rank at least two have the property that any two \mathcal{M}-parallel cylinders have homologous core curves.

Vanishing Lyapunov Exponents of the Kontsevich-Zorich Cocycle

Since the rank, rr, of an invariant subvariety, Ωg\mathcal{M}\subseteq\Omega\mathcal{M}_{g}, is a lower bound on its homological dimension, Forni’s criterion (and the cylinder deformation theorem of Wright [Wri15]) implies that at most 2g2r2g-2r Lyapunov exponents of the Kontsevich-Zorich cocycle for Lebesgue measure on \mathcal{M} vanish. (Note that if equality holds, then \mathcal{M} has minimal homological dimension).

There are two known invariant subvarieties that are not full rank, i.e rgr\neq g, and that have 2g2r2g-2r zero Lyapunov exponents. These are the Eierlegende-Wollmilchsau (independently studied by Forni [For06] and Herrlich-Schmithüsen [HS08]) and the Ornithorynque (studied by Forni-Matheus [FM], see also Forni-Matheus-Zorich [FMZ11]). Both of these subvarieties are Teichmüller curves and hence rank one111The projections of the Eierlegende-Wollmilchsau and Ornithorynque to g\mathcal{M}_{g} are the families of compact Riemann surfaces defined by yd=x(x1)(xt)y^{d}=x(x-1)(x-t), where t1{0,1,}t\in\mathbb{P}^{1}-\{0,1,\infty\}, for d=4d=4 and d=6d=6 respectively. McMullen [McM13, Theorem 8.3] identified rigid factors in the Jacobian of these families that also explain the vanishing of 2g22g-2 Lyapunov exponents.. Building on work of Möller [Möl11], recent work of Aulicino-Norton [AN20b] showed that these examples are the only rank one invariant subvarieties with 2g22g-2 vanishing exponents. Via Theorem 1.5, we extend this to the following.

Theorem 1.8.

Let Ωg\mathcal{M}\subseteq\Omega\mathcal{M}_{g} be an invariant subvariety of rank rr. Then \mathcal{M} has 2g2r2g-2r zero Lyapunov exponents (which is the maximum possible given the rank of \mathcal{M}) if and only if \mathcal{M} is the Eierlegende-Wollmilchsau, the Ornithorynque, or full rank.

Remark 1.9.

The backwards implication is an immediate consequence of Filip [Fil17, Corollary 1.7 (ii)] (for full rank), Forni [For06] (for the Eierlegende-Wollmilchsau), and Forni-Matheus [FM] (for the Ornithorynque).

The proof will show that if \mathcal{M} has rank r>1r>1, is not full rank, and has minimal homological dimension then there are never 2g2r2g-2r zero Lyapunov exponents. This reduces Theorem 1.8 to the work of Aulicino-Norton [AN20b] and Möller [Möl11] mentioned above. We would like to stress that the present work relies on Aulicino-Norton for the rank one case and does not offer a new proof of their result.

To implement this proof strategy we rely on properties of geminal varieties shown in Apisa-Wright [AWa] and use the non-varying phenomena and formulas for sums of Lyapunov exponents found in Eskin-Kontsevich-Zorich [EKZ14].

Monodromy

Let \mathcal{M} be an invariant subvariety. Since p(T)p(T\mathcal{M}) is complex-symplectic (by Avila-Eskin-Möller [AEM17]) letting WW be the subbundle of H1H_{\mathbb{R}}^{1}\restriction_{\mathcal{M}} that is symplectically orthogonal to p(T)p(T\mathcal{M}), implies that

H1=p(T)W.H_{\mathbb{R}}^{1}\restriction_{\mathcal{M}}=p(T\mathcal{M})\oplus W.

The Zariski closure of the monodromy of p(T)p(T\mathcal{M}) is the full symplectic group by Filip [Fil17, Corollary 1.7 (i)]. However, the monodromy of WW is mysterious.

By Filip [Fil17, Corollary 1.7 (ii)], there are no zero Lyapunov exponents in p(T)p(T\mathcal{M}). This implies that outside of the three exceptions listed in Theorem 1.8, the Lyapunov exponents of the Kontsevich-Zorich cocycle restricted to WW are not all zero. An immediate corollary is the following.

Corollary 1.10.

The Zariski closure of the monodromy of the bundle WW over \mathcal{M} belongs to a compact group if and only if \mathcal{M} is one of the following: the Eierlegende-Wollmilchsau, the Ornithorynque, or full rank (in which case WW is a zero-dimensional bundle and the claim is vacuous).

Context

Many authors have studied the occurrence of zero Lyapunov exponents in the spectrum of the Kontsevich-Zorich cocycle. Filip proved in [Fil17] that zero Lyapunov exponents “arise from monodromy”. The problem of which invariant subvarieties have completely degenerate Lyapunov spectra was solved in Aulicino-Norton [AN20b]. Further examples of invariant subvarieties with zero exponents were constructed by Forni-Matheus-Zorich [FMZ14b] and Grivaux-Hubert [GH14]. At the other end of the spectrum, Avila-Viana [AV07] proved the simplicity of the Lyapunov spectrum for Masur-Veech measure on strata.

For work on sums of Lyapunov exponents see Eskin-Kontsevich-Zorich [EKZ14]. For work on the Lyapunov spectrum of Veech surfaces see Bouw-Möller [BM10], Eskin-Kontsevich-Zorich [EKZ11] and Forni-Matheus-Zorich [FMZ11] (for square-tiled surfaces), and Bainbridge [Bai07] (for genus two). Bainbridge’s work builds on McMullen’s classification of SL(2,)\mathrm{SL}(2,\mathbb{R})-invariant probability measures in genus two [McM07].

An infinite collection of square-tiled surfaces with homological dimension one was produced by Matheus-Yoccoz [MY10]. McMullen [McM] introduced a notion similar to that of a square-tiled surface having homological dimension one, namely square-tiled surfaces in which every cusp has rank one. These surfaces are precisely the ones for which any sequence of closed flat geodesics, whose lengths tend to infinity, equidistribute on the surface, see McMullen [McM, Theorem 9.1] for a precise statement of a stronger result.

Finally, exponents have recently been connected to the wind-tree model, see Delecroix-Hubert-Lelièvre [DHL14].

Acknowledgments. The author is grateful to Alex Wright, David Aulicino, and Curt McMullen for helpful conversations and comments. During the preparation of this paper, the author was partially supported by NSF Postdoctoral Fellowship DMS 1803625.

2. Preliminaries on cylinder deformations

In this section we will summarize a collection of results on cylinder deformations. To avoid repetition, throughout this section we will let (X,ω)(X,\omega) be a translation surface in an invariant subvariety \mathcal{M}. We will also let Σ\Sigma denote the singularities and marked points of ω\omega.

Definition 2.1.

A cylinder on (X,ω)(X,\omega) is a maximal open embedded Euclidean cylinder. Two parallel cylinders on (X,ω)(X,\omega) are said to be \mathcal{M}-equivalent (or sometimes \mathcal{M}-parallel) if they remain parallel on all surfaces in some neighborhood of (X,ω)(X,\omega) in \mathcal{M} (see Wright [Wri15, Remark 4.2] for an explanation of the formal meaning of a cylinder persisting in a neighborhood of a translation surface). Two cylinder equivalence classes are disjoint if every cylinder in one equivalence class is disjoint from every cylinder in the other. A cylinder is called generic if all of the saddle connections on its boundary remain parallel to the core curve of the cylinder in a neighborhood of (X,ω)(X,\omega) in \mathcal{M}. An equivalence class of cylinders 𝐂\mathbf{C} on (X,ω)(X,\omega) in \mathcal{M} is called generic if it consists of generic cylinders and if there is an open neighborhood of (X,ω)(X,\omega) in \mathcal{M} on which 𝐂\mathbf{C} remains an equivalence class (and not just a subset of one).

Definition 2.2.

Given a collection of disjoint cylinders 𝐂\mathbf{C} on (X,ω)(X,\omega), let {γC}C𝐂\{\gamma_{C}\}_{C\in\mathbf{C}} be the oriented core curves of the cylinders in 𝐂\mathbf{C} and let hCh_{C} denote the height of cylinder CC. The standard deformation is defined to be σ𝐂:=C𝐂hCγC\sigma_{\mathbf{C}}:=\sum_{C\in\mathbf{C}}h_{C}\gamma_{C}^{*} where γC\gamma_{C}^{*} is the element of H1(X,Σ;)H^{1}(X,\Sigma;\mathbb{C}) that sends a homology class to its oriented intersection number with γC\gamma_{C}. When 𝐂\mathbf{C} is horizontal we will also call σ𝐂\sigma_{\mathbf{C}} the standard shear and iσ𝐂i\sigma_{\mathbf{C}} the standard dilation.

The twist space, denoted Twist(𝐂,)\mathrm{Twist}\left(\mathbf{C},\mathcal{M}\right), is the collection of all vT(X,ω)v\in T_{(X,\omega)}\mathcal{M} that can be written as C𝐂aCγC\sum_{C\in\mathbf{C}}a_{C}\gamma_{C}^{*} where aCa_{C}\in\mathbb{C}. The support of vv is the collection of cylinders CC with aC0a_{C}\neq 0.

The main theorem of Wright [Wri15, Theorem 1.1], called the cylinder deformation theorem, says that if 𝐂\mathbf{C} is an \mathcal{M}-equivalence class on (X,ω)(X,\omega) then σ𝐂\sigma_{\mathbf{C}} belongs to T(X,ω)T_{(X,\omega)}\mathcal{M}.

Building on the cylinder deformation theorem, Mirzakhani and Wright [MW17, Theorem 1.5] characterized the vectors that belong to the twist space of an equivalence class 𝐂\mathbf{C} as follows.

Theorem 2.3.

Every element of Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) can be written uniquely as the sum of a multiple of σ𝐂\sigma_{\mathbf{C}} and an element of ker(p)\ker(p).

We will now prove a result about the structure of the twist space.

Lemma 2.4.

Suppose that 𝐂1\mathbf{C}_{1} and 𝐂2\mathbf{C}_{2} are \mathcal{M}-equivalence classes of cylinders on (X,ω)(X,\omega). Let (X,ω)(X^{\prime},\omega^{\prime}) be a surface in \mathcal{M} on which the cylinders in 𝐂i\mathbf{C}_{i} persist and belong to a (possibly larger) equivalence class 𝐂i\mathbf{C}_{i}^{\prime} of cylinders for i{1,2}i\in\{1,2\}. If 𝐂1\mathbf{C}_{1} and 𝐂2\mathbf{C}_{2} are disjoint equivalence classes, then so are 𝐂1\mathbf{C}_{1}^{\prime} and 𝐂2\mathbf{C}_{2}^{\prime}.

Proof.

Two equivalence classes 𝐃1\mathbf{D}_{1} and 𝐃2\mathbf{D}_{2} are disjoint if and only if the symplectic pairing of p(σ𝐃1)p(\sigma_{\mathbf{D}_{1}}) and p(σ𝐃2)p(\sigma_{\mathbf{D}_{2}}) is zero. Let σi\sigma_{i} denote the standard deformation in 𝐂i\mathbf{C}_{i} on (X,ω)(X,\omega) and note that this cohomology class does not belong to ker(p)\ker(p). Therefore, by Theorem 2.3, on (X,ω)(X^{\prime},\omega^{\prime}), p(σi)p(\sigma_{i}) is collinear to p(σ𝐂i)p(\sigma_{\mathbf{C}_{i}^{\prime}}). Since the symplectic pairing of p(σ1)p(\sigma_{1}) and p(σ2)p(\sigma_{2}) is zero the same holds for p(σ𝐂1)p(\sigma_{\mathbf{C}_{1}^{\prime}}) and p(σ𝐂2)p(\sigma_{\mathbf{C}_{2}^{\prime}}). ∎

Lemma 2.5.

Suppose that (X,ω)(X,\omega) has a collection {𝐂i}i=1n\{\mathbf{C}_{i}\}_{i=1}^{n} of pairwise disjoint equivalence classes. Set 𝐂:=i=1n𝐂i\mathbf{C}:=\bigcup_{i=1}^{n}\mathbf{C}_{i}. Then

Twist(𝐂,)=i=1nTwist(𝐂i,).\mathrm{Twist}(\mathbf{C},\mathcal{M})=\bigoplus_{i=1}^{n}\mathrm{Twist}(\mathbf{C}_{i},\mathcal{M}).
Proof.

Let vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) and write it as i=1nvi\sum_{i=1}^{n}v_{i} where vi=C𝐂iaCγCv_{i}=\sum_{C\in\mathbf{C}_{i}}a_{C}\gamma_{C}^{*} where aCa_{C}\in\mathbb{C} and γC\gamma_{C}^{*} is the Poincare dual of the core curve of CC. By symmetry of hypotheses, it suffices to show that v1Twist(𝐂1,)v_{1}\in\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M}). Perturb (X,ω)(X,\omega) to a nearby surface (X,ω)(X^{\prime},\omega^{\prime}) where all the cylinders in 𝐂i\mathbf{C}_{i} persist and belong to a generic equivalence class 𝐂i\mathbf{C}_{i}^{\prime} of cylinders. By Lemma 2.4, {𝐂i}i=1n\{\mathbf{C}_{i}^{\prime}\}_{i=1}^{n} remains a collection of pairwise disjoint equivalence classes. Since vv pairs trivially with the core curves in 𝐂i\mathbf{C}_{i}, it also pairs trivially with those in 𝐂i\mathbf{C}_{i}^{\prime}. The twist space decomposition [AWb, Proposition 4.20] implies that v=η𝐂1+η(X,ω)\𝐂1v=\eta_{\mathbf{C}_{1}^{\prime}}+\eta_{(X,\omega)\backslash\mathbf{C}_{1}^{\prime}} where η𝐂1Twist(𝐂1,)\eta_{\mathbf{C}_{1}^{\prime}}\in\mathrm{Twist}(\mathbf{C}_{1}^{\prime},\mathcal{M}), and η(X,ω)𝐂1T(X,ω)()\eta_{(X,\omega)\setminus\mathbf{C}_{1}^{\prime}}\in T_{(X,\omega)}(\mathcal{M}) evaluates to zero on every saddle connection in 𝐂1¯\overline{\mathbf{C}_{1}^{\prime}}. Moreover, this decomposition is unique, in that if v=v+v′′v=v^{\prime}+v^{\prime\prime} where v=C𝐂1bCγCv^{\prime}=\sum_{C\in\mathbf{C}_{1}^{\prime}}b_{C}\gamma_{C}^{*} where bCb_{C}\in\mathbb{C} and v′′v^{\prime\prime} is a cohomology class that evaluates to zero on every saddle connection in 𝐂1¯\overline{\mathbf{C}_{1}^{\prime}}, then v=η𝐂1v^{\prime}=\eta_{\mathbf{C}_{1}^{\prime}} and v′′=η(X,ω)\𝐂1v^{\prime\prime}=\eta_{(X,\omega)\backslash\mathbf{C}_{1}^{\prime}}. Since v=v1+(i=2nvi)v=v_{1}+\left(\sum_{i=2}^{n}v_{i}\right) is such a decomposition (this uses that {𝐂i}i=1n\{\mathbf{C}_{i}^{\prime}\}_{i=1}^{n} is a collection of pairwise disjoint equivalence classes), v1=η𝐂1Twist(𝐂1,)v_{1}=\eta_{\mathbf{C}_{1}^{\prime}}\in\mathrm{Twist}(\mathbf{C}_{1}^{\prime},\mathcal{M}) as desired. ∎

2.1. Cylindrical Stability

An important tool in the sequel is \mathcal{M}-cylindrical stability, originally defined in Aulicino-Nguyen [AN20a, Definition 2.4].

Definition 2.6.

A surface (X,ω)(X,\omega) is called \mathcal{M}-cylindrically stable if it is horizontally periodic and, letting 𝐂\mathbf{C} denote the collection of horizontal cylinders, Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) coincides with the space Pres((X,ω),)\mathrm{Pres}\left((X,\omega),\mathcal{M}\right), defined to be the cohomology classes in T(X,ω)T_{(X,\omega)}\mathcal{M} that evaluate to zero on the core curve of every horizontal cylinder.

The following properties of cylindrically stable surfaces were first shown in Wright [Wri15]. Recall that the field 𝐤()\mathbf{k}(\mathcal{M}) is defined to be the smallest extension of \mathbb{Q} needed to define \mathcal{M} by linear equations in period coordinates. Recall too that rel():=dim()2rank()\mathrm{rel}(\mathcal{M}):=\dim(\mathcal{M})-2\mathrm{rank}(\mathcal{M}).

Lemma 2.7.

The following hold:

  1. (1)

    Any horizontally periodic surface in \mathcal{M} has at most rank()+rel()\mathrm{rank}(\mathcal{M})+\mathrm{rel}(\mathcal{M}) equivalence classes of cylinders. If rel()=0\mathrm{rel}(\mathcal{M})=0, then any cylindrically stable surface in \mathcal{M} has precisely this many horizontal equivalence classes.

  2. (2)

    If a surface is cylindrically stable, then the horizontal core curves span a subset of T(X,ω)()T_{(X,\omega)}(\mathcal{M})^{*} of dimension rank()\operatorname{rank}(\mathcal{M}).

  3. (3)

    If 𝐤()={\mathbf{k}}(\mathcal{M})=\mathbb{Q}, every surface in \mathcal{M} can be perturbed to become cylindrically stable and square-tiled in such a way that all horizontal cylinders on the original surface stay horizontal in the perturbation.

  4. (4)

    Given a collection of horizontal cylinders 𝐂\mathbf{C} on a surface (X,ω)(X,\omega) in \mathcal{M} there is a path in \mathcal{M} from (X,ω)(X,\omega) to a cylindrically stable surface (X,ω)(X^{\prime},\omega^{\prime}) along which the cylinders in 𝐂\mathbf{C} persist and remain horizontal.

Proof.

The first claim follows immediately from the cylinder deformation theorem and Apisa-Wright [AWb, Lemma 7.10 (2) and (3)]. The second and third claims are simply Apisa-Wright [AWb, Lemma 7.10 (4) and (6)]. We sketch a proof of the final claim following Wright [Wri15].

The method for producing (X,ω)(X^{\prime},\omega^{\prime}) is iterative and proceeds as follows. Begin by applying Smillie-Weiss [SW04, Cor. 6] to produce a horizontally periodic surface (X1,ω1)(X_{1},\omega_{1}) in the horocycle orbit closure of (X,ω)(X,\omega) on which the cylinders in 𝐂\mathbf{C} persist (it is possible to connect (X,ω)(X,\omega) to (X1,ω1)(X_{1},\omega_{1}) by following the horocycle flow of (X,ω)(X,\omega) until coming arbitrarily close to (X1,ω1)(X_{1},\omega_{1}) and then perturbing). Let 𝐂1\mathbf{C}_{1} denote the collection of horizontal cylinders on (X1,ω1)(X_{1},\omega_{1}). If Twist(𝐂1,)=Pres((X1,ω1),)\mathrm{Twist}\left(\mathbf{C}_{1},\mathcal{M}\right)=\mathrm{Pres}\left((X_{1},\omega_{1}),\mathcal{M}\right), then we are done.

If we are not done at stage nn, then let vv be a purely imaginary element of Pres((Xn,ωn),)Twist(𝐂n,)\mathrm{Pres}\left((X_{n},\omega_{n}),\mathcal{M}\right)-\mathrm{Twist}\left(\mathbf{C}_{n},\mathcal{M}\right). By [Wri15, Sublemma 8.7], if we travel from (Xn,ωn)(X_{n},\omega_{n}) in \mathcal{M} any sufficiently small amount in the direction of the tangent vector vv we produce a surface (Xn,ωn)(X_{n}^{\prime},\omega_{n}^{\prime}) where the cylinders in 𝐂n\mathbf{C}_{n} persist and remain horizontal, but do not cover all of the (Xn,ωn)(X_{n}^{\prime},\omega_{n}^{\prime}). Applying Smillie-Weiss [SW04, Cor. 6] again we produce a horizontally periodic surface (Xn+1,ωn+1)(X_{n+1},\omega_{n+1}) in the horocycle orbit closure of (Xn,ωn)(X_{n},\omega_{n}) on which the cylinders in 𝐂n\mathbf{C}_{n} persist and remain horizontal, but are a strict subset of the horizontal cylinders 𝐂n+1\mathbf{C}_{n+1}. When the process terminates we have found the desired surface. The previous two paragraphs are essentially contained in [Wri15, Proof of Lemma 8.6]. ∎

2.2. The Mirzakhani-Wright Partial Compactification

In Mirzakhani-Wright [MW17], a partial compactification was constructed for every invariant subvariety \mathcal{M}. The main feature is the boundary tangent formula, which we state now.

Suppose that (Xn,ωn)(X_{n},\omega_{n}) is a sequence of translation surfaces that converge in the Mirzakhani-Wright partial compactification to a surface (X,ω)(X_{\infty},\omega_{\infty}) in a component \mathcal{M}^{\prime} of the boundary. By Mirzakhani-Wright [MW17, Proposition 2.4] there is a map, called the collapse map, fn:(Xn,ωn)(X,ω)f_{n}:(X_{n},\omega_{n})\operatorname{\rightarrow}(X_{\infty},\omega_{\infty}) that takes the singular set of ωn\omega_{n} to the singular set of ω\omega_{\infty}. Given the collapse map, the collection of vanishing cyclesVn\emph{vanishing cycles}\ V_{n}, is defined to be the kernel of (fn):H1(Xn,Σn)H1(X,Σ)(f_{n})_{*}:H_{1}(X_{n},\Sigma_{n})\operatorname{\rightarrow}H_{1}(X_{\infty},\Sigma_{\infty}) where Σi\Sigma_{i} denotes the singular set of ωi\omega_{i}.

The following is due to Mirzakhani-Wright [MW17, Theorem 2.9] when (X,ω)(X_{\infty},\omega_{\infty}) is connected and Chen-Wright [CW19, Theorem 1.2 (see also Proposition 2.5)] when (X,ω)(X_{\infty},\omega_{\infty}) is disconnected.

Theorem 2.8.

For large enough nn, fnf_{n}^{*} induces an isomorphism,

T(X,ω)T(Xn,ωn)Ann(Vn)T_{(X_{\infty},\omega_{\infty})}\mathcal{M}^{\prime}\cong T_{(X_{n},\omega_{n})}\mathcal{M}\cap\mathrm{Ann}(V_{n})

where Ann(Vn)\mathrm{Ann}(V_{n}) denotes the cohomology classes in H1(Xn,Σn)H^{1}(X_{n},\Sigma_{n}) that evaluate to zero on the elements of VnV_{n}.

The following is the form in which we will primarily use the previous result.

Theorem 2.9.

Suppose that (Xn,ωn)(X_{n},\omega_{n}) is a sequence in \mathcal{M} converging to (X,ω)(X_{\infty},\omega_{\infty}) in a component \mathcal{M}^{\prime} of the boundary of \mathcal{M}. Let fn:(Xn,ωn)(X,ω)f_{n}:(X_{n},\omega_{n})\operatorname{\rightarrow}(X_{\infty},\omega_{\infty}) be the collapse maps.

  1. (1)

    If CC is a cylinder on (X,ω)(X_{\infty},\omega_{\infty}), then for sufficiently large nn, there is a cylinder CnC_{n} whose modulus, height, and circumference converge to that of CC and so fn(Cn)f_{n}(C_{n}) is homotopic to CC.

  2. (2)

    If CnC_{n} is a cylinder on (Xn,ωn)(X_{n},\omega_{n}) whose height and circumference are bounded below and above, then there is a cylinder CC on (X,ω)(X_{\infty},\omega_{\infty}) so that fn(Cn)f_{n}(C_{n}) is homotopic to CC for sufficiently large nn.

  3. (3)

    Suppose that 𝐂\mathbf{C} is a collection of cylinders on (X,ω)(X_{\infty},\omega_{\infty}). For sufficiently large nn, let fn(𝐂)f_{n}^{*}(\mathbf{C}) be the cylinders on (Xn,ωn)(X_{n},\omega_{n}) produced by (1) corresponding to the cylinders in 𝐂\mathbf{C}. Then fnf_{n}^{*} induces an isomorphism from Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}^{\prime}) to Twist(fn(𝐂),)\mathrm{Twist}(f_{n}^{*}(\mathbf{C}),\mathcal{M}).

Proof.

The first two claims are Mirzakhani-Wright [MW17, Lemma 2.15]. Given a cylinder CC let γC\gamma_{C}^{*} denote the cohomology class that records intersections with the core curve of CC. For the final claim, notice that, if \mathcal{H} is the stratum containing (X,ω)(X_{\infty},\omega_{\infty}), then γCT(X,ω)\gamma_{C}^{*}\in T_{(X_{\infty},\omega_{\infty})}\mathcal{H}. Letting CnC_{n} be as in (1), it follows from Theorem 2.8 that γCnAnn(Vn)\gamma_{C_{n}}^{*}\in\mathrm{Ann}(V_{n}). In particular, Twist(fn(𝐂),)Ann(Vn)\mathrm{Twist}(f_{n}^{*}(\mathbf{C}),\mathcal{M})\subseteq\mathrm{Ann}(V_{n}), so the result follows by Theorem 2.8. ∎

In general it can be cumbersome to establish convergence in the Mirzakhani-Wright partial compactification, but it is straightforward in the following case.

Definition 2.10.

Suppose that 𝐂\mathbf{C} is an equivalence class of generic cylinders on a surface (X,ω)(X,\omega) in an invariant subvariety \mathcal{M}. Let vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) so that there is a number tv>0t_{v}>0 so that the collapse path, i.e. (X,ω)+tv(X,\omega)+tv for t[0,tv)t\in[0,t_{v}), diverges as tt approaches tvt_{v} and so that each cylinder in 𝐂\mathbf{C} persists along the collapse path. By Apisa-Wright [AWb, Lemma 4.9], this sequence converges in the Mirzakhani-Wright partial compactification to a surface Colv(X,ω)\operatorname{Col}_{v}(X,\omega) in a component v\mathcal{M}_{v} of the boundary of \mathcal{M}. We will let 𝐂v\mathbf{C}_{v} denote the cylinders in 𝐂\mathbf{C} whose height go to zero along the collapse path.

Similarly, when 𝐂\mathbf{C} is collection of horizontal cylinders with σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M}, we will define Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) to be the limit of the path (X,ω)t(iσ𝐂)(X,\omega)-t(i\sigma_{\mathbf{C}}) for t[0,1)t\in[0,1) regardless of whether or not this path diverges. The surface Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) can be thought of as the result of vertically collapsing 𝐂\mathbf{C}. Moreover, this definition makes sense for any collection of cylinders 𝐂\mathbf{C} (by rotating the surface so the cylinders in 𝐂\mathbf{C} are horizontal, collapsing, and then rotating back). When 𝐂\mathbf{C} contains a vertical saddle connection, Col𝐂(X,ω)=Colv(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega)=\operatorname{Col}_{v}(X,\omega) for v=iσ𝐂v=-i\sigma_{\mathbf{C}} and we will let 𝐂\mathcal{M}_{\mathbf{C}} denote v\mathcal{M}_{v}.

In the sequel we will rely on the general theory of cylinder degenerations developed in Apisa-Wright [AWb, Section 4]. We begin by making the following definitions.

Definition 2.11.

Suppose that 𝐂\mathbf{C} is an equivalence class cylinders on a surface (X,ω)(X,\omega) in an invariant subvariety \mathcal{M}. Say that 𝐂\mathbf{C} is involved with rel if some vector in ker(p)T(X,ω)()\ker(p)\cap T_{(X,\omega)}(\mathcal{M}) evaluates non-trivially on a cross curve of a cylinder in 𝐂\mathbf{C}.

Let vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}). Say that vv is typical if all the cylinders in 𝐂v\mathbf{C}_{v} have ratios of heights that are constant on a neighborhood of (X,ω)(X,\omega) in \mathcal{M}.

Remark 2.12.

Note that if 𝐂\mathbf{C} is horizontal and vv is typical, then after perhaps shearing the cylinders in 𝐂\mathbf{C}, the imaginary part of vv can be seen to define a typical cylinder degeneration.

Theorem 2.13.

Suppose that 𝐂\mathbf{C} is a generic equivalence class of cylinders on a surface (X,ω)(X,\omega) in an invariant subvariety \mathcal{M}. Then there is a typical cylinder degeneration vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) and for any such vv, dim(v)=dim()1\dim(\mathcal{M}_{v})=\dim(\mathcal{M})-1 and the cylinders in Colv(𝐂)\operatorname{Col}_{v}(\mathbf{C}) remain generic. Moreover, if 𝐂\mathbf{C} is involved with rel, then rank(v)=rank()\mathrm{rank}(\mathcal{M}_{v})=\mathrm{rank}(\mathcal{M}). Otherwise, rank(v)=rank()1\mathrm{rank}(\mathcal{M}_{v})=\mathrm{rank}(\mathcal{M})-1.

Proof.

Every claim except the final one is contained in Apisa-Wright [AWb, Lemmas 6.5, 11.2, and 11.4]. Suppose now that 𝐂\mathbf{C} is not involved with rel. This implies that the twist space of 𝐂\mathbf{C} is spanned by σ𝐂\sigma_{\mathbf{C}} (by Theorem 2.3). In particular, there is a saddle connection ss contained in 𝐂\mathbf{C} whose length goes to zero on Colv(X,ω)\operatorname{Col}_{v}(X,\omega). Since v\mathcal{M}_{v} has codimension one, every element of (T(X,ω))(T_{(X,\omega)}\mathcal{M})^{*} generated by a vanishing cycle is collinear to ss. Since 𝐂\mathbf{C} is not involved with rel, rank(v)rank()1\mathrm{rank}(\mathcal{M}_{v})\leq\mathrm{rank}(\mathcal{M})-1 by Apisa-Wright [AWb, Lemma 3.8]. Equality must hold by Apisa-Wright [AWb, Corollary 3.7]. ∎

To close this subsection, we discuss the way in which translation covers interact with the boundary. Recall that a translation cover f:(X,ω)(Y,η)f:(X,\omega)\operatorname{\rightarrow}(Y,\eta) is a holomorphic branched cover f:XYf:X\operatorname{\rightarrow}Y so that fη=ωf^{*}\eta=\omega.

Convention 2.14.

For translation covers the image of any marked point is a marked point and all branch points are marked.

The following result morally says that a translation cover can be “collapsed to a translation cover on the boundary”.

Lemma 2.15 (Lemma 2.2 in Apisa-Wright [AWd]).

Suppose that f:(X,ω)(Y,η)f:(X,\omega)\operatorname{\rightarrow}(Y,\eta) is a translation covering. Let 𝐂(X,ω)\mathbf{C}\subset(X,\omega) be a collection of parallel cylinders such that f1(f(𝐂¯))=𝐂¯f^{-1}(f(\overline{\mathbf{C}}))=\overline{\mathbf{C}} and 𝐂¯(X,ω)\overline{\mathbf{C}}\neq(X,\omega). Then there is a translation cover

Col𝐂(f):Col𝐂(X,ω)Colf(𝐂)(Y,η)\operatorname{Col}_{\mathbf{C}}(f):\operatorname{Col}_{\mathbf{C}}(X,\omega)\operatorname{\rightarrow}\operatorname{Col}_{f(\mathbf{C})}(Y,\eta)

of the same degree.

We now recall terminology that will be used when surfaces in the boundary of \mathcal{M} have multiple components.

Definition 2.16.

Suppose that \mathcal{M}^{\prime} is an invariant subvariety in a product of strata 1×n\mathcal{H}_{1}\times\ldots\mathcal{H}_{n}. \mathcal{M}^{\prime} is not prime if, after perhaps re-indexing, there is a constant 1k<n1\leq k<n, so that =′′×′′′\mathcal{M}^{\prime}=\mathcal{M}^{\prime\prime}\times\mathcal{M}^{\prime\prime\prime} where ′′\mathcal{M}^{\prime\prime} is an invariant subvariety in 1××k\mathcal{H}_{1}\times\ldots\times\mathcal{H}_{k} and ′′′\mathcal{M}^{\prime\prime\prime} is an invariant subvariety in k+1××n\mathcal{H}_{k+1}\times\ldots\times\mathcal{H}_{n}. By Chen-Wright [CW19, Lemma 7.10], \mathcal{M}^{\prime} has a unique prime decomposition, i.e. \mathcal{M}^{\prime} can be represented as a product of prime invariant subvarieties.

3. Basics about minimal homological dimension

Proof of Theorem 1.7:.

Suppose first that \mathcal{M} has minimal homological dimension. Let 𝐂\mathbf{C} be an equivalence class of cylinders on a surface (X,ω)(X,\omega) in \mathcal{M}. By applying Lemma 2.7 (4), we may suppose without loss of generality that (X,ω)(X,\omega) is cylindrically stable and that 𝐂\mathbf{C} is contained in an equivalence class 𝐂1\mathbf{C}_{1} of horizontal cylinders (applying the lemma may have caused 𝐂\mathbf{C} to become a proper subset of an equivalence class of cylinders). By Lemma 2.7 (2), the horizontal core curves of (X,ω)(X,\omega) span a subset of T(X,ω)()T_{(X,\omega)}(\mathcal{M})^{*} of dimension rank()\operatorname{rank}(\mathcal{M}). Since any rel vector evaluates to zero on these core curves, in fact the horizontal core curves on (X,ω)(X,\omega) span a subset of p(T(X,ω)())p(T_{(X,\omega)}(\mathcal{M}))^{*} of dimension rank()\operatorname{rank}(\mathcal{M}).

Let WW be the span of the horizontal core curves of (X,ω)(X,\omega) in H1(X)H_{1}(X). By definition of minimal homological dimension, dimWrank()\dim W\leq\mathrm{rank}(\mathcal{M}). Let ϕ:H1(X)p(T(X,ω))\phi:H_{1}(X)\operatorname{\rightarrow}p\left(T_{(X,\omega)}\mathcal{M}\right)^{*} be the linear map given by associating to each homology class its corresponding functional on cohomology. Since dimϕ(W)=rank()\dim\phi(W)=\mathrm{rank}(\mathcal{M}), ϕW\phi\restriction_{W} is an isomorphism onto its image. By [Wri15, Lemma 4.7] any two core curves of a cylinder in 𝐂\mathbf{C} define collinear elements of p(T(X,ω))p\left(T_{(X,\omega)}\mathcal{M}\right)^{*} and hence the core curves must be collinear in H1(X)H_{1}(X), in particular any two core curves of cylinders in 𝐂\mathbf{C} are homologous.

Now suppose that for every surface (Y,η)(Y,\eta) in \mathcal{M} and every equivalence class 𝐂\mathbf{C} of cylinders on (Y,η)(Y,\eta), the core curves of cylinders in 𝐂\mathbf{C} are homologous. Let (X,ω)(X,\omega) be a horizontally periodic surface in \mathcal{M}. Letting WW be the span of the horizontal cylinder core curves in H1(X)H_{1}(X), we want to show that dimWrank()\dim W\leq\mathrm{rank}(\mathcal{M}). By Poincare duality, it suffices to show that PD(W)\mathrm{PD}(W), the span of the Poincare duals of the horizontal core curves, has dimension at most rank()\mathrm{rank}(\mathcal{M}). If 𝐂\mathbf{C} is an equivalence class of horizontal cylinders and γ\gamma is the core curve of a cylinder in 𝐂\mathbf{C}, then its Poincare dual γ\gamma^{*} is collinear to σ𝐂\sigma_{\mathbf{C}} since all the cylinders in 𝐂\mathbf{C} have homologous core curves. This shows that PD(W)\mathrm{PD}(W) is contained in p(T(X,ω))p(T_{(X,\omega)}\mathcal{M}). Moreover, PD(W)\mathrm{PD}(W) is Lagrangian since WW is Lagrangian and so dimW=dimPD(W)rank()\dim W=\dim\mathrm{PD}(W)\leq\mathrm{rank}(\mathcal{M}) as desired. ∎

Corollary 3.1.

If \mathcal{M} has minimal homological dimension, then 𝐤()=\mathbf{k}(\mathcal{M})=\mathbb{Q}.

Proof.

Given an equivalence class of cylinders 𝐂\mathbf{C}, the ratio of lengths of core curves of cylinders in 𝐂\mathbf{C} is one since the core curves are all pairwise homologous. The claim now holds by Wright [Wri15, Theorem 7.1], which states that 𝐤()\mathbf{k}(\mathcal{M}) is the smallest field extension of \mathbb{Q} containing the ratios of circumferences of cylinders in 𝐂\mathbf{C}. ∎

Lemma 3.2.

Let \mathcal{M}^{\prime} be a component of the boundary of an invariant subvariety \mathcal{M} containing connected surfaces. If \mathcal{M} has minimal homological dimension, then so does \mathcal{M}^{\prime}.

Proof.

Let \mathcal{M}^{\prime} be a component of the boundary of \mathcal{M}. Let (Xn,ωn)(X_{n},\omega_{n}) be a sequence of surfaces in \mathcal{M} that converge to a connected surface (Y,η)(Y,\eta) in \mathcal{M}^{\prime}. By Chen-Wright [CW19, Proposition 2.5] (see also Mirzakhani-Wright [MW17, Proposition 2.6]), we may suppose without loss of generality that (Y,η)(Y,\eta) has dense orbit in \mathcal{M}^{\prime}.

Let (Z,ζ)(Z,\zeta) be any surface in \mathcal{M}^{\prime} and let 𝐃\mathbf{D} be an equivalence class of cylinders on it. By Theorem 1.7, we wish to show that the core curves of cylinders in 𝐃\mathbf{D} are pairwise homologous. The cylinders in 𝐃\mathbf{D} persist in a neighborhood UU of (Z,ζ)(Z,\zeta) in \mathcal{M}^{\prime}. Since (Y,η)(Y,\eta) has dense orbit in \mathcal{M}^{\prime} there is an element gg of GL(2,)\mathrm{GL}(2,\mathbb{R}) so that g(Y,η)Ug\cdot(Y,\eta)\in U. Let 𝐁\mathbf{B} denote the cylinders on (Y,η)(Y,\eta) equivalent to the ones in g1(𝐃)g^{-1}(\mathbf{D}) (notice that moving from (Z,ζ)(Z,\zeta) to g(Y,η)g\cdot(Y,\eta) could have created new cylinders equivalent to those in 𝐃\mathbf{D}). It suffices to show that the core curves of cylinders in 𝐁\mathbf{B} are pairwise homologous.

For sufficiently large nn, 𝐁\mathbf{B} corresponds to a collection of cylinders 𝐁n\mathbf{B}_{n} on (Xn,ωn)(X_{n},\omega_{n}) (by Theorem 2.9 (1)) and there is an isomorphism

f:T(Y,η)Ann(Vn)T(Xn,ωn)f^{*}:T_{(Y,\eta)}\mathcal{M}^{\prime}\operatorname{\rightarrow}\mathrm{Ann}(V_{n})\cap T_{(X_{n},\omega_{n})}\mathcal{M}

where ff is the collapse map, the isomorphism is the one in Theorem 2.8, and VnV_{n} is the collection of vanishing cycles on (Xn,ωn)(X_{n},\omega_{n}). Fix such a sufficiently large nn and suppose that the cylinders in 𝐁n\mathbf{B}_{n} belong to \mathcal{M}-equivalence classes 𝐂1,,𝐂m\mathbf{C}_{1},\ldots,\mathbf{C}_{m}. Let σ\sigma denote fσ𝐁f^{*}\sigma_{\mathbf{B}}. This element belongs to T(Xn,ωn)T_{(X_{n},\omega_{n})}\mathcal{M} by the cylinder deformation theorem and Theorem 2.9 (3).

Write σ=i=1mσi\sigma=\sum_{i=1}^{m}\sigma_{i} where σi=C𝐁n𝐂iaCγC\sigma_{i}=\sum_{C\in\mathbf{B}_{n}\cap\mathbf{C}_{i}}a_{C}\gamma_{C}^{*} where aCa_{C}\in\mathbb{C}. For iji\neq j, notice that 𝐂i\mathbf{C}_{i}^{\prime} and 𝐂j\mathbf{C}_{j}^{\prime} are disjoint since both collections of cylinders consists of cylinders with homologous core curves and since the cylinders in 𝐁n𝐂i\mathbf{B}_{n}\cap\mathbf{C}_{i} are disjoint from those in 𝐁n𝐂j\mathbf{B}_{n}\cap\mathbf{C}_{j}. By Lemma 2.5, it follows that σiT(Xn,ωn)\sigma_{i}\in T_{(X_{n},\omega_{n})}\mathcal{M} for all ii.

By Theorem 2.9 (3), σiAnn(Vn)\sigma_{i}\in\mathrm{Ann}(V_{n}) for all ii. Let 𝐀i\mathbf{A}_{i} be the cylinder homotopic to the cylinders in f(𝐁n𝐂i)f\left(\mathbf{B}_{n}\cap\mathbf{C}_{i}\right). Note that the cylinders in 𝐀i\mathbf{A}_{i} have homologous core curves since this is true of the cylinders in 𝐁n𝐂i\mathbf{B}_{n}\cap\mathbf{C}_{i}. By Theorem 2.9 (3), σ𝐀i=(f)1(σi)\sigma_{\mathbf{A}_{i}}=\left(f^{*}\right)^{-1}\left(\sigma_{i}\right) is an elements of T(Y,η)T_{(Y,\eta)}\mathcal{M}^{\prime}. By Theorem 2.3, for any ii, there is a nonzero constant aia_{i} so that σ𝐁aiσ𝐀i\sigma_{\mathbf{B}}-a_{i}\sigma_{\mathbf{A}_{i}} is zero in absolute cohomology. In particular, this implies that p(σ𝐀i)p(\sigma_{\mathbf{A}_{i}}) is collinear to p(σ𝐀j)p(\sigma_{\mathbf{A}_{j}}) for any ii and jj. Since the core curves of cylinders in 𝐀i\mathbf{A}_{i} are pairwise homologous, this shows that the core curves of cylinders in 𝐁\mathbf{B} are pairwise homologous as desired. ∎

For the following it will be useful to recall the notation for cylinder degenerations established in Definition 2.10.

Corollary 3.3.

Let 𝐂\mathbf{C} be an equivalence class of generic cylinders on (X,ω)(X,\omega) in an invariant subvariety \mathcal{M} of minimal homological dimension. Suppose that vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) defines a cylinder degeneration and that 𝐂¯(X,ω)\overline{\mathbf{C}}\neq(X,\omega). Then Colv(X,ω)\operatorname{Col}_{v}(X,\omega) is connected and v\mathcal{M}_{v} has minimal homological dimension.

Proof.

By Lemma 3.2 it suffices to show that Colv(X,ω)\operatorname{Col}_{v}(X,\omega) is connected. Suppose not in order to derive a contradiction. Since 𝐂¯(X,ω)\overline{\mathbf{C}}\neq(X,\omega), Smillie-Weiss [SW04, Corollary 6] implies that there is a cylinder DD in the complement of 𝐂\mathbf{C} that is disjoint from 𝐂¯\overline{\mathbf{C}}. Let 𝐃\mathbf{D} be its equivalence class. By the cylinder proportion theorem (Nguyen-Wright [NW14, Proposition 3.2]), 𝐂\mathbf{C} and 𝐃\mathbf{D} are disjoint.

By Apisa-Wright [AWb, Lemma 9.1], v\mathcal{M}_{v} is prime. By Chen-Wright [CW19, Theorem 1.3], since v\mathcal{M}_{v} is prime, any deformation of Colv(X,ω)\operatorname{Col}_{v}(X,\omega) that remains in v\mathcal{M}_{v} and changes the period of some absolute cycle on one component of Colv(X,ω)\operatorname{Col}_{v}(X,\omega) changes the periods of absolute cycles on every component of Colv(X,ω)\operatorname{Col}_{v}(X,\omega).

Since 𝐃\mathbf{D} is disjoint from 𝐂\mathbf{C}, it follows that σ𝐃\sigma_{\mathbf{D}} is an element of TColv(X,ω)vT_{\operatorname{Col}_{v}(X,\omega)}\mathcal{M}_{v} (for instance by Theorem 2.9 (3)). Notice that along the path Colv(X,ω)+tσ𝐃\operatorname{Col}_{v}(X,\omega)+t\sigma_{\mathbf{D}} for tt a small real number, the periods of absolute cycles change on the components of Colv(X,ω)\operatorname{Col}_{v}(X,\omega) that contain a cylinder from 𝐃\mathbf{D}. This shows that a cylinder from 𝐃\mathbf{D} persists on every component of Colv(X,ω)\operatorname{Col}_{v}(X,\omega).

However, since Colv(X,ω)\operatorname{Col}_{v}(X,\omega) has multiple components it is possible to find a simple closed curve on one component of Colv(X,ω)\operatorname{Col}_{v}(X,\omega) that intersects the core curve of a cylinder in 𝐃\mathbf{D} exactly once. This curve remains a simple closed curve on (X,ω)(X,\omega) and intersects the core curve of one cylinder in 𝐃\mathbf{D} exactly once, but does not intersect all the core curves of the cylinders in 𝐃\mathbf{D}. This contradicts Theorem 1.7, which states that all core curves of cylinders in 𝐃\mathbf{D} are homologous. ∎

4. Cylinder rigid subvarieties

In this section we introduce a family of invariant subvarieties that is stable under degeneration and that includes every invariant subvariety of rel zero that consists of connected surfaces.

Definition 4.1.

Suppose that \mathcal{M} is an invariant subvariety (possibly in a stratum of disconnected surfaces). A collection of cylinders 𝐂\mathbf{C} is called a subequivalence class if the cylinders in 𝐂\mathbf{C} are all \mathcal{M}-equivalent to each other and 𝐂\mathbf{C} is a minimal collection of cylinders so that σ𝐂\sigma_{\mathbf{C}} belongs to T(X,ω)T_{(X,\omega)}\mathcal{M}.

We will say that \mathcal{M} is a CR invariant subvariety, where CR stands for “cylinder rigid” if there are finite sets S1S_{1}\subseteq\mathbb{Q} and S2S_{2}\subseteq\mathbb{R} so that the following holds:

  1. (1)

    For each equivalence class 𝐂\mathbf{C} of cylinders on a surface (X,ω)(X,\omega) in \mathcal{M}, σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M}.

  2. (2)

    Subequivalent cylinders remain subequivalent as long as they persist.

  3. (3)

    The ratio of moduli (resp. circumferences) of subequivalent cylinders belongs to S1S_{1} (resp. S2S_{2}).

Note that (1) implies that every equivalence class on a surface in \mathcal{M} can be partitioned into subequivalence classes.

Note too that (1) is the statement of the cylinder deformation theorem. The reason we must include it as a condition is entirely because the cylinder deformation theorem is not known to hold when (X,ω)(X,\omega) is disconnected.

The following is entirely due to Mirzakhani-Wright [MW17].

Lemma 4.2.

If \mathcal{M} has rel zero and any surface in \mathcal{M} is connected, then \mathcal{M} is a CR invariant subvariety.

Proof.

For equivalent cylinders, (3) holds for moduli, by [MW17, Corollary 1.6] and, for circumferences, by the cylinder finiteness theorem [MW17, Theorem 1.4]. Since the ratio of heights of any pair of equivalent cylinders cannot be changed by deforming the surface, it follows that equivalence classes are subequivalence classes. Since equivalent cylinders remains equivalent as long as they persist (2) holds. Condition (1) is the cylinder deformation theorem of Wright [Wri15]. ∎

4.1. Preliminary Results

Lemma 4.3.

Let 𝐂\mathbf{C} be a subequivalence class of cylinders on a surface (X,ω)(X,\omega) in a CR subvariety \mathcal{M}. On any surface in \mathcal{M} where the cylinders in 𝐂\mathbf{C} persist, they remain a subequivalence class.

Proof.

Suppose that the claim fails and that (X,ω)(X^{\prime},\omega^{\prime}) is a surface where the cylinders in 𝐂\mathbf{C} are a subset of a larger subequivalence class 𝐂\mathbf{C}^{\prime}. By definition of subequivalence class, σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M} and σ𝐂T(X,ω)\sigma_{\mathbf{C}^{\prime}}\in T_{(X^{\prime},\omega^{\prime})}\mathcal{M}. But then the cylinders in 𝐂\mathbf{C} have their moduli change along the path (X,ω)+tσ𝐂(X^{\prime},\omega^{\prime})+t\sigma_{\mathbf{C}} whereas those in 𝐂𝐂\mathbf{C}^{\prime}-\mathbf{C} have constant moduli contradicting Definition 4.1 (2) and (3). ∎

The following argument is often described as an “overcollapsing argument” for reasons that will become clear.

Lemma 4.4.

Suppose that \mathcal{M} is a CR subvariety and that 𝐂1\mathbf{C}_{1} and 𝐂2\mathbf{C}_{2} are distinct subequivalence classes of cylinders that happen to be parallel on (X,ω)(X,\omega)\in\mathcal{M}. Then if one cylinder in 𝐂1\mathbf{C}_{1} shares a boundary saddle connection with a cylinder in 𝐂2\mathbf{C}_{2}, every cylinder in 𝐂1\mathbf{C}_{1} shares a boundary saddle connection with a cylinder in 𝐂2\mathbf{C}_{2}.

Proof.

Without loss of generality suppose that the cylinders in 𝐂1𝐂2\mathbf{C}_{1}\cup\mathbf{C}_{2} are horizontal. Suppose that C1C_{1} and C2C_{2} share a boundary saddle connection ss and suppose without loss of generality that ss lies on the bottom boundary of C2C_{2} and where Ci𝐂iC_{i}\in\mathbf{C}_{i}. Shear (X,ω)(X,\omega), i.e. apply an element of (1t01)\begin{pmatrix}1&t\\ 0&1\end{pmatrix} for some tt\in\mathbb{R}, to form a surface (X,ω)(X^{\prime},\omega^{\prime}) on which there are no vertical saddle connections and so that there is a singularity zz on the top boundary of C2C_{2} that lies directly vertically above an interior point of ss (i.e. the vertical separatrix traveling down from zz into C2C_{2} travels the height of C2C_{2} down from zz before arriving at an interior point of ss). Apply the standard dilation, i.e. travel in \mathcal{M} in the direction of iσ𝐂2-i\sigma_{\mathbf{C}_{2}}, until the heights of the cylinders in 𝐂2\mathbf{C}_{2} reach zero. At this point, the singularity zz has accumulated on the saddle connection ss. Continuing to travel in the direction of iσ𝐂2-i\sigma_{\mathbf{C}_{2}} (we can travel in this direction indefinitely while remaining in \mathcal{M} since (X,ω)(X^{\prime},\omega^{\prime}) had no vertical saddle connections) the point zz moves into C1C_{1} causing the height of C1C_{1} to decrease. By Definition 4.1 (3), the height of every cylinder in 𝐂1\mathbf{C}_{1} must decrease and so every cylinder in 𝐂1\mathbf{C}_{1} must have shared a boundary saddle connection with a cylinder in 𝐂2\mathbf{C}_{2}. ∎

Lemma 4.5.

Let UU be an open subset of an invariant subvariety \mathcal{M}. Suppose that (X,ω)U(X,\omega)\in U contains a collection of cylinders 𝐂\mathbf{C} that can be partitioned into subequivalence classes {𝐂i}i=1n\{\mathbf{C}_{i}\}_{i=1}^{n} satisfying Definition 4.1 (2) and (3) for all deformations remaining in UU. Then the following hold:

  1. (1)

    Any element of Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) can be expressed uniquely as a linear combination of {σ𝐂i}i=1n\{\sigma_{\mathbf{C}_{i}}\}_{i=1}^{n}.

  2. (2)

    The support of any element of Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) is a union of subequivalence classes of cylinders.

  3. (3)

    Two cylinders in 𝐂\mathbf{C} are subequivalent if and only if there is some ii so that both cylinders belong to 𝐂i\mathbf{C}_{i}.

Proof.

The second two claims follow immediately from the first, which we now prove. Suppose without loss of generality that the cylinders in 𝐂\mathbf{C} are horizontal. Since the real and imaginary parts of any element of Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) belong to Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) it suffices to prove the claim for purely imaginary elements.

By Definition 4.1 (2) and (3), the ratio of heights of any two subequivalent cylinders is locally constant in UU. In particular, this implies that if vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) is purely imaginary then it has the form

i=1naiC𝐂ihCγC=i=1naiσ𝐂i\sum_{i=1}^{n}a_{i}\sum_{C\in\mathbf{C}_{i}}h_{C}\gamma_{C}^{*}=\sum_{i=1}^{n}a_{i}\sigma_{\mathbf{C}_{i}}

where aia_{i} is purely imaginary and hCh_{C} (resp. γC\gamma_{C}^{*}) denotes the height (resp. intersection pairing with the core curve) of CC. The uniqueness is obvious. ∎

4.2. The boundary of a CR subvariety

Say that two \mathcal{M}-equivalent cylinders CC and CC^{\prime} on a surface in \mathcal{M} are weakly-subequivalent if there is a collection 𝐂\mathbf{C} of \mathcal{M}-equivalent cylinders containing CC and CC^{\prime} and so that Twist(𝐂,)\mathrm{Twist}\left(\mathbf{C},\mathcal{M}\right) is one-dimensional with the support of any nonzero element being 𝐂\mathbf{C}. It is clear that CC and CC^{\prime} remain weakly subequivalent along any path on which the cylinders in 𝐂\mathbf{C} persist. We will say that (X,ω)(X,\omega)\in\mathcal{M} is a CR point if the following hold:

  1. (1)

    Two cylinders are weakly subequivalent if and only if they are subequivalent.

  2. (2)

    Weakly subequivalent cylinders satisfy Definition 4.1 (3).

  3. (3)

    Definition 4.1 (1) holds.

Lemma 4.6.

Let UU be an open subset of an invariant subvariety \mathcal{M}. Definition 4.1 holds on UU if and only if every point in UU is a CR point.

Proof.

Suppose first that Definition 4.1 holds on UU. Then two cylinders are weakly subequivalent if and only if they are subequivalent by Lemma 4.5. The other conditions are immediate.

Suppose now that every point in UU is a CR point. We must only verify Definition 4.1 (2). It suffices to show that if (X,ω)U(X,\omega)\in U has two weakly subequivalent cylinders C1C_{1} and C2C_{2} that persist along a path γ\gamma (contained in UU) from (X,ω)(X,\omega) to (X,ω)(X^{\prime},\omega^{\prime}), then C1C_{1} and C2C_{2} remain weakly subequivalent on (X,ω)(X^{\prime},\omega^{\prime})

Let 𝐂\mathbf{C} be the collection of cylinders on (X,ω)(X,\omega) containing C1C_{1} and C2C_{2} and so that Twist(𝐂,)\mathrm{Twist}\left(\mathbf{C},\mathcal{M}\right) is one-dimensional with the support of any nonzero element being 𝐂\mathbf{C}. It suffices to show that the cylinders in 𝐂\mathbf{C} persist along γ\gamma.

As long as 𝐂\mathbf{C} persists, the cylinders in it are pairwise weakly subequivalent and hence the ratio of moduli (resp. circumferences) of any two cylinders in 𝐂\mathbf{C} is contained in the finite set S1S_{1} (resp. S2S_{2}). Since C1C_{1} persists along γ\gamma its modulus and circumference are bounded above and away from zero along γ\gamma. The same thus holds for the cylinders in 𝐂\mathbf{C} as long as they persist along γ\gamma. In other words, as long as the cylinders in 𝐂\mathbf{C} persist along γ\gamma they have moduli and circumference bounded away from zero and bounded above. But this just means that the cylinders in 𝐂\mathbf{C} persist along γ\gamma as desired. ∎

Lemma 4.7.

Let UU be an open subset of an invariant subvariety \mathcal{M}. If every point in UU is a CR point, then the limit of any convergent sequence of points in UU is a CR point.

Proof.

Let (Xn,ωn)(X_{n},\omega_{n}) be a sequence of points in UU converging to (X,ω)(X,\omega). If (X,ω)(X,\omega) belongs to a component of the boundary, call this component \mathcal{M}^{\prime}, otherwise, set :=\mathcal{M}^{\prime}:=\mathcal{M}.

The result will follow from the following three sublemmas. Each proof will begin in the same way. We will take a collection of cylinders 𝐂\mathbf{C} on (X,ω)(X,\omega). By Theorem 2.9 (1) and (3), after perhaps passing to a subsequence, we may find cylinders 𝐂n\mathbf{C}_{n} on (Xn,ωn)(X_{n},\omega_{n}) that correspond to those in 𝐂\mathbf{C} and so that this correspondence induces an isomorphism between Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}^{\prime}) and Twist(𝐂n,)\mathrm{Twist}(\mathbf{C}_{n},\mathcal{M}). To avoid repeating this setup three times, we state it now once. But bear in mind that the cylinders in 𝐂\mathbf{C} will differ between the following three arguments.

Sublemma 4.8.

If 𝐂\mathbf{C} is an equivalence class then σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M}^{\prime}.

Proof.

Let 𝐂n\mathbf{C}_{n}^{\prime} be the union of all cylinders on (Xn,ωn)(X_{n},\omega_{n}) that are subequivalent to those in 𝐂n\mathbf{C}_{n}. Since the cylinders in 𝐂n\mathbf{C}_{n} have heights and circumferences that converge the same must hold for the cylinders in 𝐂n\mathbf{C}_{n}^{\prime} after passing to a subsequence (by Definition 4.1 (3)). Therefore, after passing to a subsequence, we may assume that each cylinder in 𝐂n\mathbf{C}_{n}^{\prime} converges to one on (X,ω)(X,\omega) (by Theorem 2.9 (2)). The limiting cylinder is necessarily equivalent to one in 𝐂\mathbf{C}, so this shows that, for sufficiently large nn, 𝐂n=𝐂n\mathbf{C}_{n}=\mathbf{C}_{n}^{\prime}, i.e. that 𝐂n\mathbf{C}_{n} is a union of subequivalence classes, and hence that σ𝐂nT(Xn,ωn)\sigma_{\mathbf{C}_{n}}\in T_{(X_{n},\omega_{n})}\mathcal{M}. By Theorem 2.9 (3), σ𝐂n\sigma_{\mathbf{C}_{n}} corresponds to an element of T(X,ω)T_{(X,\omega)}\mathcal{M}^{\prime} and these elements converge to σ𝐂\sigma_{\mathbf{C}}. Hence, σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M}. ∎

Sublemma 4.9.

If two cylinders C1C_{1} and C2C_{2} are weakly subequivalent on (X,ω)(X,\omega)\in\mathcal{M}^{\prime} then they are subequivalent and their ratio of moduli (resp. circumferences) belongs to S1S_{1} (resp. S2S_{2}).

Proof.

Let 𝐂\mathbf{C} be the collection of cylinders on (X,ω)(X,\omega) containing C1C_{1} and C2C_{2} and so that Twist(𝐂,)\mathrm{Twist}\left(\mathbf{C},\mathcal{M}\right) is one-dimensional with the support of any nonzero element being 𝐂\mathbf{C}. By Lemma 4.5 (2), 𝐂n\mathbf{C}_{n} is a subequivalence class of cylinders whose ratios of moduli (resp. circumferences) belong to S1S_{1} (resp. S2S_{2}). Since the cylinders in 𝐂n\mathbf{C}_{n} converge to those in 𝐂\mathbf{C} the result follows as in the previous sublemma. ∎

Sublemma 4.10.

If two cylinders C1C_{1} and C2C_{2} are subequivalent on (X,ω)(X,\omega)\in\mathcal{M}^{\prime} then they are weakly subequivalent.

Proof.

Let 𝐂\mathbf{C} be the collection of cylinders on (X,ω)(X,\omega) containing C1C_{1} and C2C_{2} so that σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M}. Since σ𝐂\sigma_{\mathbf{C}} is an element of Twist(𝐂n,)\mathrm{Twist}(\mathbf{C}_{n},\mathcal{M}) whose support is 𝐂n\mathbf{C}_{n}, 𝐂n\mathbf{C}_{n} is a union of subequivalence classes by Lemma 4.5 (2). After passing to a subsequence we may suppose that the partition of 𝐂n\mathbf{C}_{n} into subequivalence classes does not depend on nn (recall that we have an identification of the cylinders in 𝐂n\mathbf{C}_{n} with the cylinders in 𝐂\mathbf{C}). Since the cylinders in 𝐂n\mathbf{C}_{n} converge to 𝐂\mathbf{C}, we see that 𝐂\mathbf{C} is partitioned into the same number of subequivalence classes as 𝐂n\mathbf{C}_{n}. Since 𝐂\mathbf{C} is itself a subequivalence class the same must hold for 𝐂n\mathbf{C}_{n}. This shows that Twist(𝐂n,)\mathrm{Twist}(\mathbf{C}_{n},\mathcal{M}) is one-dimensional and spanned by σ𝐂n\sigma_{\mathbf{C}_{n}} by Lemma 4.5 (1). Since the cylinders in 𝐂n\mathbf{C}_{n} converge to 𝐂\mathbf{C}, Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) is one-dimensional and spanned by σ𝐂\sigma_{\mathbf{C}}, which shows that any two cylinders in 𝐂\mathbf{C} are weakly subequivalent. ∎

Corollary 4.11.

Suppose that UU is an open subset of a prime invariant subvariety \mathcal{M}. If each point in UU is a CR point then \mathcal{M} is a CR subvariety.

Proof.

Since \mathcal{M} is prime, the GL(2,)\mathrm{GL}(2,\mathbb{R}) action is ergodic on \mathcal{M} (by Chen-Wright [CW19, Corollary 7.4]). This implies that U:=gGL(2,)gUU^{\prime}:=\bigcup_{g\in\mathrm{GL}(2,\mathbb{R})}gU is open, dense, and that every point in it is a CR point. Since UU is open and dense in \mathcal{M}, every point in \mathcal{M} is a CR point (by Lemma 4.7). Therefore, \mathcal{M} is a CR subvariety by Lemma 4.6. ∎

Proposition 4.12.

Suppose that \mathcal{M} is a CR subvariety whose elements are connected surfaces. If \mathcal{M}^{\prime} is a component of the boundary of \mathcal{M}, then it is a CR subvariety.

The requirement that the surfaces in \mathcal{M} are connected is present solely because it is required to apply the boundary theory developed in Mirzakhani-Wright [MW17] and Chen-Wright [CW19].

Proof.

By Chen-Wright [CW19, Proposition 2.5] (see also Mirzakhani-Wright [MW17, Proposition 2.6]), there is an open subset UU\subseteq\mathcal{M}^{\prime} consisting of limits of sequences of surfaces in \mathcal{M}. By Lemma 4.7, every point in UU is a CR point. Let =1××k\mathcal{M}^{\prime}=\mathcal{M}_{1}\times\ldots\times\mathcal{M}_{k} be the prime decomposition of \mathcal{M}^{\prime} (see Definition 2.16). Since i\mathcal{M}_{i} is prime and since every point in the projection of UU to i\mathcal{M}_{i} is a CR point, i\mathcal{M}_{i} is a CR subvariety by Corollary 4.11. Since no cylinders on a surface in i\mathcal{M}_{i} can be equivalent or subequivalent to cylinders on a surface in j\mathcal{M}_{j} if iji\neq j, it follows that \mathcal{M} itself is a CR subvariety. ∎

5. The base case of the proof of Theorem 1.5

This section is dedicated to the proof of the following.

Proposition 5.1.

If \mathcal{M} is a rank two rel zero invariant subvariety of minimal homological dimension, then \mathcal{M} is geminal.

The general definition of “geminal” appears in Definition 6.7, but when \mathcal{M} has rel zero, it suffices to show that every equivalence class of cylinders consists of isometric cylinders and has at most two elements. To this end, suppose that 𝐂1\mathbf{C}_{1} is an equivalence class of cylinders on a surface (X,ω)(X,\omega) in \mathcal{M}.

Without loss of generality suppose that the cylinders in 𝐂1\mathbf{C}_{1} are horizontal. By perturbing, we may suppose moreover that (X,ω)(X,\omega) is cylindrically stable (by Theorem 2.7 (3) and Corollary 3.1). We will perturb so that if two cylinders in 𝐂1\mathbf{C}_{1} are not isometric before perturbing they are not isometric after perturbing. Note that after perturbing 𝐂1\mathbf{C}_{1} remains an equivalence class, and not just a subset of one (by Lemmas 4.2 and 4.3).

By Lemma 2.7 (1) there is exactly one other equivalence class 𝐂2\mathbf{C}_{2} of horizontal cylinders. In particular, there is a cylinder in 𝐂1\mathbf{C}_{1} that shares a boundary saddle connection with a cylinder in 𝐂2\mathbf{C}_{2}.

Lemma 5.2.

There are at most two cylinders in 𝐂1\mathbf{C}_{1}. If there are two, then the top boundary of one coincides with the bottom boundary of the other.

Proof.

Let nn be the number of cylinders in 𝐂1\mathbf{C}_{1}. We will show that n=2n=2. Since \mathcal{M} has minimal homological dimension, fixing i{1,2}i\in\{1,2\}, any two cylinders in 𝐂i\mathbf{C}_{i} have core curves that are homologous to each other (by Theorem 1.7). Cutting the core curves of the cylinders in 𝐂1\mathbf{C}_{1} creates n1n-1 subsurfaces, each of which has two boundary components - each one corresponding to a core curve of a cylinder in 𝐂1\mathbf{C}_{1}. Since the core curves of cylinders in 𝐂2\mathbf{C}_{2} are all homologous to each other (and not homologous to the core curve of any cylinder in 𝐂1\mathbf{C}_{1}), the cylinders in 𝐂2\mathbf{C}_{2} belong to exactly one of these subsurfaces and hence there are at most two cylinders in 𝐂1\mathbf{C}_{1} which can share a boundary saddle connection with a cylinder in 𝐂2\mathbf{C}_{2}. By Lemma 4.4, every cylinder in 𝐂1\mathbf{C}_{1} shares a boundary saddle connection with a cylinder in 𝐂2\mathbf{C}_{2}, so there are at most two cylinders in 𝐂1\mathbf{C}_{1}.

Since the cylinders in 𝐂2\mathbf{C}_{2} are contained in exactly one subsurface of (X,ω)𝐂1¯(X,\omega)-\overline{\mathbf{C}_{1}}, it follows that if there are two cylinders in 𝐂1\mathbf{C}_{1} the top boundary of one must coincide with the bottom boundary of the other. ∎

Since there is nothing more to prove when 𝐂1\mathbf{C}_{1} consists of a single cylinder, we suppose that 𝐂1\mathbf{C}_{1} consists of two cylinders, which we call CC and CC^{\prime}.

To conclude the proof of Proposition 5.1, it suffices to show that the cylinders in 𝐂1\mathbf{C}_{1} are isometric. Since \mathcal{M} has minimal homological dimension, the core curves of cylinders in 𝐂1\mathbf{C}_{1} are homologous (by Theorem 1.7) and hence have equal length. So it suffices to show that the cylinders in 𝐂1\mathbf{C}_{1} have equal heights.

Since the cylinders in 𝐂2\mathbf{C}_{2} are not generically parallel to those in 𝐂1\mathbf{C}_{1}, there is a surface (X,ω)(X^{\prime},\omega^{\prime}) that is arbitrarily close to (X,ω)(X,\omega) on which the cylinders in 𝐂1\mathbf{C}_{1} remain horizontal, the cylinders in 𝐂2\mathbf{C}_{2} are not, and the cylinders in 𝐂2\mathbf{C}_{2} are generic. We will assume that this perturbation was performed so that if CC and CC^{\prime} had unequal height before the perturbation they did so after as well. As before, 𝐂1\mathbf{C}_{1} and 𝐂2\mathbf{C}_{2} remain equivalence classes, and not just subsets of one (by Lemmas 4.2 and 4.3). By applying the matrix (1t01)\begin{pmatrix}1&t\\ 0&1\end{pmatrix} we will suppose that 𝐂2\mathbf{C}_{2} is vertical on (X,ω)(X^{\prime},\omega^{\prime}). After applying the standard shear in 𝐂2\mathbf{C}_{2} (which is possible by the cylinder deformation theorem) we may also suppose that, on (X,ω)(X^{\prime},\omega^{\prime}), there are cylinders in 𝐂2\mathbf{C}_{2} that contain horizontal saddle connections. By [Api20, Lemma 9.1], (X,ω)(X^{\prime},\omega^{\prime}) is horizontally periodic and not covered by the cylinders in 𝐂1\mathbf{C}_{1} since these cylinders do not intersect 𝐂2\mathbf{C}_{2}. Let 𝐂3\mathbf{C}_{3} be the equivalence class of the horizontal cylinders that intersect 𝐂2\mathbf{C}_{2}. Since equivalent cylinders are homologous (by Theorem 1.7) and since the cylinders in 𝐂1\mathbf{C}_{1} do not intersect those in 𝐂2\mathbf{C}_{2}, we have that 𝐂3𝐂1\mathbf{C}_{3}\neq\mathbf{C}_{1}. 𝐂1\mathbf{C}_{1} and 𝐂3\mathbf{C}_{3} are the only two equivalence classes of horizontal cylinders on (X,ω)(X^{\prime},\omega^{\prime}) (by Lemma 2.7 (1)).

Lemma 5.3.

Col𝐂2(X,ω)\operatorname{Col}_{\mathbf{C}_{2}}(X^{\prime},\omega^{\prime}) is connected and the core curves of cylinders in Col𝐂2(𝐂1𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}\cup\mathbf{C}_{3}) are all homologous. Moreover, Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) and Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3}) are subequivalence classes of cylinders.

Proof.

The first claim follow from Corollary 3.3, which also implies that 𝐂2\mathcal{M}_{\mathbf{C}_{2}} has minimal homological dimension. Since \mathcal{M} has rank two rel zero, 𝐂2\mathcal{M}_{\mathbf{C}_{2}} must have rank one and hence if two cylinders are parallel on a surface in 𝐂2\mathcal{M}_{\mathbf{C}_{2}} they are 𝐂2\mathcal{M}_{\mathbf{C}_{2}}-equivalent. Since the cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) and Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3}) are parallel they must be 𝐂2\mathcal{M}_{\mathbf{C}_{2}}-equivalent and hence the second claim follows by Theorem 1.7. The third claim follows from Theorem 2.9 (3). ∎

Our strategy will be to overcollapse the cylinders in Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3}) as in the proof of Lemma 4.4 and to conclude that the heights of each cylinder in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) change at the same rate under this deformation, which will imply that they have equal height.

Remark 5.4.

The results in Lemma 5.3 are the reason we pass to the boundary. If we were to attempt an overcollapsing argument without degenerating it would be hard to control how the heights of the cylinders in 𝐂1\mathbf{C}_{1} change. However, the extra information that all four cylinders in Col𝐂2(𝐂1𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}\left(\mathbf{C}_{1}\cup\mathbf{C}_{3}\right) are homologous makes it easy to compute the change in heights of the cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) after overcollapsing.

Begin by shearing Col𝐂2(X,ω)\operatorname{Col}_{\mathbf{C}_{2}}(X^{\prime},\omega^{\prime}) so that there are no vertical saddle connections. Let (Y,η)(Y,\eta) denote the resulting surface.

To fix notation, suppose that DD is a cylinder of height hh in Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3}) on (Y,η)(Y,\eta). If there is a second cylinder in Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3}) we call it DD^{\prime} and denote its height by hh^{\prime}. Now, as in the proof of Lemma 4.4, we will overcollapse Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3}) into Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}), that is, we will flow from (Y,η)(Y,\eta) in \mathcal{M} in the direction of iσCol𝐂2(𝐂3)-i\sigma_{\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3})} until the heights of the cylinders in Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3}) are zero. Then we will continue flowing in the direction of iσCol𝐂2(𝐂3)-i\sigma_{\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3})}.

To be concrete, we will let (Yt,ηt):=(Y,η)(1t)iσCol𝐂2(𝐂3)(Y_{t},\eta_{t}):=(Y,\eta)-(1-t)i\sigma_{\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3})}. Since there are no vertical saddle connections on (Y,η)(Y,\eta) this surface is defined for all real tt.

Lemma 5.5.

The derivatives, with respect to tt, of the heights of the cylinders of Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) on (Yt,ηt)(Y_{t},\eta_{t}) for t(ϵ,0)t\in(-\epsilon,0) are equal for any sufficiently small ϵ\epsilon.

Proof.

Suppose without loss of generality that Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) borders DD along its top boundary. On (Y0,η0)(Y_{0},\eta_{0}) new singularities have accumulated on the top boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C). Intuitively, these singularities “came from Col𝐂2(𝐂3)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3})”. However, since the bottom boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) coincides with the top boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C^{\prime}), no new singularities have accumulated there.

Triangulate Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) by saddle connections on (Y0,η0)(Y_{0},\eta_{0}) using all the saddle connections on the boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) as edges of the triangulation and then adding in additional saddle connections, the set of which we call SS, that join one boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) to the other. Extend the triangulation to a triangulation TT by saddle connections of (Y0,η0)(Y_{0},\eta_{0}). There is an open subset UU of the stratum containing (Y0,η0)(Y_{0},\eta_{0}) on which the cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) persist and so that TT remains a triangulation by saddle connections for every surface in UU. Select ϵ\epsilon so that (Yt,ηt)(Y_{t},\eta_{t}) belongs to UU for all t(ϵ,+ϵ)t\in(-\epsilon,+\epsilon). In particular, for these values of tt, the saddle connections in SS remain saddle connections and the height of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) on (Yt,ηt)(Y_{t},\eta_{t}) for t(ϵ,ϵ)t\in(-\epsilon,\epsilon) is given by minsS(ηt(s))\min_{s\in S}\left(\eta_{t}(s)\right) (this uses the fact that, along this path, no new singularities accumulate on the bottom boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C)).

Sublemma 5.6.

For t(0,ϵ)t\in(0,\epsilon), each saddle connection in SS connects a point on the bottom boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) to one of the following: a point in the top boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C), a point in the top boundary of DD, and (provided that DD^{\prime} exists) a point in the top boundary of DD^{\prime}. The derivatives of the imaginary parts of the periods of saddle connections in SS with respect to tt are, respectively, 0, h-h, and (h+h)-(h+h^{\prime}).

Proof.

The trichotomy is obvious. Since periods vary linearly with tt along the path, it suffices to show that, on (Yt,ηt)(Y_{t},\eta_{t}) for t(0,ϵ)t\in(0,\epsilon), any saddle connection in SS crosses each horizontal cylinder at most once.

Suppose to a contradiction that a saddle connection sSs\in S crosses a horizontal cylinder on (Y,η)(Y,\eta) more than once. By adding part of the core curve of that cylinder to ss it is possible to form a simple closed curve that has positive intersection number with some horizontal cylinders, but not with Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C^{\prime}), into which ss does not cross. This contradicts the fact that the four horizontal cylinders on (Yt,ηt)(Y_{t},\eta_{t}), for t(0,ϵ)t\in(0,\epsilon), have homologous core curves (by Lemma 5.3). ∎

When Col𝐂2(𝐂3)={D}\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3})=\{D\} for t(ϵ,0)t\in(-\epsilon,0) the derivatives of the heights of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) and Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C^{\prime}) are both equal to h-h. This follows since, because new singularities have accumulated on the top boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C), one of the saddle connections in SS joins a zero on the bottom boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) to a zero on the top boundary of DD on (Yt,ηt)(Y_{t},\eta_{t}) for t(0,ϵ)t\in(0,\epsilon). Similarly, when Col𝐂2(𝐂3)={D,D}\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{3})=\{D,D^{\prime}\}, by construction, there is a singularity from the top boundary of DD^{\prime} that accumulates on the boundary of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C). As before, this shows that the derivative of the height of Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C) for t(ϵ,0)t\in(-\epsilon,0) is (h+h)-(h+h^{\prime}). By symmetry of hypotheses the same holds for Col𝐂2(C)\operatorname{Col}_{\mathbf{C}_{2}}(C^{\prime}). ∎

By Proposition 4.12, since the cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) are subequivalent on (Y,η)(Y,\eta) and persist on (Yt,ηt)(Y_{t},\eta_{t}) for all t(ϵ,1]t\in(-\epsilon,1], it follows that the ratio of moduli of cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) is constant for all tt. By Lemma 5.5 this ratio must be one. Since the ratio of heights of cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) is the same as the ratio of moduli (since the cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) have homologous core curves) it follows that heights of the cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) are equal on (Y,η)(Y,\eta). Since the heights of the cylinders in Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) on (Y,η)(Y,\eta) are the same as the heights of the cylinders in 𝐂1\mathbf{C}_{1}, the cylinders in 𝐂1\mathbf{C}_{1} have identical heights, as desired.

6. Preliminaries on geminal varieties

In this section we will assemble various results and establish simple consequences of them that we will require for the proof of Theorem 1.5.

6.1. Minimal covers

One of the most important objects in the sequel will be the minimal cover associated to a translation surface. This cover is defined by the following result, which is a combination of a result of Möller [Möl06, Theorem 2.6] and an extension found in [AWc, Lemma 3.3].

Theorem 6.1.

Suppose that (X,ω)(X,\omega) is not a torus cover. There is a unique translation surface (Xmin,ωmin)(X_{min},\omega_{min}) and a translation covering

πXmin:(X,ω)(Xmin,ωmin)\pi_{X_{min}}:(X,\omega)\rightarrow(X_{min},\omega_{min})

such that any translation cover from (X,ω)(X,\omega) to a translation surface is a factor of πXmin\pi_{X_{min}}.

Additionally, there is a quadratic differential (Qmin,qmin)(Q_{min},q_{min}) with a degree 1 or 2 map (Xmin,ωmin)(Qmin,qmin)(X_{min},\omega_{min})\rightarrow(Q_{min},q_{min}) such that any map from (X,ω)(X,\omega) to a quadratic differential is a factor of the composite map πQmin:(X,ω)(Qmin,qmin)\pi_{Q_{min}}:(X,\omega)\rightarrow(Q_{min},q_{min}).

6.2. Marked points

We begin with the following two definitions.

Definition 6.2.

Given a translation surface (X,ω)(X,\omega) with marked points let (X,ω)\operatorname{\mathcal{F}}(X,\omega) be the surface with the marked points forgotten. If \mathcal{M} is the orbit closure of (X,ω)(X,\omega), then ()\operatorname{\mathcal{F}}(\mathcal{M}) will denote the orbit closure of (X,ω)\operatorname{\mathcal{F}}(X,\omega).

Definition 6.3.

Let (X,ω)(X,\omega) be a surface with dense orbit in an invariant subvariety \mathcal{M}. Given a finite collection of points PP on (X,ω)(X,\omega) we will let (X,ω;P)(X,\omega;P) denote the result of marking the points PP on (X,ω)(X,\omega). The points PP are said to be generic if the following occurs

dimGL(2,)(X,ω;P)¯=|P|+dim.\dim\overline{\mathrm{GL}(2,\mathbb{R})\cdot(X,\omega;P)}=|P|+\dim\mathcal{M}.

A point pp on (X,ω)(X,\omega) is said to be periodic if pp is not a zero of ω\omega and

dimGL(2,)(X,ω;{p})¯=dim.\dim\overline{\mathrm{GL}(2,\mathbb{R})\cdot(X,\omega;\{p\})}=\dim\mathcal{M}.

Finally, if QQ denotes the collection of marked points on (X,ω)(X,\omega) then a point qQq\in Q is said to be free if it can be moved around the surface while remaining in \mathcal{M} and while fixing the position of all other marked points and the underlying unmarked surface.

Theorem 6.4 (Apisa [Api20]).

If (X,ω)(X,\omega) is a translation surface of genus at least two so that (X,ω)\operatorname{\mathcal{F}}(X,\omega) has dense orbit in a non-hyperelliptic component of a stratum, then any collection of points on (X,ω)(X,\omega) that does not include zeros of ω\omega is generic.

The following result is an immediate consequence of Apisa-Wright [AWc].

Theorem 6.5.

Let (X,ω)(X,\omega) be a translation surface of genus at least two with marked points QQ and so that (X,ω)\operatorname{\mathcal{F}}(X,\omega) has dense orbit in a hyperelliptic locus. Let \mathcal{M} be the orbit closure of (X,ω;Q)(X,\omega;Q). The marked points on a surface in \mathcal{M} consist of free points, pairs of points exchanged by the hyperelliptic involution, fixed points of the hyperelliptic involution, and zeros of ω\omega, with no further constraints on the points.

Proof.

Every hyperelliptic locus is a locus of holonomy double covers of a stratum 𝒬\mathcal{Q} of genus zero quadratic differentials. The rank of 𝒬\mathcal{Q} is the same as the genus of XX, so in our case, the rank of 𝒬\mathcal{Q} is at least two. By Apisa-Wright [AWc, Theorem 1.4], there are no periodic points on a surface with dense orbit in 𝒬\mathcal{Q}; this uses that 𝒬\mathcal{Q} has rank at least two and the fact that a stratum of genus zero quadratic differentials never contains a hyperelliptic connected component. By Apisa-Wright [AWc, Lemma 4.5], the quotient of (X,ω)(X,\omega) by the hyperelliptic involution is πQmin\pi_{Q_{min}}. The lemma now follows from Apisa-Wright [AWc, Theorem 1.3]. ∎

Corollary 6.6.

If \mathcal{M} is a hyperelliptic locus of translation surfaces of genus at least two, then any generic cylinder on any surface in \mathcal{M} is simple or half-simple.

Proof.

Suppose that pp is a marked point that is neither a zero nor a fixed point of the hyperelliptic involution. By Theorem 6.5, if pp appears on the boundary of a generic cylinder CC then there is a saddle connection joining pp to itself that comprises one boundary of CC (if not then it would be possible to move pp so the saddle connection with one endpoint at pp in the boundary of CC ceases to be parallel to the core curve of CC). It therefore suffices to show that if (X,ω)(X,\omega) only has fixed points of the hyperelliptic involution marked then the generic cylinders are simple or half-simple. In this case, \mathcal{M} is a quadratic double and the result follows from Apisa-Wright [AWb, Lemma 12.4]. ∎

6.3. Geminal varieties

In this subsection we will present a class of invariant subvarieties that were originally studied in Apisa-Wright [AWa].

Definition 6.7.

An invariant subvariety \mathcal{M} is said to be geminal if for any cylinder CC on any (X,ω)(X,\omega)\in\mathcal{M}, either

  • any cylinder deformation of CC remains in \mathcal{M}, or

  • there is a cylinder CC^{\prime} such that CC and CC^{\prime} are parallel and have the same height and circumference on (X,ω)(X,\omega) as well as on all small deformations of (X,ω)(X,\omega) in \mathcal{M}, and any cylinder deformation that deforms CC and CC^{\prime} equally remains in \mathcal{M}.

In the first case we say that CC is free, and in the second case we say that CC and CC^{\prime} are twins. \mathcal{M} is called hh-geminal if additionally twin cylinders have homologous core curves. The partition of an equivalence class of cylinders into free cylinders and pairs of twins is called a geminal partition

The simplest example of a geminal invariant subvariety, other than a component of a stratum, is a quadratic double, i.e. a full locus of holonomy double covers where the collection of marked points is fixed by the holonomy involution and otherwise unconstrained. Before proceeding we establish the following useful corollary of the results of the previous subsection.

Corollary 6.8.

Let 𝐂\mathbf{C} be an equivalence class of generic cylinders on a surface (X,ω)(X,\omega) in a hyperelliptic locus \mathcal{M}. If 𝐂\mathbf{C} does not admit a geminal partition, then there is a cylinder in 𝐂\mathbf{C} with a free marked point on its boundary.

Proof.

Without loss of generality, suppose that the only marked points on (X,ω)(X,\omega) lie on the boundary of cylinders in 𝐂\mathbf{C}. If all the marked points were fixed by the hyperelliptic involution, then \mathcal{M} would be a quadratic double and hence geminal. Therefore, not all the marked points are fixed by the hyperelliptic involution and so one of them must be free by Theorem 6.5

To state the strongest possible result on geminal subvarieties we recall the following definitions.

Definition 6.9.

Let (X,ω)(X,\omega) be a translation surface. A translation cover f:(X,ω)(X,ω)f:(X,\omega)\rightarrow(X^{\prime},\omega^{\prime}) will be called good if every cylinder CC on (X,ω)(X,\omega) is the preimage of its image under ff. The cover will be called optimal if it is good and any other good map is a factor of it.

If additionally (X,ω)(X,\omega) belongs to an invariant subvariety \mathcal{M}, we will say that ff is \mathcal{M}-generic if the map ff can be deformed to every nearby surface in \mathcal{M}. A map ff defined on (X,ω)(X,\omega) will be called \mathcal{M}-good if it is \mathcal{M}-generic and the deformations of the map are good on all deformations of (X,ω)(X,\omega) in \mathcal{M}. The map ff will be called \mathcal{M}-optimal if it is \mathcal{M}-good and any other \mathcal{M}-good map is a factor of it.

Finally, if (X,ω)(X,\omega) is a torus cover we will let πabs\pi_{abs} denote the minimal degree map to the torus.

Remark 6.10.

If (X,ω)(X,\omega) has dense orbit in an invariant subvariety of rank at least two, then πXmin\pi_{X_{min}} is \mathcal{M}-generic. Given a path in \mathcal{M} from (X,ω)(X,\omega) to another surface (X,ω)(X^{\prime},\omega^{\prime}), πXmin\pi_{X_{min}} must become a translation cover on (X,ω)(X^{\prime},\omega^{\prime}). This cover is exactly πXmin\pi_{X^{\prime}_{min}} when (X,ω)(X^{\prime},\omega^{\prime}) has dense orbit. This observation will allow us to make statements about πXmin\pi_{X_{min}} and then prove them even after perturbing to a nearby surface.

The following result is Apisa-Wright [AWa, Lemma 6.14]. Note that the statement of Theorem 6.11 (2) is slightly stronger than what is stated there, but that it follows from the proof.

Theorem 6.11.

Suppose that the orbit closure of (X,ω)(X,\omega) is a rank one subvariety \mathcal{M} of minimal homological dimension.

  1. (1)

    The minimal degree map πabs\pi_{abs} from (X,ω)(X,\omega) to a torus is the optimal map.

  2. (2)

    For any collection of cylinders 𝐂\mathbf{C} on (X,ω)(X,\omega) so that σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M}, Col𝐂(πabs)\operatorname{Col}_{\mathbf{C}}(\pi_{abs}) is the optimal map for the connected surface Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega).

The following result is mostly contained in Apisa-Wright [AWa, Proposition 8.1].

Theorem 6.12.

Suppose that \mathcal{M} is an hh-geminal invariant subvariety of rank at least two.

  1. (1)

    Every surface in \mathcal{M} has an \mathcal{M}-optimal map πopt\pi_{opt}, which coincides with πXmin\pi_{X_{min}} for any surface with dense orbit in \mathcal{M}.

  2. (2)

    \mathcal{M} is either a stratum of Abelian differentials or a full locus of covers of a quadratic double of a genus zero stratum.

  3. (3)

    If the degree of the optimal map is greater than one, then every cylinder has a twin.

  4. (4)

    If 𝐂\mathbf{C} is a collection of generic equivalent cylinders on a surface (X,ω)(X,\omega) in \mathcal{M} such that σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M} and so that 𝐂\mathcal{M}_{\mathbf{C}} has dimension exactly one less than that of \mathcal{M}, then Col𝐂(πopt)\operatorname{Col}_{\mathbf{C}}(\pi_{opt}) is the 𝐂\mathcal{M}_{\mathbf{C}}-optimal map for Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega).

Proof.

Noting that the only Abelian or quadratic doubles that are hh-geminal are quadratic doubles of genus zero strata, the only item that is not immediately implied by Apisa-Wright [AWa, Proposition 8.1] is (4). Suppose without loss of generality that 𝐂\mathbf{C} is horizontal.

We begin by noting that, since σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M}, 𝐂\mathbf{C} can be partitioned into free cylinders and twins, i.e. subequivalence classes, which we denote by 𝐂1,,𝐂n\mathbf{C}_{1},\ldots,\mathbf{C}_{n}. Moreover,

Col𝐂(X,ω)=Col𝐂σ(1)Col𝐂σ(n)(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega)=\operatorname{Col}_{\mathbf{C}_{\sigma(1)}}\ldots\operatorname{Col}_{\mathbf{C}_{\sigma(n)}}(X,\omega)

for any permutation σSym(n)\sigma\in\mathrm{Sym}(n). Since, by assumption, 𝐂\mathcal{M}_{\mathbf{C}} has codimension one, there is a unique subequivalence class, which is 𝐂1\mathbf{C}_{1} up to re-indexing, that contains a vertical saddle connection. By Apisa-Wright [AWa, Proposition 8.1], Col𝐂1(πopt)\operatorname{Col}_{\mathbf{C}_{1}}(\pi_{opt}) is the 𝐂1\mathcal{M}_{\mathbf{C}_{1}}-optimal map. Since none of the subequivalence classes 𝐂2,,𝐂n\mathbf{C}_{2},\ldots,\mathbf{C}_{n} contain vertical saddle connections, applying Col𝐂i\operatorname{Col}_{\mathbf{C}_{i}} for i>1i>1 does not pass to the boundary of 𝐂1\mathcal{M}_{\mathbf{C}_{1}}, so Col𝐂(πopt)\operatorname{Col}_{\mathbf{C}}(\pi_{opt}) is the 𝐂\mathcal{M}_{\mathbf{C}}-optimal map for Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega). ∎

Recall that if (X,ω)(X,\omega) is hyperelliptic then a Weierstrass point is a fixed point of the hyperelliptic involution. A Weierstrass point is said to be regular if it is not a zero of ω\omega.

Corollary 6.13.

If \mathcal{M} is hh-geminal, rank at least two, and the \mathcal{M}-optimal map πopt\pi_{opt} is not the identity, then all but perhaps one of the regular Weierstrass points are branch points of πopt\pi_{opt}.

Proof.

Let (X,ω)(X,\omega)\in\mathcal{M}. If πopt\pi_{opt} is not the identity, then every cylinder on πopt(X,ω)\pi_{opt}(X,\omega) has a twin (by Theorem 6.12 (3)) and hence πopt(X,ω)\pi_{opt}(X,\omega) belongs to a hyperelliptic locus (by Theorem 6.12 (2)) which we will denote by opt\mathcal{M}_{opt}.

Sublemma 6.14.

All but at most one regular Weierstrass point is a marked point.

Proof.

Every cylinder on πopt(X,ω)\pi_{opt}(X,\omega) has a twin by Theorem 6.12 (3). If two regular Weierstrass point were unmarked then opt\mathcal{M}_{opt} contains a surface where these two Weierstrass points lie on the core curve of a cylinder CC (for instance since there is some cylinder between two regular Weierstrass points and there is a path in opt\mathcal{M}_{opt} moving any two regular Weierstrass points to any two others while fixing the underlying surface. This follows for instance since it is possible to arbitrarily permute the poles on a genus zero quadratic differential while fixing all zeros). Since CC is fixed by the hyperelliptic involution it is a free cylinder, contradicting Theorem 6.12 (3). ∎

Sublemma 6.15.

Let pp be a regular Weierstrass point on πopt(X,ω)\pi_{opt}(X,\omega) that is not a branch point. Let (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega) denote (X,ω)(X,\omega) with the marked points in πopt1(p)\pi_{opt}^{-1}(p) forgotten. Let \mathcal{M}^{\prime} denote the orbit closure of (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega). Then \mathcal{M}^{\prime} remains geminal.

Proof.

On πopt(X,ω)\pi_{opt}(X,\omega) any generic cylinder that contains pp in its boundary has a twin, i.e. the image of the cylinder under the hyperelliptic involution is distinct. This shows that no free generic cylinder on (X,ω)(X,\omega) contains a point in πopt1(p)\pi_{opt}^{-1}(p) in its boundary. Therefore, free cylinders on (X,ω)(X,\omega) remain free cylinders after forgetting these points.

Therefore if a cylinder DD in (X,ω)(X,\omega) contains a point of πopt1(p)\pi_{opt}^{-1}(p) in its boundary, it has a twin DD^{\prime}. Moreover, there is a cylinder CC on πopt(X,ω)\pi_{opt}(X,\omega) that is divided into two by the marked Weierstrass point pp and another, not necessarily marked, Weierstrass point pp^{\prime}, and so DD=πopt1(C)D\cup D^{\prime}=\pi_{opt}^{-1}(C). If pp^{\prime} is marked, then DD and DD^{\prime} remain cylinders on (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega) and in particular they remain twins. If pp^{\prime} is unmarked, then DDD\cup D^{\prime} becomes a single free cylinder on (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega). This shows that \mathcal{M} remains geminal. ∎

If there are two regular Weierstrass points on πopt(X,ω)\pi_{opt}(X,\omega) that are not branch points of πopt\pi_{opt}, then forgetting them (as in Sublemma 6.15), produces a geminal invariant subvariety that contradicts Sublemma 6.14. ∎

7. hh-geminal subvarieties up to marked points

In this section we will study invariant subvarieties that are hh-geminal up to marked points. We will show that every surface in such a variety has an optimal map and study limits of that map under general cylinder degenerations.

Definition 7.1.

An invariant subvariety \mathcal{M} is said to be hh-geminal up to marked points if there is a surface (X,ω)(X,\omega) in \mathcal{M} with dense orbit and a finite collection PP of \mathcal{M}-periodic points on (X,ω)(X,\omega) so that the orbit closure of (X,ω;P)(X,\omega;P) is hh-geminal.

If \mathcal{M} has rank at least two, then let pt\mathcal{M}^{pt} denote \mathcal{M} with all its periodic points marked. Since \mathcal{M} has rank at least two, only a finite number of periodic points must be added by Eskin-Filip-Wright [EFW18, Theorem 1.5] (see Apisa-Wright [AWc, Section 4.2] for a discussion). In this case, \mathcal{M} is hh-geminal up to marked points if pt\mathcal{M}^{pt} is hh-geminal.

We begin by showing that adding all the periodic points to an hh-geminal subvariety of rank at least two does not change the fact that it is hh-geminal.

Lemma 7.2.

If \mathcal{M} is an hh-geminal subvariety of rank at least two, then pt\mathcal{M}^{pt} is also hh-geminal.

Proof.

By Theorem 6.12 (2), \mathcal{M} is either a nonhyperelliptic component of a stratum of Abelian differentials or a locus of covers of a genus zero quadratic double. In the first case there are no periodic points by Theorem 6.4. On a quadratic double of a genus zero stratum, the only periodic points are fixed points of the hyperelliptic involution by Theorem 6.5. After marking such points, the locus is still a quadratic double of a genus zero stratum. The result now follows since a full locus of good covers of a genus zero quadratic double is hh-geminal. ∎

Lemma 7.3.

Let f:(X,ω)(Y,η)f:(X,\omega)\operatorname{\rightarrow}(Y,\eta) be a good translation cover. Fix a marked point q(Y,η)q\in(Y,\eta). Let (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega) denote (X,ω)(X,\omega) with a subset of the points in f1(q)f^{-1}(q) removed. Let (Y,η)\operatorname{\mathcal{F}}^{\prime}(Y,\eta) denote (Y,η)(Y,\eta) where, if every preimage of qq is removed, qq is removed, and where (Y,η)=(Y,η)\operatorname{\mathcal{F}}^{\prime}(Y,\eta)=(Y,\eta) otherwise. We adopt the convention that a zero can never be unmarked. Then f:(X,ω)(Y,η)f:\operatorname{\mathcal{F}}^{\prime}(X,\omega)\operatorname{\rightarrow}\operatorname{\mathcal{F}}^{\prime}(Y,\eta) is good.

Proof.

By assumption, the preimage under ff of a cylinder C(Y,η)C\subseteq(Y,\eta) is a single cylinder. If some of the preimages of qq remain marked on (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega), then f1(C)f^{-1}(C) remains a cylinder on (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega). In other words, the only way that f:(Y,η)(X,ω)f:\operatorname{\mathcal{F}}^{\prime}(Y,\eta)\operatorname{\rightarrow}\operatorname{\mathcal{F}}^{\prime}(X,\omega) could fail to be good is if every preimage of qq has been removed (in particular, qq is not a branch point); we make this assumption now.

It is easy to see that if CC is a cylinder on (Y,η)(Y,\eta) that continues to be a cylinder on (Y,η)\operatorname{\mathcal{F}}^{\prime}(Y,\eta) then its preimage on (X,ω)\operatorname{\mathcal{F}}^{\prime}(X,\omega) continues to be a single cylinder.

We must therefore consider the situation where CC ceases to be a cylinder on (Y,η)\operatorname{\mathcal{F}}^{\prime}(Y,\eta), i.e. where, on (Y,η)(Y,\eta), one of its boundary components consists of a saddle connection ss joining qq to itself. Since qq is a marked point, there is another cylinder CC^{\prime} on (Y,η)(Y,\eta) that also has ss as one of the components of its boundary. While CC is no longer a cylinder on (Y,η)\operatorname{\mathcal{F}}^{\prime}(Y,\eta), CCC\cup C^{\prime} is. On (X,ω)(X,\omega) the preimage of CCC\cup C^{\prime} is a union of two cylinders DDD\cup D^{\prime} both of which share a boundary component f1(s)f^{-1}(s). Since qq is not a branch point, f1(s)f^{-1}(s) is just a collection of saddle connections joining marked points in the preimage of qq. In particular, once we forget all preimages of qq, DDD\cup D^{\prime} becomes a single cylinder.

Since every cylinder on (Y,η)\operatorname{\mathcal{F}}^{\prime}(Y,\eta) was either a cylinder on (Y,η)(Y,\eta) or contains a cylinder on (Y,η)(Y,\eta) that ceases to be one on (Y,η)\operatorname{\mathcal{F}}^{\prime}(Y,\eta), we are done. ∎

Corollary 7.4.

Let \mathcal{M} be a rank at least two invariant subvariety that is hh-geminal up to marked points. If (X,ω)(X,\omega) has dense orbit in \mathcal{M}, then πXmin\pi_{X_{min}} is \mathcal{M}-optimal.

Proof.

Let (X,ω)pt(X,\omega)^{pt} denote (X,ω)(X,\omega) with all of its \mathcal{M}-periodic points marked. By definition, its orbit closure is pt\mathcal{M}^{pt}, which is hh-geminal by assumption. By Theorem 6.12 (1), πXmin\pi_{X_{min}} is an optimal map when its domain is taken to be (X,ω)pt(X,\omega)^{pt}. Therefore, πXmin\pi_{X_{min}} is a good map even when its domain is taken to be (X,ω)(X,\omega) (by Lemma 7.3). The map is optimal by Theorem 6.1. \mathcal{M}-optimality follows by Remark 6.10. ∎

Corollary 7.5.

Suppose that 𝐂\mathbf{C} is a collection of generic \mathcal{M}-equivalent cylinders on a surface (X,ω)(X,\omega) in an invariant subvariety \mathcal{M} so that σ𝐂T(X,ω)\sigma_{\mathbf{C}}\in T_{(X,\omega)}\mathcal{M} and such that one of the following holds:

  1. (1)

    \mathcal{M} has rank one and minimal homological dimension.

  2. (2)

    \mathcal{M} has rank at least two and is hh-geminal up to marked points.

Let πopt\pi_{opt} be the \mathcal{M}-optimal map on (X,ω)(X,\omega). If 𝐂\mathcal{M}_{\mathbf{C}} has dimension one less than that of \mathcal{M}, then Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) is connected and Col𝐂(πopt)\operatorname{Col}_{\mathbf{C}}(\pi_{opt}) is 𝐂\mathcal{M}_{\mathbf{C}}-optimal. Moreover, if \mathcal{M} has rank two, then 𝐂\mathcal{M}_{\mathbf{C}} is hh-geminal up to marked points.

Proof.

When \mathcal{M} has rank one this claim is immediate from Theorem 6.11. Therefore, assume that \mathcal{M} has rank at least two and that it is hh-geminal up to marked points.

Let 𝐂pt\mathbf{C}^{pt} denote the cylinders corresponding to 𝐂\mathbf{C} on (X,ω)pt(X,\omega)^{pt}, which we will use to denote the surface (X,ω)(X,\omega) with all of its periodic points marked. Assume without loss of generality that 𝐂\mathbf{C} is horizontal.

Sublemma 7.6.

There is an arbitrarily small purely imaginary vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) so that after replacing (X,ω)(X,\omega) with (X,ω)+v(X,\omega)+v, the cylinders in 𝐂pt\mathbf{C}^{pt} are pt\mathcal{M}^{pt}-generic.

Proof.

If \mathcal{M} is a nonhyperelliptic component of a stratum, then 𝐂=𝐂pt\mathbf{C}=\mathbf{C}^{pt} (by Theorem 6.4) and there is nothing to show. Otherwise, \mathcal{M} is a full locus of covers of a hyperelliptic locus (by Theorem 6.12 (2)).

Let 𝐃\mathbf{D} (resp. 𝐃pt\mathbf{D}^{pt}) be the cylinders that are the image of 𝐂\mathbf{C} (resp. 𝐂pt\mathbf{C}^{pt}) under πopt\pi_{opt}. It follows from Theorem 6.5 that, since the cylinders in 𝐃\mathbf{D} are generic, the cylinders in 𝐃pt\mathbf{D}^{pt} fail to be generic if and only if there are two free points pp and pp^{\prime} on the boundary of cylinders in 𝐃\mathbf{D} so that, letting JJ denote the hyperelliptic involution, pp and J(p)J(p^{\prime}) lie on the same horizontal leaf. It is always possible to move free points along vertical leaves to avoid this. ∎

Notice that using the previous sublemma to replace (X,ω)(X,\omega) with (X,ω)+v(X,\omega)+v does not affect the surface Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) since vv was a purely imaginary element of Twist(𝐂,)\mathrm{Twist}(\mathbf{C},\mathcal{M}) and since, to form Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) we vertically collapse the cylinders in 𝐂\mathbf{C}. Therefore, assume without loss of generality that 𝐂pt\mathbf{C}^{pt} consists of pt\mathcal{M}^{pt}-generic cylinders.

Sublemma 7.7.

𝐂\mathcal{M}_{\mathbf{C}} is hh-geminal up to marked points. Moreover,

rank(𝐂)=rank(𝐂ptpt)anddim𝐂ptpt=dimpt1.\mathrm{rank}(\mathcal{M}_{\mathbf{C}})=\mathrm{rank}(\mathcal{M}_{\mathbf{C}^{pt}}^{pt})\qquad\text{and}\qquad\dim\mathcal{M}_{\mathbf{C}^{pt}}^{pt}=\dim\mathcal{M}^{pt}-1.
Proof.

Since Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) is simply Col𝐂pt((X,ω)pt)\operatorname{Col}_{\mathbf{C}^{pt}}\left((X,\omega)^{pt}\right) with some marked points forgotten, we have that dim𝐂ptptdim𝐂\dim\mathcal{M}^{pt}_{\mathbf{C}^{pt}}\geq\dim\mathcal{M}_{\mathbf{C}} and rank(𝐂)=rank(𝐂ptpt)\mathrm{rank}(\mathcal{M}_{\mathbf{C}})=\mathrm{rank}(\mathcal{M}_{\mathbf{C}^{pt}}^{pt}). By definition of periodic points, and since the dimension always decreases when passing to the boundary, we have the following,

dim1=dim𝐂dim𝐂ptptdimpt1=dim1.\dim\mathcal{M}-1=\dim\mathcal{M}_{\mathbf{C}}\leq\dim\mathcal{M}^{pt}_{\mathbf{C}^{pt}}\leq\dim\mathcal{M}^{pt}-1=\dim\mathcal{M}-1.

This shows that dim𝐂ptpt=dim𝐂\dim\mathcal{M}^{pt}_{\mathbf{C}^{pt}}=\dim\mathcal{M}_{\mathbf{C}} and hence that the marked points forgotten in the passage from Col𝐂pt((X,ω)pt)\operatorname{Col}_{\mathbf{C}^{pt}}\left((X,\omega)^{pt}\right) to Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) were periodic points. In particular, 𝐂\mathcal{M}_{\mathbf{C}} is hh-geminal up to marked points since 𝐂ptpt\mathcal{M}^{pt}_{\mathbf{C}^{pt}} is hh-geminal by Apisa-Wright [AWa, Lemma 4.4]. ∎

Sublemma 7.8.

𝐂\mathcal{M}_{\mathbf{C}} and 𝐂ptpt\mathcal{M}_{\mathbf{C}^{pt}}^{pt} consist of connected surfaces, have minimal homological dimension, and Col𝐂pt(πopt)\operatorname{Col}_{\mathbf{C}^{pt}}(\pi_{opt}) is 𝐂ptpt\mathcal{M}_{\mathbf{C}^{pt}}^{pt}-optimal.

Proof.

Since pt\mathcal{M}^{pt} is hh-geminal by assumption, it follows that it has minimal homological dimension (this follows from Theorem 6.12 (2)). Therefore, Col𝐂pt((X,ω)pt)\operatorname{Col}_{\mathbf{C}^{pt}}((X,\omega)^{pt}) is connected and 𝐂ptpt\mathcal{M}_{\mathbf{C}^{pt}}^{pt} has minimal homological dimension (by Corollary 3.3). The same holds for Col𝐂(X,ω)\operatorname{Col}_{\mathbf{C}}(X,\omega) and 𝐂\mathcal{M}_{\mathbf{C}} respectively. By Theorem 6.12 (4), Col𝐂pt(πopt)\operatorname{Col}_{\mathbf{C}^{pt}}(\pi_{opt}) is 𝐂ptpt\mathcal{M}^{pt}_{\mathbf{C}^{pt}}-optimal (note that the condition that dim𝐂ptpt=dimpt1\dim\mathcal{M}_{\mathbf{C}^{pt}}^{pt}=\dim\mathcal{M}^{pt}-1 is satisfied by Sublemma 7.7). Note that in this proof the application of Theorem 6.12 and Corollary 3.3 required that 𝐂pt\mathbf{C}^{pt} consisted of generic cylinders. ∎

It remains to see that Col𝐂(πopt)\operatorname{Col}_{\mathbf{C}}(\pi_{opt}) is 𝐂\mathcal{M}_{\mathbf{C}}-optimal. Suppose first that 𝐂\mathcal{M}_{\mathbf{C}} has rank one. By Sublemma 7.8 and Theorem 6.11, Col𝐂pt(πopt)=πabs\operatorname{Col}_{\mathbf{C}^{pt}}(\pi_{opt})=\pi_{abs}. Therefore, Col𝐂(πopt)=πabs\operatorname{Col}_{\mathbf{C}}(\pi_{opt})=\pi_{abs}, which is the 𝐂\mathcal{M}_{\mathbf{C}}-optimal map (by Sublemma 7.8 and Theorem 6.11).

Suppose finally that 𝐂\mathcal{M}_{\mathbf{C}} has rank two. By Sublemma 7.8 and Theorem 6.12 (1), when Col𝐂pt(πopt)\operatorname{Col}_{\mathbf{C}^{pt}}(\pi_{opt}) is deformed to a nearby surface with dense orbit it is the minimal cover. The same must hold for Col𝐂(πopt)\operatorname{Col}_{\mathbf{C}}(\pi_{opt}) and hence Col𝐂(πopt)\operatorname{Col}_{\mathbf{C}}(\pi_{opt}) must be 𝐂\mathcal{M}_{\mathbf{C}}-optimal (by Corollary 7.4 and the fact that we have established that 𝐂\mathcal{M}_{\mathbf{C}} is hh-geminal up to marked points and of rank at least two). ∎

7.1. General degenerations of optimal maps

At this point we have shown that, if \mathcal{M} is hh-geminal up to marked points, then the surfaces in \mathcal{M} possess \mathcal{M}-optimal maps that are well-behaved with respect to cylinder degenerations performed using the standard shear. We now wish to study what happens to these optimal maps under more general cylinder degenerations.

Throughout this subsection we will assume that 𝐂\mathbf{C} is an equivalence class of generic cylinders on a surface (X,ω)(X,\omega) in an invariant subvariety \mathcal{M} and that vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) defines a cylinder degeneration.

Definition 7.9.

Say that vv is orthogonal if, after rotating 𝐂\mathbf{C} so that it is horizontal, vv is purely imaginary.

Recall that 𝐂v\mathbf{C}_{v} was defined in Definition 2.10.

Definition 7.10.

Suppose that π:(X,ω)(Y,η)\pi:(X,\omega)\operatorname{\rightarrow}(Y,\eta) is a good map and that vv is orthogonal. By definition, for each cylinder C𝐂C\in\mathbf{C} there is a cylinder D(Y,η)D\subseteq(Y,\eta) whose full preimage under π\pi is CC. If v=C𝐂aCγCv=\sum_{C\in\mathbf{C}}a_{C}\gamma_{C}^{*} where aCa_{C}\in\mathbb{C} and γC\gamma_{C} denotes the core curve of CC, then let π(v):=C𝐂aCγπ(C)\pi(v):=\sum_{C\in\mathbf{C}}a_{C}\gamma_{\pi(C)}^{*}. It is obvious that (X,ω)+tv(X,\omega)+tv remains a translation cover of (Y,η)+tπ(v)(Y,\eta)+t\pi(v). Both of these paths converge to surfaces (X,ω)(X^{\prime},\omega^{\prime}) and (Y,η)(Y^{\prime},\eta^{\prime}) by Apisa-Wright [AWb, Lemma 4.9] as tt approaches tvt_{v} (see Definition 2.10 for the definition of tvt_{v}). Notice that setting v:=C𝐂vaCγCv^{\prime}:=\sum_{C\notin\mathbf{C}_{v}}a_{C}\gamma_{C}^{*} (and using that vv is orthogonal) we have

(X,ω)=Col𝐂v((X,ω)+v)and(Y,ω)=Colπ(𝐂)π(v)((Y,η)+v).(X^{\prime},\omega^{\prime})=\operatorname{Col}_{\mathbf{C}_{v}}((X,\omega)+v^{\prime})\quad\text{and}\quad(Y^{\prime},\omega^{\prime})=\operatorname{Col}_{\pi(\mathbf{C})_{\pi(v)}}((Y,\eta)+v^{\prime}).

Since passing from (X,ω)(X,\omega) to (X,ω)+v(X,\omega)+v^{\prime} simply involves applying an invertible linear map to cylinders in 𝐂𝐂v\mathbf{C}-\mathbf{C}_{v}, it is clear that π\pi induces a map

π:(X,ω)+v(Y,η)+π(v).\pi^{\prime}:(X,\omega)+v^{\prime}\operatorname{\rightarrow}(Y,\eta)+\pi(v^{\prime}).

Define a map

Colv(π):Colv(X,ω)Colπ(v)(Y,η).\operatorname{Col}_{v}(\pi):\operatorname{Col}_{v}(X,\omega)\operatorname{\rightarrow}\operatorname{Col}_{\pi(v)}(Y,\eta).

by setting Colv(π):=Col𝐂v(π)\operatorname{Col}_{v}(\pi):=\operatorname{Col}_{\mathbf{C}_{v}}(\pi^{\prime}).

Lemma 7.11.

Suppose that vv is orthogonal and that 𝐂¯(X,ω)\overline{\mathbf{C}}\neq(X,\omega). If Colv(X,ω)\operatorname{Col}_{v}(X,\omega) is connected, then there is an arbitrarily small element wTwist(𝐂𝐂v,)w\in\mathrm{Twist}(\mathbf{C}-\mathbf{C}_{v},\mathcal{M}) so that Colv(X,ω)\operatorname{Col}_{v}(X,\omega) and Col𝐂((X,ω)+w)\operatorname{Col}_{\mathbf{C}}\left((X,\omega)+w\right) belong to the same component of the boundary.

The connectedness is solely used to apply the cylinder deformation theorem to surfaces in v\mathcal{M}_{v}.

Proof.

Without loss of generality, suppose that 𝐂\mathbf{C} is horizontal and vv is purely imaginary. If 𝐂v=𝐂\mathbf{C}_{v}=\mathbf{C} there is nothing to show, so suppose that this is not the case. Since Colv(𝐂)\operatorname{Col}_{v}(\mathbf{C}) remains an equivalence class of cylinders, the standard shear is an element of TColv(X,ω)vT_{\operatorname{Col}_{v}(X,\omega)}\mathcal{M}_{v} by the cylinder deformation theorem. Let ww be the corresponding element in Twist(𝐂𝐂v,)\mathrm{Twist}(\mathbf{C}-\mathbf{C}_{v},\mathcal{M}). For almost every real aa, (X,ω)+aw(X,\omega)+aw contains no vertical saddle connections in 𝐂¯\overline{\mathbf{C}} except for those in 𝐂v¯\overline{\mathbf{C}_{v}}. Notice that Colv(X,ω)\operatorname{Col}_{v}(X,\omega) is in the same component of the boundary as

Colv(X,ω)+aσColv(𝐂)=Colv((X,ω)+aw).\operatorname{Col}_{v}(X,\omega)+a\sigma_{\operatorname{Col}_{v}(\mathbf{C})}=\operatorname{Col}_{v}((X,\omega)+aw).

Since Colv((X,ω)+aw)\operatorname{Col}_{v}((X,\omega)+aw) contains no vertical saddle connections in Colv(𝐂)¯\overline{\operatorname{Col}_{v}(\mathbf{C})} (by our choice of aa), it belongs to the same component of the boundary as

ColColv(𝐂)Colv((X,ω)+aw)=Col𝐂((X,ω)+aw).\operatorname{Col}_{\operatorname{Col}_{v}(\mathbf{C})}\operatorname{Col}_{v}((X,\omega)+aw)=\operatorname{Col}_{\mathbf{C}}\left((X,\omega)+aw\right).

This shows that Colv(X,ω)\operatorname{Col}_{v}(X,\omega) and Col𝐂((X,ω)+aw)\operatorname{Col}_{\mathbf{C}}\left((X,\omega)+aw\right) belong to the same component of the boundary, as desired. ∎

Lemma 7.12.

Suppose that vv is orthogonal and that 𝐂¯(X,ω)\overline{\mathbf{C}}\neq(X,\omega). Suppose that 𝐂=v\mathcal{M}_{\mathbf{C}}=\mathcal{M}_{v} and that Colv(X,ω)\operatorname{Col}_{v}(X,\omega) is connected. Suppose finally that π\pi is a translation cover with domain (X,ω)(X,\omega). If Col𝐂(π)\operatorname{Col}_{\mathbf{C}}(\pi) is 𝐂\mathcal{M}_{\mathbf{C}}-optimal, then so is Colv(π)\operatorname{Col}_{v}(\pi).

Proof.

Suppose without loss of generality that 𝐂\mathbf{C} is horizontal. If 𝐂v=𝐂\mathbf{C}_{v}=\mathbf{C} there is nothing to prove so suppose that this is not the case. Let γ(t)=Colv(X,ω)itσColv(𝐂)\gamma(t)=\operatorname{Col}_{v}(X,\omega)-it\sigma_{\operatorname{Col}_{v}(\mathbf{C})}, which is a path in v\mathcal{M}_{v} (by the cylinder deformation theorem) so that γ(1)=Col𝐂(X,ω)\gamma(1)=\operatorname{Col}_{\mathbf{C}}(X,\omega). By assumption, Col𝐂(π)\operatorname{Col}_{\mathbf{C}}(\pi) is 𝐂\mathcal{M}_{\mathbf{C}}-optimal, so it is possible to deform it along the path so that it becomes a translation cover π\pi^{\prime} on Colv(X,ω)\operatorname{Col}_{v}(X,\omega). Since π\pi^{\prime} and Colv(π)\operatorname{Col}_{v}(\pi) are holomorphic maps that have the same fibers on the open set Colv(X,ω)Colv(𝐂)\operatorname{Col}_{v}(X,\omega)-\operatorname{Col}_{v}(\mathbf{C}), they must coincide and so Colv(π)\operatorname{Col}_{v}(\pi) is \mathcal{M}-optimal. ∎

8. Proof of Theorem 1.5

This section is devoted to the proof of Theorem 1.5. We proceed by induction using Proposition 5.1 as the base case. The following assumption is the inductive hypothesis.

Assumption 8.1.

Suppose that \mathcal{M} is an invariant subvariety of minimal homological dimension that is rank at least two and not rank two rel zero. Any smaller dimensional invariant subvariety of minimal homological dimension and rank at least two is hh-geminal up to marked points.

Our goal is to show that \mathcal{M} is hh-geminal up to marked points.

Lemma 8.2.

If (X,ω)(X,\omega) has dense orbit in \mathcal{M}, then πXmin\pi_{X_{min}} is \mathcal{M}-optimal.

Suppose additionally that 𝐂\mathbf{C} is a generic equivalence class of cylinders with vTwist(𝐂,)v\in\mathrm{Twist}(\mathbf{C},\mathcal{M}) defining a typical orthogonal cylinder degeneration. Then v\mathcal{M}_{v} has minimal homological dimension, Colv(X,ω)\operatorname{Col}_{v}(X,\omega) is connected, and Colv(πXmin)\operatorname{Col}_{v}(\pi_{X_{min}}) is v\mathcal{M}_{v}-optimal.

Proof.

Throughout this proof it will be important to keep Remark 6.10 in mind.

Let 𝐂1\mathbf{C}_{1} be an equivalence class of cylinders on (X,ω)(X,\omega). After perhaps perturbing we may assume that the cylinders in 𝐂1\mathbf{C}_{1} are horizontal and form a generic equivalence class. After perturbing again (using Corollary 3.1 and Lemma 2.7 (3)), suppose that (X,ω)(X,\omega) is cylindrically stable.

If 𝐂1\mathbf{C}_{1} is involved with rel (see Definition 2.11) or if the rank of \mathcal{M} is at least three, then let 𝐂2\mathbf{C}_{2} be any other equivalence class of horizontal cylinders. If \mathcal{M} has rank two and 𝐂1\mathbf{C}_{1} is not involved with rel then let 𝐂2\mathbf{C}_{2} be any equivalence class of horizontal cylinders involved with rel (such an equivalence class of cylinders exists since, when \mathcal{M} has rank two, it has positive rel, by Assumption 8.1, and so at least one horizontal equivalence class of cylinders is involved with rel by definition of cylindrical stability). Perturb (X,ω)(X,\omega) once more so that 𝐂1\mathbf{C}_{1} and 𝐂2\mathbf{C}_{2} become generic equivalence classes and so (X,ω)(X,\omega) has dense orbit in \mathcal{M}.

For i{1,2}i\in\{1,2\}, there is a viTwist(𝐂i,)v_{i}\in\mathrm{Twist}(\mathbf{C}_{i},\mathcal{M}) that defines a typical cylinder degeneration (by Theorem 2.13). Without loss of generality, after perhaps applying the standard shear to 𝐂1\mathbf{C}_{1} and 𝐂2\mathbf{C}_{2}, we may suppose that v1v_{1} and v2v_{2} are typical orthogonal degenerations (see Remark 2.12). By Lemma 7.11, we may suppose, again after perhaps perturbing, that vi=𝐂i\mathcal{M}_{v_{i}}=\mathcal{M}_{\mathbf{C}_{i}}. Notice that the following hold:

  1. (1)

    vi\mathcal{M}_{v_{i}} has minimal homological dimension and consists of connected surfaces by Corollary 3.3.

  2. (2)

    vi\mathcal{M}_{v_{i}} has codimension one and rank(vi)=rank()\mathrm{rank}(\mathcal{M}_{v_{i}})=\mathrm{rank}(\mathcal{M}) if 𝐂i\mathbf{C}_{i} is involved with rel and rank(vi)=rank()1\mathrm{rank}(\mathcal{M}_{v_{i}})=\mathrm{rank}(\mathcal{M})-1 otherwise, by Theorem 2.13.

  3. (3)

    If vi\mathcal{M}_{v_{i}} has rank at least two, then it is hh-geminal up to marked points and any surface (X,ω)(X,\omega) with dense orbit in vi\mathcal{M}_{v_{i}} has the property that πXmin\pi_{X_{min}} is vi\mathcal{M}_{v_{i}}-optimal (by (1), Assumption 8.1, and Corollary 7.4). Note that vi\mathcal{M}_{v_{i}} has rank at least two when \mathcal{M} has rank at least three and also when 𝐂i\mathbf{C}_{i} is involved with rel by (2). Our choice of 𝐂2\mathbf{C}_{2} implies that this occurs for v1\mathcal{M}_{v_{1}} or v2\mathcal{M}_{v_{2}} and possibly for both.

  4. (4)

    On Col𝐂i(X,ω)\operatorname{Col}_{\mathbf{C}_{i}}(X,\omega) there is an 𝐂i\mathcal{M}_{\mathbf{C}_{i}}-optimal map πi\pi_{i} (by (1) and Theorem 6.11 when vi\mathcal{M}_{v_{i}} has rank one and by (3) when vi\mathcal{M}_{v_{i}} has rank at least two).

  5. (5)

    Since Col𝐂i+1(𝐂i)\operatorname{Col}_{\mathbf{C}_{i+1}}(\mathbf{C}_{i}) remains a collection of generic equivalent cylinder with 𝐂1,𝐂2\mathcal{M}_{\mathbf{C}_{1},\mathbf{C}_{2}} having dimension one less than 𝐂i\mathcal{M}_{\mathbf{C}_{i}} (by Theorem 2.13), ColCol𝐂i(𝐂i+1)(πi)\operatorname{Col}_{\operatorname{Col}_{\mathbf{C}_{i}}(\mathbf{C}_{i+1})}(\pi_{i}) is the unique 𝐂1,𝐂2\mathcal{M}_{\mathbf{C}_{1},\mathbf{C}_{2}}-optimal map on Col𝐂1,𝐂2(X,ω)\operatorname{Col}_{\mathbf{C}_{1},\mathbf{C}_{2}}(X,\omega) (by Corollary 7.5).

In light of (5), by the diamond lemma (Apisa-Wright [AWd, Lemma 2.3]), there is a map π\pi on (X,ω)(X,\omega) so that Col𝐂i(π)=πi\operatorname{Col}_{\mathbf{C}_{i}}(\pi)=\pi_{i}. Note that the condition in the diamond lemma that πi1(πi(Col𝐂i(𝐂i+1)))=Col𝐂i(𝐂i+1)\pi_{i}^{-1}\left(\pi_{i}\left(\operatorname{Col}_{\mathbf{C}_{i}}(\mathbf{C}_{i+1})\right)\right)=\operatorname{Col}_{\mathbf{C}_{i}}(\mathbf{C}_{i+1}) follows by definition of 𝐂i\mathcal{M}_{\mathbf{C}_{i}}-optimal.

By (3) there is some j{1,2}j\in\{1,2\} so that πj\pi_{j} is 𝐂j\mathcal{M}_{\mathbf{C}_{j}}-generic and becomes πYmin\pi_{Y_{min}} for any nearby surface (Y,η)(Y,\eta) with dense orbit in 𝐂j\mathcal{M}_{\mathbf{C}_{j}}. Since πXmin\pi_{X_{min}} is \mathcal{M}-generic (since (X,ω)(X,\omega) has dense orbit in \mathcal{M}), it follows that Col𝐂j(πXmin)\operatorname{Col}_{\mathbf{C}_{j}}(\pi_{X_{min}}) is 𝐂j\mathcal{M}_{\mathbf{C}_{j}}-generic (it suffices to note that a neighborhood of Col𝐂j(X,ω)\operatorname{Col}_{\mathbf{C}_{j}}(X,\omega) can be obtained by perturbing (X,ω)(X,\omega) and then collapsing 𝐂j\mathbf{C}_{j}. This follows from Mirzakhani-Wright [MW17, Proposition 2.6] together with the main results of Mirzakhani-Wright and Chen-Wright [MW17, CW19].) If ππXmin\pi\neq\pi_{X_{min}}, then Col𝐂j(πXmin)\operatorname{Col}_{\mathbf{C}_{j}}(\pi_{X_{min}}) has larger degree than πj\pi_{j}. So on a nearby surface (Y,η)𝐂j(Y,\eta)\in\mathcal{M}_{\mathbf{C}_{j}} with dense orbit the map corresponding to Col𝐂j(πXmin)\operatorname{Col}_{\mathbf{C}_{j}}(\pi_{X_{min}}) would have larger degree than πYmin\pi_{Y_{min}}. This contradicts Theorem 6.1 and shows that π=πXmin\pi=\pi_{X_{min}}.

Since 𝐂1\mathbf{C}_{1} is arbitrary and each cylinder in it is the full preimage of its image under π\pi (since this is the case for Col𝐂2(𝐂1)\operatorname{Col}_{\mathbf{C}_{2}}(\mathbf{C}_{1}) with respect to π2\pi_{2}), it follows that πXmin\pi_{X_{min}} is \mathcal{M}-optimal. Since v1v_{1} was an arbitrary typical orthogonal cylinder degeneration of 𝐂1\mathbf{C}_{1} and since we arranged for v1=𝐂1\mathcal{M}_{v_{1}}=\mathcal{M}_{\mathbf{C}_{1}}, the second claim follows from Lemma 7.12. ∎

We now proceed with the proof that \mathcal{M} is hh-geminal up to marked points. Fix a surface (X,ω)(X,\omega) with dense orbit in \mathcal{M} and let (X,ω)(X^{\prime},\omega^{\prime}) denote (X,ω)(X,\omega) with all of its periodic points marked. Let min\mathcal{M}_{min} (resp. min\mathcal{M}_{min}^{\prime}) denote the orbit closure of (Xmin,ωmin)(X_{min},\omega_{min}) (resp. (Xmin,ωmin)(X_{min}^{\prime},\omega_{min}^{\prime})). Notice that these surfaces first appear in Theorem 6.1.

Recall the convention that if CC is a cylinder we will let γC\gamma_{C}^{*} denote the intersection pairing with its core curve.

Lemma 8.3.

If min\mathcal{M}_{min} has full rank, i.e. has rank equal to that of the stratum of Abelian differentials containing it, then \mathcal{M} is hh-geminal up to marked points.

Proof.

If min\mathcal{M}_{min} has full rank, then by Mirzakhani-Wright [MW18, Theorem 1.1], (min)\operatorname{\mathcal{F}}(\mathcal{M}_{min}) is either a nonhyperelliptic component of a stratum of Abelian differentials or a hyperelliptic locus (possibly equal to the full component) of a stratum. In the first case (by Theorem 6.4), min\mathcal{M}_{min}^{\prime} is itself a stratum and so every cylinder is free. In the second (by Theorem 6.5), min\mathcal{M}_{min}^{\prime} is a hyperelliptic locus with every fixed point of the hyperelliptic involution marked and with all other marked points occurring in pairs exchanged by the hyperelliptic involution. In particular, min\mathcal{M}_{min}^{\prime} is a quadratic double and hence hh-geminal. Since πXmin\pi_{X_{min}} is optimal (by Lemma 8.2), every cylinder on (X,ω)(X^{\prime},\omega^{\prime}) contains exactly one cylinder in its preimage. This shows that the orbit closure of (X,ω)(X^{\prime},\omega^{\prime}) is hh-geminal and hence that \mathcal{M} is hh-geminal up to marked points. ∎

Our goal is therefore to show that min\mathcal{M}_{min} has full rank. The following is a useful test to determine when this is the case. For ease of notation we will let π:=πXmin\pi:=\pi_{X_{min}}.

Lemma 8.4.

Suppose that 𝐂\mathbf{C} is a generic equivalence class of cylinders on (X,ω)(X,\omega). Suppose too that CC is a cylinder in 𝐂\mathbf{C} so that π(C)\pi(C) has a boundary comprised of a single saddle connection. Suppose finally that vTwist(𝐂,)v\in\mathrm{Twist}\left(\mathbf{C},\mathcal{M}\right) determines an orthogonal cylinder degeneration with 𝐂v={C}\mathbf{C}_{v}=\{C\}. Then min\mathcal{M}_{min} has full rank.

Proof.

Without loss of generality (after perhaps rotating and shearing), suppose that 𝐂\mathbf{C} consists of horizontal cylinders and that π(C)\pi(C) contains a vertical saddle connection ss. If v=D𝐂aDγDv=\sum_{D\in\mathbf{C}}a_{D}\gamma_{D}^{*}, then let w:=D𝐂aDγπ(D)w:=\sum_{D\in\mathbf{C}}a_{D}\gamma_{\pi(D)}^{*}. Notice that ww is a purely imaginary rel vector in Tπ(X,ω)minT_{\pi(X,\omega)}\mathcal{M}_{min} and (π(𝐂))w={π(C)}(\pi(\mathbf{C}))_{w}=\{\pi(C)\}.

It is easy to see that, since π(C)\pi(C) has one boundary consisting of a single saddle connection, that Colw(X,ω)\operatorname{Col}_{w}(X,\omega) is connected and that the collection of vanishing cycles is just the line generated by ss. For instance the second claim follows from Apisa-Wright [AWb, Lemma 4.25]. Let \mathcal{H} be the component of the stratum of Abelian differentials containing π(X,ω)\pi(X,\omega). By Apisa-Wright [AWb, Lemma 3.8] since ww is a rel vector that evaluates nontrivially on ss, we have the following:

(8.0.1) rank((min)w)=rank(min)andrank(w)=rank().\mathrm{rank}((\mathcal{M}_{min})_{w})=\mathrm{rank}(\mathcal{M}_{min})\qquad\text{and}\qquad\mathrm{rank}(\mathcal{H}_{w})=\mathrm{rank}(\mathcal{H}).

By Lemma 8.2, since vv is a typical orthogonal degeneration, v\mathcal{M}_{v} has minimal homological dimension and consists of connected surfaces. By Equation 8.0.1 (which implies that rank(v)=rank()\mathrm{rank}(\mathcal{M}_{v})=\mathrm{rank}(\mathcal{M})) and Assumption 8.1, v\mathcal{M}_{v} is hh-geminal up to marked points and the v\mathcal{M}_{v}-optimal map coincides with the minimal cover on any surface in v\mathcal{M}_{v} with dense orbit (by Corollary 7.4). Therefore, by Lemma 8.2 we have the following,

(min)w=(v)min.(\mathcal{M}_{min})_{w}=(\mathcal{M}_{v})_{min}.

Moreover, since v\mathcal{M}_{v} is hh-geminal up to marked points, (v)min(\mathcal{M}_{v})_{min} has full rank (by Theorem 6.12 (2)). Since (min)w\left(\mathcal{M}_{min}\right)_{w} has the same rank as w\mathcal{H}_{w}, the same is true of min\mathcal{M}_{min} and \mathcal{H}, by Equation (8.0.1), as desired. ∎

We will now rephrase the preceding result into the form in which we will apply it.

Corollary 8.5.

Suppose that 𝐂\mathbf{C} is a generic equivalence class containing at least two horizontal cylinders on (X,ω)(X,\omega). Suppose too that ww is a typical orthogonal degeneration in Twist(𝐃,)\mathrm{Twist}(\mathbf{D},\mathcal{M}) where w\mathcal{M}_{w} has rank at least two and where 𝐃\mathbf{D} is an equivalence class either equal to 𝐂\mathbf{C} or disjoint and not parallel to it. Finally suppose that one of the following happens:

  1. (1)

    There is a cylinder CC in 𝐂\mathbf{C} so that Colw(π)(Colw(C))\operatorname{Col}_{w}(\pi)(\operatorname{Col}_{w}(C)) is free, or

  2. (2)

    There are cylinders of generically equal circumference C1C_{1} and C2C_{2} in 𝐂\mathbf{C} so that γC1γC2T(X,ω)\gamma_{C_{1}}^{*}-\gamma_{C_{2}}^{*}\in T_{(X,\omega)}\mathcal{M}, or

  3. (3)

    There is a cylinder CC in 𝐂\mathbf{C} so that Colw(π)(Colw(C))\operatorname{Col}_{w}(\pi)(\operatorname{Col}_{w}(C)) contains a free marked point on its boundary.

Then \mathcal{M} is hh-geminal up to marked points.

Proof.

Note that w\mathcal{M}_{w} is either a stratum of Abelian differentials or a full locus of translation covers of a hyperelliptic locus (by Lemma 8.2, Assumption 8.1, and Theorem 6.12 (2)). In the second case, the cover is given by Colw(π)\operatorname{Col}_{w}(\pi) by Lemma 8.2.

Since the cylinders in 𝐂\mathbf{C} are generic, the same holds for those in Colw(𝐂)\operatorname{Col}_{w}(\mathbf{C}). This is obvious in the case that 𝐃\mathbf{D} is disjoint and non-parallel to 𝐂\mathbf{C} and follows from Theorem 2.13 in the case that 𝐂=𝐃\mathbf{C}=\mathbf{D}. Since Colw(π)(Colw(𝐂))\operatorname{Col}_{w}(\pi)\left(\operatorname{Col}_{w}(\mathbf{C})\right) is a collection of generic cylinders we see that those cylinders are all simple when w\mathcal{M}_{w} is a stratum and consists of simple and half-simple cylinders when w\mathcal{M}_{w} is a full locus of covers of a hyperelliptic locus (by Corollary 6.6). It follows that for each C𝐂C\in\mathbf{C}, π(C)\pi(C) is simple or half simple, since Colw(π)(Colw(C))\operatorname{Col}_{w}(\pi)(\operatorname{Col}_{w}(C)) has at least as many saddle connections on each boundary component as π(C)\pi(C).

By Lemmas 8.3 and 8.4 it suffices to show that there is a rel deformation that increases the height of one cylinder in 𝐂\mathbf{C} while not increasing the height of all other cylinders in 𝐂\mathbf{C}.

Suppose first that C𝐂C\in\mathbf{C} is a cylinder so that Colw(π)(Colw(C))\operatorname{Col}_{w}(\pi)(\operatorname{Col}_{w}(C)) is free. It follows that π(C)\pi(C) and hence CC itself are also free. By Mirzakhani-Wright (Theorem 2.3), since 𝐂{C}\mathbf{C}\neq\{C\}, there is a positive real number aa so that v:=i(γC+aσ𝐂)v:=i\left(-\gamma_{C}^{*}+a\sigma_{\mathbf{C}}\right) is rel. This is the desired rel deformation.

The second claim is immediate since γC1γC2\gamma_{C_{1}}^{*}-\gamma_{C_{2}}^{*} is rel by Apisa-Wright [AWb, Corollary 11.5].

Suppose now that C𝐂C\in\mathbf{C} is a cylinder so that Colw(π)(Colw(C))\operatorname{Col}_{w}(\pi)(\operatorname{Col}_{w}(C)) contains a free point on its boundary. Since this cylinder is generic, the boundary containing the free point must consist of a saddle connection ss joining the free marked point to itself. In particular, there is another cylinder D𝐂D\in\mathbf{C} so that Colw(π)(Colw(D))\operatorname{Col}_{w}(\pi)(\operatorname{Col}_{w}(D)) also has a boundary comprised of ss. It follows that, since the marked point is free, γCγDT(X,ω)\gamma_{C}^{*}-\gamma_{D}^{*}\in T_{(X,\omega)}\mathcal{M}. This reduces to the previous case. ∎

We may assume without loss of generality that \mathcal{M} is not geminal (by Lemma 7.2). Therefore, assume without loss of generality that there is an equivalence class 𝐂1\mathbf{C}_{1} of cylinders on (X,ω)(X,\omega) that does not admit a geminal partition (see Definition 6.7). As in the proof of Lemma 8.2, we may assume without loss of generality that 𝐂1\mathbf{C}_{1} is generic, horizontal, and that its complement contains a generic equivalence class 𝐂2\mathbf{C}_{2}. If ker(p)T(X,ω)\ker(p)\cap T_{(X,\omega)}\mathcal{M} is not contained in Twist(𝐂1,)\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M}), then we may additionally suppose that 𝐂2\mathbf{C}_{2} is involved with rel.

Lemma 8.6.

If \mathcal{M} has no rel or if ker(p)T(X,ω)\ker(p)\cap T_{(X,\omega)}\mathcal{M} is not contained in Twist(𝐂1,)\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M}), then \mathcal{M} is hh-geminal up to marked points.

Proof.

Let wTwist(𝐂2,)w\in\mathrm{Twist}(\mathbf{C}_{2},\mathcal{M}) define a typical orthogonal cylinder degeneration (such an element exists by Theorem 2.13 and Remark 2.12). w\mathcal{M}_{w} has rank at least two, of minimal homological dimension, and consists of connected surfaces (by Theorem 2.13 and Corollary 3.3). Moreover, Colw(π)\operatorname{Col}_{w}(\pi) is w\mathcal{M}_{w}-optimal (by Lemma 8.2). By Assumption 8.1 and Theorem 6.12 (2), w\mathcal{M}_{w} is either a non-hyperelliptic component of a stratum of Abelian differentials or a full locus of covers of a hyperelliptic locus. In the first case, all the cylinders in 𝐂1\mathbf{C}_{1} would be free, contradicting our assumption that 𝐂1\mathbf{C}_{1} does not admit a geminal partition. Therefore, suppose that (w)min(\mathcal{M}_{w})_{min} is a hyperelliptic locus.

Let 𝐃1:=Colw(π)(Colw(𝐂1))\mathbf{D}_{1}:=\operatorname{Col}_{w}(\pi)\left(\operatorname{Col}_{w}(\mathbf{C}_{1})\right). Since 𝐂1\mathbf{C}_{1} does not admit a geminal partition, the same holds for π(𝐂1)\pi(\mathbf{C}_{1}) and hence for 𝐃1\mathbf{D}_{1} as well, implying that the boundary of one of the cylinders in 𝐃1\mathbf{D}_{1} contains a free marked point (by Corollary 6.8). We are done by Corollary 8.5 (3). ∎

Suppose therefore that \mathcal{M} has rel and that ker(p)T(X,ω)Twist(𝐂1,)\ker(p)\cap T_{(X,\omega)}\mathcal{M}\subseteq\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M}).

Lemma 8.7.

If \mathcal{M} is not hh-geminal up to marked points, then for any typical orthogonal cylinder degeneration vTwist(𝐂1,)v\in\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M}), (v)min(\mathcal{M}_{v})_{min} is a genus zero quadratic double.

Equivalently, for any typical orthogonal cylinder degeneration wTwist(π(𝐂1),min)w\in\mathrm{Twist}(\pi(\mathbf{C}_{1}),\mathcal{M}_{min}), (min)w(\mathcal{M}_{min})_{w} is a genus zero quadratic double.

Proof.

Since 𝐂1\mathbf{C}_{1} is involved with rel by assumption, v\mathcal{M}_{v} has the same rank as \mathcal{M} (which is at least two) by Theorem 2.13. So v\mathcal{M}_{v} is either a component of a stratum of Abelian differentials or a full locus of translation covers of a hyperelliptic locus (by Assumption 8.1 and Theorem 6.12 (2)). In the first case, \mathcal{M} is hh-geminal up to marked points by Corollary 8.5 (1).

Suppose therefore that (v)min(\mathcal{M}_{v})_{min} is a hyperelliptic locus, but one which is not a quadratic double. That is, the marked points are not invariant by the hyperelliptic involution and so one of them must be free (by Theorem 6.5). Set 𝐃1:=Colv(π)(Colv(𝐂1))\mathbf{D}_{1}:=\operatorname{Col}_{v}(\pi)(\operatorname{Col}_{v}(\mathbf{C}_{1}))

Sublemma 8.8.

Every free marked point on Colv(π)(Colv(X,ω))\operatorname{Col}_{v}(\pi)(\operatorname{Col}_{v}(X,\omega)) is contained on the boundary of a cylinder in 𝐃1\mathbf{D}_{1}.

Proof.

By Theorem 2.13, rank()=rank(v)\mathrm{rank}(\mathcal{M})=\mathrm{rank}(\mathcal{M}_{v}) and dim(v)=dim()1\dim(\mathcal{M}_{v})=\dim(\mathcal{M})-1. Therefore, the dimension rvr_{v} of ker(p)TColv(X,ω)v\ker(p)\cap T_{\operatorname{Col}_{v}(X,\omega)}\mathcal{M}_{v} is exactly one less than the dimension rr of ker(p)T(X,ω)\ker(p)\cap T_{(X,\omega)}\mathcal{M}. In other words, rv=r1r_{v}=r-1. Since ker(p)T(X,ω)Twist(𝐂1,)\ker(p)\cap T_{(X,\omega)}\mathcal{M}\subseteq\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M}), we have, by Theorem 2.3,

dimTwist(𝐂1,)=r+1.\dim\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M})=r+1.

Since vv is typical, Twist(Colv(𝐂1),v)\mathrm{Twist}(\operatorname{Col}_{v}(\mathbf{C}_{1}),\mathcal{M}_{v}) has dimension exactly one less than that of Twist(𝐂1,)\mathrm{Twist}(\mathbf{C}_{1},\mathcal{M}) (for instance by Theorem 2.9), i.e.

dimTwist(Colv(𝐂1),v)=r=rv+1.\dim\mathrm{Twist}(\operatorname{Col}_{v}(\mathbf{C}_{1}),\mathcal{M}_{v})=r=r_{v}+1.

Since Colv(X,ω)\operatorname{Col}_{v}(X,\omega) is connected (by Corollary 3.3), it follows from Theorem 2.3 that ker(p)TColv(X,ω)vTwist(Colv(𝐂1),)\ker(p)\cap T_{\operatorname{Col}_{v}(X,\omega)}\mathcal{M}_{v}\subseteq\mathrm{Twist}(\operatorname{Col}_{v}(\mathbf{C}_{1}),\mathcal{M}).

Consequently, ker(p)TColv(π)(Colv(X,ω))(v)minTwist(𝐃1,(v)min)\ker(p)\cap T_{\operatorname{Col}_{v}(\pi)(\operatorname{Col}_{v}(X,\omega))}(\mathcal{M}_{v})_{min}\subseteq\mathrm{Twist}(\mathbf{D}_{1},(\mathcal{M}_{v})_{min}). In particular, every free marked point must be contained on the boundary of a cylinder in 𝐃1\mathbf{D}_{1}. ∎

Since the boundary of a cylinder in 𝐃1\mathbf{D}_{1} contains a free marked point, \mathcal{M} is hh-geminal up to marked points by Corollary 8.5 (3).

By the preceding lemma, we are left to consider the case where, for any typical orthogonal cylinder degeneration wTwist(π(𝐂1),min)w\in\mathrm{Twist}(\pi(\mathbf{C}_{1}),\mathcal{M}_{min}), (min)w(\mathcal{M}_{min})_{w} is a genus zero quadratic double. Note that by Apisa-Wright [AWb], specifically the argument beginning in the paragraph after the proof of Lemma 12.1 through the proof of Corollary 12.3, implies that there are two cylinders C1C_{1} and C2C_{2} of generically equal circumference in π(𝐂1)\pi(\mathbf{C}_{1}) so that γπ(C1)γπ(C2)Tπ(X,ω)min\gamma_{\pi(C_{1})}^{*}-\gamma_{\pi(C_{2})}^{*}\in T_{\pi(X,\omega)}\mathcal{M}_{min}. Therefore, \mathcal{M} is hh-geminal up to marked points by Corollary 8.5 (2).

9. Proof of Theorem 1.8

This entire section is dedicated to the proof of Theorem 1.8. As mentioned in Remark 1.9, only the forward implication of the claim requires proof.

Suppose therefore that \mathcal{M} is an invariant subvariety of rank rr that consists of genus gg surfaces. Suppose too that, with respect to Lebesgue measure on the unit-area locus of \mathcal{M}, the Kontsevich-Zorich cocycle has 2g2r2g-2r zero Lyapunov exponents. The goal of this section is to show that \mathcal{M} is one of the following: the Eierlegende-Wollmilchsau, the Ornithorynque, or full rank.

When r=1r=1 this result is due to Aulicino-Norton [AN20b], so we will suppose in this section that r>1r>1. By Forni’s criterion (see [For02] and [For11]), \mathcal{M} must have minimal homological dimension. Therefore, by Theorem 1.5, after marking all periodic points (which does not affect the number of zero exponents) \mathcal{M} is hh-geminal. We will suppose in order to deduce a contradiction that \mathcal{M} is not full rank.

By Theorem 1.5, there is a hyperelliptic locus min\mathcal{M}_{min} so that \mathcal{M} is a full locus of covers of min\mathcal{M}_{min}. Since we have supposed that \mathcal{M} is not full rank, the degree of these covers is at least two. Since min\mathcal{M}_{min} is a hyperelliptic locus, min\mathcal{M}_{min} is the locus of holonomy double covers of surfaces in the stratum of quadratic differentials 𝒬(d1,,dn)\mathcal{Q}(d_{1},\ldots,d_{n}) where idi=4\sum_{i}d_{i}=-4. By Eskin-Kontsevich-Zorich [EKZ14, Corollary 1] the sum of positive Lyapunov exponents of min\mathcal{M}_{min} (and indeed for any invariant subvariety therein) is 14diodd1di+2\frac{1}{4}\sum_{d_{i}odd}\frac{1}{d_{i}+2}.

Lemma 9.1.

Let 𝒩\mathcal{N}\subseteq\mathcal{M} be any invariant subvariety. The sum of the positive Lyapunov exponents for the Kontsevich-Zorich cocycle with respect to Lebesgue measure on the unit-area locus of 𝒩\mathcal{N} is 14diodd1di+2\frac{1}{4}\sum_{d_{i}odd}\frac{1}{d_{i}+2}.

Proof.

Since p(T)p(T\mathcal{M}) is complex-symplectic (by Avila-Eskin-Möller [AEM17]) letting WW be the subbundle of H1H_{\mathbb{R}}^{1}\restriction_{\mathcal{M}} that is symplectically orthogonal to p(T)p(T\mathcal{M}), implies that

H1=p(T)W.H_{\mathbb{R}}^{1}\restriction_{\mathcal{M}}=p(T\mathcal{M})\oplus W.

The sum of the positive Lyapunov exponents of p(T)p(T\mathcal{M}) restricted to 𝒩\mathcal{N} is 14diodd1di+2\frac{1}{4}\sum_{d_{i}odd}\frac{1}{d_{i}+2} by Eskin-Kontsevich-Zorich [EKZ14, Corollary 1]. Therefore, it suffices to show that WW restricted to 𝒩\mathcal{N} belongs to the Forni subspace. This will follow from showing that the monodromy of WW over \mathcal{M} belongs to a compact group (this property is then inherited by the restriction of WW to 𝒩\mathcal{N}). This in turn follows by Filip [Fil17, Theorem 1.1]. ∎

Let (mi)(m_{i}) (resp. (mi)(m_{i}^{\prime})) denote the order of the zeros on surfaces in \mathcal{M} (resp. min\mathcal{M}_{min}).

Let (X,ω)(X^{\prime},\omega^{\prime}) be any square-tiled surface in min\mathcal{M}_{min} so that there is a surface (X,ω)(X,\omega) in \mathcal{M} that covers (X,ω)(X^{\prime},\omega^{\prime}) under its \mathcal{M}-optimal map

πopt:(X,ω)(X,ω).\pi_{opt}:(X,\omega)\operatorname{\rightarrow}(X^{\prime},\omega^{\prime}).

Note that (X,ω)(X,\omega) is also square-tiled. Let Γ\Gamma (resp. Γ\Gamma^{\prime}) denote the Veech group of (X,ω)(X,\omega) (resp. (X,ω)(X^{\prime},\omega^{\prime})). Notice that Γ\Gamma is a subgroup of Γ\Gamma^{\prime}. Given an element gjΓg_{j}\Gamma of SL(2,)/Γ\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma, we will let (hij)(h_{ij}) and (wij)(w_{ij}) denote the heights and widths of horizontal cylinders on gj(X,ω)g_{j}\cdot(X,\omega). We will let (hik)(h_{ik}^{\prime}) and (wik)(w_{ik}^{\prime}) denote similar quantities given gkΓg_{k}\Gamma^{\prime} applied to (X,ω)(X^{\prime},\omega^{\prime}). By Eskin-Kontsevich-Zorich [EKZ14, Corollary 8] the sum of the positive Lyapunov exponents over the Teichmüller curve generated by (X,ω)(X,\omega) is the following,

(9.0.1) 112imi(mi+2)mi+1+1|SL(2,)/Γ|gjSL(2,)/Γihijwij.\frac{1}{12}\sum_{i}\frac{m_{i}(m_{i}+2)}{m_{i}+1}+\frac{1}{|\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma|}\sum_{g_{j}\in\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma}\sum_{i}\frac{h_{ij}}{w_{ij}}.

Let dd denote the degree of πopt\pi_{opt}. By definition of an \mathcal{M}-optimal map, the preimage of a cylinder on (X,ω)(X^{\prime},\omega^{\prime}) on (X,ω)(X,\omega) is a single cylinder of the same height and whose circumference is dd times longer. This observation implies the following,

(9.0.2) 1|SL(2,)/Γ|gjSL(2,)/Γihijwij=1|SL(2,)/Γ|1|Γ/Γ|gjΓ/ΓgkSL(2,)/Γihikdwik.\frac{1}{|\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma|}\sum_{g_{j}\in\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma}\sum_{i}\frac{h_{ij}}{w_{ij}}=\frac{1}{|\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma^{\prime}|}\frac{1}{|\Gamma^{\prime}/\Gamma|}\sum_{g_{j}\in\Gamma^{\prime}/\Gamma}\sum_{g_{k}\in\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma^{\prime}}\sum_{i}\frac{h_{ik}^{\prime}}{dw_{ik}^{\prime}}.

Since the right-hand side of Equation (9.0.2) does not depend on jj, we have the following,

(9.0.3) 1|SL(2,)/Γ|gjSL(2,)/Γihijwij=1d|SL(2,)/Γ|gkSL(2,)/Γihikwik.\frac{1}{|\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma|}\sum_{g_{j}\in\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma}\sum_{i}\frac{h_{ij}}{w_{ij}}=\frac{1}{d|\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma^{\prime}|}\sum_{g_{k}\in\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma^{\prime}}\sum_{i}\frac{h_{ik}^{\prime}}{w_{ik}^{\prime}}.

Combining Eskin-Kontsevich-Zorich [EKZ14, Corollary 1] and [EKZ14, Corollary 8] yields,

(9.0.4) 14diodd1di+2=112imi(mi+2)mi+1+1|SL(2,)/Γ|gkSL(2,)/Γihikwik.\frac{1}{4}\sum_{d_{i}odd}\frac{1}{d_{i}+2}=\frac{1}{12}\sum_{i}\frac{m_{i}^{\prime}(m_{i}^{\prime}+2)}{m_{i}^{\prime}+1}+\frac{1}{|\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma^{\prime}|}\sum_{g_{k}\in\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma^{\prime}}\sum_{i}\frac{h_{ik}^{\prime}}{w_{ik}^{\prime}}.

where the final sum is over horizontal cylinders (indexed by ii) on gk(X,ω)g_{k}(X^{\prime},\omega^{\prime}). Combining Equations (9.0.4) and (9.0.3) yields,

(9.0.5) 1|SL(2,)/Γ|gjSL(2,)/Γihijwij=1d(14diodd1di+2112imi(mi+2)mi+1).\frac{1}{|\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma|}\sum_{g_{j}\in\mathrm{SL}\left(2,\mathbb{Z}\right)/\Gamma}\sum_{i}\frac{h_{ij}}{w_{ij}}=\frac{1}{d}\left(\frac{1}{4}\sum_{d_{i}odd}\frac{1}{d_{i}+2}-\frac{1}{12}\sum_{i}\frac{m_{i}^{\prime}(m_{i}^{\prime}+2)}{m_{i}^{\prime}+1}\right).

Substituting Equation (9.0.5) into Equation (9.0.1) and appealing to Lemma 9.1 yields the following,

(9.0.6) 14(11d)diodd1di+2=112(imi(mi+2)mi+11dimi(mi+2)mi+1).\frac{1}{4}\left(1-\frac{1}{d}\right)\sum_{d_{i}odd}\frac{1}{d_{i}+2}=\frac{1}{12}\left(\sum_{i}\frac{m_{i}(m_{i}+2)}{m_{i}+1}-\frac{1}{d}\sum_{i}\frac{m_{i}^{\prime}(m_{i}^{\prime}+2)}{m_{i}^{\prime}+1}\right).

Let gg be the genus of (X,ω)(X,\omega) and gg^{\prime} the genus of (X,ω)(X^{\prime},\omega^{\prime}). Using the trivial observations that 1<mi+2mi+1321<\frac{m_{i}+2}{m_{i}+1}\leq\frac{3}{2} (since mi1m_{i}\geq 1) and that imi=2g2\sum_{i}m_{i}=2g-2 (and that the same relations hold after adding primes), Equation (9.0.6) produces the following inequality,

(9.0.7) 3(11d)diodd1di+2>(2g2)32d(2g2).3\left(1-\frac{1}{d}\right)\sum_{d_{i}odd}\frac{1}{d_{i}+2}>(2g-2)-\frac{3}{2d}(2g^{\prime}-2).

By the Riemann-Hurwitz formula, Equation (9.0.7) becomes,

(9.0.8) 3(11d)diodd1di+2>(d32d)(2g2)+R.3\left(1-\frac{1}{d}\right)\sum_{d_{i}odd}\frac{1}{d_{i}+2}>\left(d-\frac{3}{2d}\right)(2g^{\prime}-2)+R.

where RR is the ramification term, i.e. R=pX(ep1)R=\sum_{p\in X}(e_{p}-1) where epe_{p} is the ramification index of πopt\pi_{opt} at pp. Since \mathcal{M} is hh-geminal of rank at least two and since πopt\pi_{opt} has degree at least two, πopt\pi_{opt} is branched over every regular Weierstrass point except possibly one (by Corollary 6.13). This implies that RP1R\geq P-1 where PP denotes the number of regular Weierstrass points on (X,ω)(X^{\prime},\omega^{\prime}). Since the sum diodd1di+2\sum_{d_{i}odd}\frac{1}{d_{i}+2} can be interpreted as a sum over the Weierstrass points of (X,ω)(X^{\prime},\omega^{\prime}) - where each regular Weierstrass point contributes 11 to the sum and every other Weierstrass point contributes a number bounded above by 13\frac{1}{3} - Equation (9.0.8) implies the following,

(9.0.9) 3(11d)(P+13(2g+2P))>(d32d)(2g2)+(P1).3\left(1-\frac{1}{d}\right)\left(P+\frac{1}{3}\left(2g^{\prime}+2-P\right)\right)>\left(d-\frac{3}{2d}\right)(2g^{\prime}-2)+(P-1).

Simplifying the left hand side gives,

(11d)((2g2)+4+2P)>(d32d)(2g2)+(P1).\left(1-\frac{1}{d}\right)\left(\left(2g^{\prime}-2\right)+4+2P\right)>\left(d-\frac{3}{2d}\right)(2g^{\prime}-2)+(P-1).

Multiplying through by 2d2d yields,

(d1)(2(2g2)+8+4P)>(2d23)(2g2)+2d(P1).\left(d-1\right)\left(2\left(2g^{\prime}-2\right)+8+4P\right)>\left(2d^{2}-3\right)(2g^{\prime}-2)+2d(P-1).

Combining terms produces the following,

8(d1)+4P(d1)2d(P1)>(2d22d1)(2g2).8(d-1)+4P(d-1)-2d(P-1)>\left(2d^{2}-2d-1\right)(2g^{\prime}-2).

So we have,

10d8+(2d4)P>(2d22d1)(2g2).10d-8+(2d-4)P>\left(2d^{2}-2d-1\right)(2g^{\prime}-2).

Since P2g+2=(2g2)+4P\leq 2g^{\prime}+2=(2g^{\prime}-2)+4,

(9.0.10) 18d24>(2d24d+3)(2g2)18d-24>\left(2d^{2}-4d+3\right)(2g^{\prime}-2)

This shows that d4d\leq 4 and that g=2g^{\prime}=2 (notice that g1g^{\prime}\geq 1 and that g1g^{\prime}\neq 1 since then \mathcal{M} would be a locus of torus covers, contradicting the fact that it has rank at least two). Set

Λ:=3(11d)diodd1di+2\Lambda:=3\left(1-\frac{1}{d}\right)\sum_{d_{i}odd}\frac{1}{d_{i}+2}

Since g=2g^{\prime}=2, min\mathcal{M}_{min} is the locus of holonomy double covers of either 𝒬(1,15)\mathcal{Q}(1,-1^{5}) or 𝒬(2,16)\mathcal{Q}(2,-1^{6}), for which P=5P=5 and P=6P=6 respectively. Therefore, Λ=16(11d)\Lambda=16\left(1-\frac{1}{d}\right) when P=5P=5 and Λ=18(11d)\Lambda=18\left(1-\frac{1}{d}\right) when P=6P=6. Since g=2g^{\prime}=2, the inequality P1RP-1\leq R together with Equation (9.0.8) implies the following

(9.0.11) P1R<Λ(2d3d).P-1\leq R<\Lambda-\left(2d-\frac{3}{d}\right).

We will now divide into two cases.

Case 1: P=6P=6.

In this case, Equation (9.0.11) becomes

5R<18(11d)(2d3d).5\leq R<18\left(1-\frac{1}{d}\right)-\left(2d-\frac{3}{d}\right).

Since 2d42\leq d\leq 4, R{5,6}R\in\{5,6\}. Since RR is even, R=6R=6. Since there is branching over at least 55 regular Weierstrass points, there are at least four regular Weierstrass points that are simple branch points, i.e. their preimage contains exactly one ramification point and that point is doubly ramified. If none of the zeros of ω\omega^{\prime} are branch points, then (X,ω)(X,\omega) has at least 2d+42d+4 zeros of order 11. Similarly, if one of the zeros is a branch point then every branch point is simple and so (X,ω)(X,\omega) has 2d+42d+4 zeros of order 11. Equation (9.0.6) implies that

18(11d)(4+2d)323d.18\left(1-\frac{1}{d}\right)\geq(4+2d)\frac{3}{2}-\frac{3}{d}.

This equation is equivalent to

0>6d224d+300>6d^{2}-24d+30

which never holds for dd real, a contradiction.

Case 2: P=5P=5.

In this case, Equation (9.0.11) becomes

4R16(11d)(2d3d).4\leq R\leq 16\left(1-\frac{1}{d}\right)-\left(2d-\frac{3}{d}\right).

Since 2d42\leq d\leq 4, R{4,5}R\in\{4,5\}. Since RR is even, R=4R=4. Since there is branching over at least 44 regular Weierstrass points, the only branch points are 44 regular Weierstrass points, which are simple branch points. This implies that (X,ω)(14,2d)(X,\omega)\in\mathcal{H}\left(1^{4},2^{d}\right) where exponents indicate multiplicity. Equation (9.0.6) then implies that

16(11d)=4(32)+d(83)83d.16\left(1-\frac{1}{d}\right)=4\left(\frac{3}{2}\right)+d\left(\frac{8}{3}\right)-\frac{8}{3d}.

So

8d230d+40=0.8d^{2}-30d+40=0.

However, this equation has no real roots, so we have a contradiction.

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