Moduli of tropical plane curves
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DOI: 10.1186/s40687-014-0018-1
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- Brodsky, S., Joswig, M., Morrison, R. et al. Mathematical Sciences (2015) 2: 4. doi:10.1186/s40687-014-0018-1
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Abstract
We study the moduli space of metric graphs that arise from tropical plane curves. There are far fewer such graphs than tropicalizations of classical plane curves. For fixed genus g, our moduli space is a stacky fan whose cones are indexed by regular unimodular triangulations of Newton polygons with g interior lattice points. It has dimension 2g+1 unless g≤3 or g=7. We compute these spaces explicitly for g≤5.
Introduction
Tropical plane curves C are dual to regular subdivisions of their Newton polygon P. The tropical curve C is smooth if that subdivision is a unimodular triangulation Δ, i.e. it consists of triangles whose only lattice points are its three vertices. The genusg=g(C) is the number of interior lattice points of P. Each bounded edge of C has a well-defined lattice length. The curve C contains a subdivision of a metric graph of genus g with vertices of valency ≥3 as in [5], and this subdivision is unique for g≥2. The underlying graph G is planar and has g distinguished cycles, one for each interior lattice point of P. We call G the skeleton of C. It is the smallest subspace of C to which C admits a deformation retract.
For basics on tropical geometry and further references, the reader is referred to [19,26]. Let \(\mathbb {M}_{g}\) denote the moduli space of metric graphs of genus g. The moduli space \(\mathbb {M}_{g}\) is obtained by gluing together finitely many orthants \(\mathbb {R}_{\geq 0}^{m}\), m≤3g−3, one for each combinatorial type of graph, modulo the identifications corresponding to graph automorphisms. These automorphisms endow the moduli space \(\mathbb {M}_{g}\) with the structure of a stacky fan. We refer to [7,11] for the definition of \(\mathbb {M}_{g}\), combinatorial details, and applications in algebraic geometry. The maximal cones of \(\mathbb {M}_{g}\) correspond to trivalent graphs of genus g. These have 2g−2 vertices and 3g−3 edges, so \(\mathbb {M}_{g}\) is pure of dimension 3g−3. The number of trivalent graphs for g=2,3,…,10 is 2,5,17,71,388,2592,21096,204638,2317172; see [6] and [11, Prop. 2.1].
Fix a (convex) lattice polygon P with \(g = \# (\text {int}(P) \cap \mathbb {Z}^{2})\). Let \(\mathbb {M}_{P}\) be the closure in \(\mathbb {M}_{g}\) of the set of metric graphs that are realized by smooth tropical plane curves with Newton polygon P. For a fixed regular unimodular triangulation Δ of P, let \(\mathbb {M}_{\Delta } \) be the closure of the cone of metric graphs from tropical curves dual to Δ. These curves all have the same skeleton G, and \(\mathbb {M}_{\Delta }\) is a convex polyhedral cone in the orthant \(\mathbb {R}_{\geq 0}^{3g-3}\) of metrics on G. Working modulo automorphisms of G, we identify \(\mathbb {M}_{\Delta }\) with its image in the stacky fan \(\mathbb {M}_{g}\).
Here, P runs over isomorphism classes of lattice polygons with g interior lattice points. The number of such classes is finite by Proposition 2.3.
This paper presents a computational study of the moduli spaces \(\mathbb {M}_{g}^{\text {planar}}\). We construct the decompositions in Equations 2 and 3, explicitly. Our first result reveals the dimensions:
Theorem1.1.
In each case, the cone \(\,\mathbb {M}_{\Delta }\) of honeycomb curves supported on P attains this dimension.
Honeycomb curves are introduced in Section ‘Honeycombs’. That section furnishes the proof of Theorem 1.1. The connection between tropical and classical curves will be explained in Section ‘Algebraic geometry’. The number 2g+1 in Equation 4 is the dimension of the classical moduli space of trigonal curves of genus g, whose tropicalization is related to our stacky fan \(\mathbb {M}_{g}^{\text {planar}}\). Our primary source for the relevant material from algebraic geometry is the article [10] by Castryck and Voight. Our paper can be seen as a refined combinatorial extension of theirs. For related recent work that incorporates also immersions of tropical curves, see Cartwright et al. [8].
We begin in Section ‘Combinatorics and computations’ with an introduction to the relevant background from geometric combinatorics. The objects in Equations 1 to 3 are carefully defined, and we explain our algorithms for computing these explicitly, using the software packages TOPCOM [28] and polymake [2,16].
Our main results in this paper are Theorems 5.1, 6.3, 7.1, and 8.5. These concern g=3,4,5, and they are presented in Sections ‘Genus three’ through ‘Genus five and beyond’. The proofs of these theorems rely on the computer calculations that are described in Section ‘Combinatorics and computations’. In Section ‘Genus three’, we study plane quartics as in Figure 1. Their Newton polygon is the size four triangle T_{4}. This models non-hyperelliptic genus 3 curves in their canonical embedding. We compute the space \(\mathbb {M}_{T_{4}}\). Four of the five trivalent graphs of genus 3 are realized by smooth tropical plane curves.
In Section ‘Hyperelliptic curves’, we show that all metric graphs arising from hyperelliptic polygons of given genus arise from a single polygon, namely, the hyperelliptic triangle. We determine the space \(\mathbb {M}^{\text {planar}}_{3,\text {hyp}}\), which together with \(\mathbb {M}_{T_{4}}\) gives \(\mathbb {M}^{\text {planar}}_{3}\). Section ‘Genus four’ deals with curves of genus g=4. Here, Equation 3 is a union over four polygons, and precisely 13 of the 17 trivalent graphs G are realized in Equation 2. The dimensions of the cones \(\mathbb {M}_{P,G}\) range between 4 and 9. In Section ‘Genus five and beyond’, we study curves of genus g=5. Here, 38 of the 71 trivalent graphs are realizable. Some others are ruled out by the sprawling condition in Proposition 8.3. We end with a brief discussion of g≥6 and some open questions.
Combinatorics and computations
The methodology of this paper is computations in geometric combinatorics. In this section, we fix notation, supply definitions, present algorithms, and give some core results. For additional background, the reader is referred to the book by De Loera, Rambau, and Santos [13].
The tropical curve C defined by this min-plus polynomial consists of all points \((x,y) \in \mathbb {R}^{2}\) for which the minimum among the quantities i·x+j·y+h(i,j) is attained at least twice as (i,j) runs over A. The curve C is dual to the regular subdivisionΔ of A defined by h. To construct Δ, we lift each lattice point a∈A to the height h(a) then take the lower convex hull of the lifted points in \(\mathbb {R}^{3}\). Finally, we project back to \(\mathbb {R}^{2}\) by omitting the height. The maximal cells are the images of the facets of the lower convex hull under the projection. The set of all height functions h which induce the same subdivision Δ is a relatively open polyhedral cone in \(\mathbb {R}^{A}\). This is called the secondary cone and is denoted Σ(Δ). The collection of all secondary cones Σ(Δ) is a complete polyhedral fan in \(\mathbb {R}^{A}\), the secondary fan of A.
A subdivision Δ is a triangulation if all maximal cells are triangles. The maximal cones in the secondary fan Σ(Δ) correspond to the regular triangulations Δ of A. Such a cone is the product of a pointed cone of dimension #A−3 and a 3-dimensional subspace of \(\mathbb {R}^{A}\).
This is a linear inequality for \(h \in \mathbb {R}^{A}\). It can be viewed as a ‘flip condition’, determining which of the two diagonals of a quadrilateral are in the subdivision. We have one such inequality for each interior edge bc of Δ. The set of solutions to these linear inequalities is the secondary cone Σ(Δ). From this, it follows that the lineality space Σ(Δ)∩−Σ(Δ) of the secondary cone is 3-dimensional. It is the space Lin(A) of functions \(h \in \mathbb {R}^{A}\) that are restrictions of affine-linear functions on \(\mathbb {R}^{2}\). We usually identify Σ(A) with its image in \(\mathbb {R}^{A} /\text {Lin}(A)\), which is a pointed cone of dimension #A−3. That pointed cone has finitely many rays, and we represent these by vectors in \(\mathbb {R}^{A}\).
The map λ takes h and outputs the vector whose bc coordinate equals Equation 5. This determinant is nonnegative: it is precisely the length of the edge of the tropical curve C that is dual to bc. Hence, λ(h) is the vector whose coordinates are the lengths of the bounded edges of C, and κ(λ(h)) is the vector whose 3g−3 coordinates are the lengths of the edges of the skeleton G.
Remark2.1.
The (lattice) length of an edge of C with slope p/q, where p,q are relatively prime integers, is the Euclidean length of the edge divided by \(\sqrt {p^{2}+q^{2}}\). This lets one quickly read off the lengths from a picture of C without having to compute the determinant (Equation 5).
Our discussion implies the following result on the cone of metric graphs arising from Δ:
Proposition2.2.
The cone \(\,\mathbb {M}_{\Delta }\) is the image of the secondary cone Σ(Δ) under κ∘λ.
- 1.
compute all regular unimodular triangulations of \(A = P \cap \mathbb {Z}^{2}\) up to symmetry;
- 2.
sort the triangulations into buckets, one for each trivalent graph G of genus g;
- 3.
for each triangulation Δ with skeleton G, compute its secondary cone \(\Sigma (\Delta) \subset \mathbb {R}^{A}\);
- 4.
for each secondary cone Σ(Δ), compute its image \(\mathbb {M}_{\Delta }\) in the moduli space \(\mathbb {M}_{g}\) via Equation 7;
- 5.
merge the results to get the fans \(\mathbb {M}_{P,G} \subset \mathbb {R}^{3g-3}\) in (1) and the moduli space \(\mathbb {M}_{P}\) in Equation 2.
Step 1 is based on computing the secondary fan of A. There are two different approaches to doing this. The first, more direct, method is implemented in Gfan [20]. It starts out with one regular triangulation of Δ, e.g. a placing triangulation arising from a fixed ordering of A. This comes with an inequality description for Σ(Δ), as in Equation 5. From this, Gfan computes the rays and the facets of Σ(Δ). Then, Gfan proceeds to an adjacent secondary cone Σ(Δ^{′}) by producing a new height function from traversing a facet of Σ(Δ). Iterating this process results in a breadth-first search through the edge graph of the secondary polytope of A.
The second method starts out the same. But it passes from Δ to a neighboring triangulation Δ^{′} that need not be regular. It simply performs a purely combinatorial restructuring known as a bistellar flip. The resulting breadth-first search is implemented in TOPCOM [28]. Note that a bistellar flip corresponds to inverting the sign in one of the inequalities in Equation 5.
Neither algorithm is generally superior to the other, and sometimes it is difficult to predict which one will perform better. The flip algorithm may suffer from wasting time by also computing non-regular triangulations, while the polyhedral algorithm is genuinely costly since it employs exact rational arithmetic. The flip algorithm also uses exact coordinates but only in a preprocessing step which encodes the point configuration as an oriented matroid. Both algorithms can be modified to enumerate all regular unimodular triangulations up to symmetry only. For our particular planar instances, we found TOPCOM to be more powerful.
We start Step 2 by computing the dual graph of a given Δ. The nodes are the triangles and the edges record incidence. Hence, each node has degree 1, 2, or 3. We then recursively delete the nodes of degree 1. Next, we recursively contract edges which are incident with a node of degree 2. The resulting trivalent graph G is the skeleton of Δ. It often has loops and multiple edges. In this process, we keep track of the history of all deletions and contractions.
Steps 3 and 4 are carried out using polymake [16]. Here, the buckets or even the individual triangulations can be treated in parallel. The secondary cone Σ(Δ) is defined in \(\mathbb {R}^{A}\) by the linear inequalities λ(h)≥0 in Equation 5. From this, we compute the facets and rays of Σ(Δ). This is essentially a convex hull computation. In order to get unique rays modulo Lin(A), we fix h=0 on the three vertices of one particular triangle. Since the cones are rather small, the choice of the convex hull algorithm does not matter much. For details on state-of-the-art convex hull computations and an up-to-date description of the polymake system, see [2].
For Step 4, we apply the linear map κ∘λ to all rays of the secondary cone Σ(Δ). Their images are vectors in \(\mathbb {R}^{3g-3}\) that span the moduli cone \(\mathbb {M}_{\Delta } = (\kappa \circ \lambda)(\Sigma (\Delta))\). Via a convex hull computation as above, we compute all the rays and facets of \(\mathbb {M}_{\Delta } \).
The cones \(\mathbb {M}_{\Delta }\) are generally not full-dimensional in \(\mathbb {R}^{3g-3}\). The points in the relative interior are images of interior points of Σ(Δ). Only these represent smooth tropical curves. However, it can happen that another cone \(\mathbb {M}_{\Delta '}\) is a face of \(\mathbb {M}_{\Delta }\). In that case, the metric graphs in the relative interior of that face are also realizable by smooth tropical curves.
Step 5 has not been fully automatized yet, but we carry it out in a case-by-case manner. This will be described in detail for curves of genus g=3 in Sections ‘Genus three’ and ‘Hyperelliptic curves’.
We now come to the question of what lattice polygons P should be the input for Step 1. Our point of departure towards answering that question is the following finiteness result.
Proposition2.3.
For every fixed genus g≥1, there are only finitely many lattice polygons P with g interior lattice points, up to integer affine isomorphisms in \(\mathbb {Z}^{2}\).
Proof and Discussion.
Scott [29] proved that \(\#\left (\partial P\cap \mathbb {Z}^{2}\right) \leq 2g+7\), and this bound is sharp. This means that the number of interior lattice points yields a bound on the total number of lattice points in P. This result was generalized to arbitrary dimensions by Hensley [18]. Lagarias and Ziegler [24] improved Hensley’s bound and further observed that there are only finitely many lattice polytopes with a given total number of lattice points, up to unimodular equivalence [24, Theorem 2]. Castryck [9] gave an algorithm for finding all lattice polygons of a given genus, along with the number of lattice polygons for each genus up to 30. We remark that the assumption g≥1 is essential, as there are lattice triangles of arbitrarily large area and without any interior lattice point.
Proposition 2.3 ensures that the union in Equation 3 is finite. However, from the full list of polygons P with g interior lattice points, only very few will be needed to construct \(\mathbb {M}_{g}^{\text {planar}}\). To show this, and to illustrate the concepts seen so far, we now discuss our spaces for g≤2.
Example2.4.
All inclusions in Equation 12 are equalities for this particular choice of (P,Δ).
Example2.5.
In Section ‘Hyperelliptic curves’, we extend this analysis to hyperelliptic curves of genus g≥3. See Figure three in [11]. The graphs G_{1} and G_{2} represent the chains for g=2. For information on hyperelliptic skeletons, see [12].
With g=1,2 out of the way, we now assume g≥3. We follow the approach of Castryck and Voight [10] in constructing polygons P that suffice for the union (Equation 3). We write P_{int} for the convex hull of the g interior lattice points of P. This is the interior hull of P. The relationship between the polygons P and P_{int} is studied in polyhedral adjunction theory [14].
Lemma2.6.
Let P⊆Q be lattice polygons with P_{int}=Q_{int}. Then \(\mathbb {M}_{P}\) is contained in \(\mathbb {M}_{Q}\).
Proof.
By [13], Lemma 4.3.5, a triangulation Δ of any point set S can be extended to a triangulation Δ^{′} of any superset S^{′}⊃S. If Δ is regular, then so is Δ^{′}. Applying this result to a regular triangulation of P which uses all lattice points in P yields a regular triangulation of Q which uses all lattice points in Q. The triangulations of a lattice polygon which use all lattice points are precisely the unimodular ones (This is a special property of planar triangulations.). We conclude that every tropical curve C dual to Δ is contained in a curve C^{′} dual to Δ^{′}, except for unbounded edges of C. The skeleton and its possible metrics remain unchanged, since P_{int}=Q_{int}. We therefore have the equality of moduli cones \(\mathbb {M}_{\Delta } = \mathbb {M}_{\Delta '}\). The unions for P and Q in Equation 2 show that \(\mathbb {M}_{P} \subseteq \mathbb {M}_{Q}\).
This lemma shows that we only need to consider maximal polygons, i.e. those P that are maximal with respect to inclusion for fixed P_{int}. If P_{int} is 2-dimensional, then this determines P uniquely. Namely, suppose that \(P_{\text {int}} = \{(x,y) \in \mathbb {R}^{2} \,:\, a_{i} x + b_{i} y \leq c_{i} \,\text {for} \,\, i = 1,2,\ldots,s \}\), where \(\gcd (a_{i},b_{i},c_{i})=1\) for all i. Then, P is the polygon \(\,\{(x,y) \in \mathbb {R}^{2} \,:\, a_{i} x + b_{i} y \leq c_{i}+1 \,\,\text {for} \,\, i = 1,2,\ldots,s \}\). If P is a lattice polygon, then it is a maximal lattice polygon. However, it can happen that P has non-integral vertices. In that case, the given P_{int} is not the interior of any lattice polygon.
The maximal polygon P is not uniquely determined by P_{int} when P_{int} is a line segment. For each g≥2, there are g+2 distinct hyperelliptic trapezoids to be considered. We shall see in Theorem 6.1 that for our purposes, it suffices to use the triangle conv{(0,0),(0,2),(2g+2,0)}.
Here is the list of all maximal polygons we use as input for the pipeline described above.
Proposition2.7.
The notation we use for polygons is as follows. We write \(Q^{(g)}_{i}\) for maximal polygons of genus g, but we also use a systematic notation for families of polygons, including the trianglesT_{d}= conv{(0,0),(0,d),(d,0)} and the rectanglesR_{d,e}= conv{(0,0),(d,0),(0,e),(d,e)}.
However, neither of these two triangles arises as P_{int} for any lattice polygon P. For each genus g, we construct the stacky fans \(\mathbb {M}_{g}^{\text {planar}}\) by computing each of the spaces \(\mathbb {M}_{Q^{(g)}_{i}}\) and then subdividing their union appropriately. This is then augmented in Section ‘Hyperelliptic curves’ by the spaces \(\mathbb {M}_{P}\) where P_{int} is not 2-dimensional, but is instead a line segment.
Algebraic geometry
Both spaces have dimension 3g−3 for g≥2. The map (Equation 10) is referred to as ‘naive set-theoretic tropicalization’ by Abramovich, Caporaso, and Payne [1]. We point to that article and its bibliography for the proper moduli-theoretic settings for our combinatorial objects.
Consider plane curves defined by a Laurent polynomial \(f=\sum _{(i,j)\in \mathbb {Z}^{2}}c_{\textit {ij}}x^{i}y^{j}\in K\left [x^{\pm },y^{\pm }\right ]\) with Newton polygon P. For τ a face of P, we let \(f|_{\tau }=\sum _{(i,j)\in \tau }c_{\textit {ij}}x^{i}y^{j}\) and say that f is non-degenerate if f|_{τ} has no singularities in (K^{∗})^{2} for any face τ of P. Non-degenerate polynomials are useful for studying many subjects in algebraic geometry, including singularity theory [23], the theory of sparse resultants [17], and topology of real algebraic curves [27].
This moduli space was introduced and studied by Castryck and Voight in [10]. That article was a primary source of inspiration for our study. In particular, [10], Theorem 2.1 determined the dimensions of the spaces \(\mathcal {M}_{g}^{\text {planar}}\) for all g. Whenever we speak about the ‘dimension expected from classical algebraic geometry’, as we do in Theorem 1.1, this refers to the formulas for \(\dim (\mathcal {M}_{P})\) and \(\dim \left (\mathcal {M}_{g}^{\text {planar}}\right)\) that were derived by Castryck and Voight.
By the Structure Theorem for Tropical Varieties [26, §3.3], these dimensions are preserved under the tropicalization map (Equation 10). The images \( \operatorname{trop}\left({\mathcal{M}}_P\right) \) and \( \operatorname{trop}\left(\underset{g}{\overset{\mathrm{planar}}{\mathcal{M}}}\right) \) are stacky fans that live inside \(\mathbb {M}_{g} = {\text {trop}}(\mathcal {M}_{g})\) and have the expected dimension. Furthermore, all maximal cones in \({\text {trop}}(\mathcal {M}_{P})\) have the same dimension since \(\mathcal {M}_{P}\) is irreducible (in fact, unirational).
For g≥3, the inclusions between the second row and the third row are strict, by a wide margin. This is the distinction between tropicalizations of plane curves and tropical plane curves. One main objective of this paper is to understand how the latter sit inside the former.
This is the stacky fan in [11], Figure one. The space \(\mathbb {M}_{T_{4}}=\mathbb {M}^{\text {planar}}_{3,\text {nonhyp}}\) of tropical plane quartics is also 6-dimensional, but it is smaller. It fills up less than 30% of the curves in \(\mathbb {M}_{3}\); see Corollary 5.2. Most metric graphs of genus 3 do not come from plane quartics.
For g=4, the canonical curve is a complete intersection of a quadric surface with a cubic surface. If the quadric is smooth, then we get a curve of bidegree (3,3) in \(\mathbb {P}^{1} \times \mathbb {P}^{1}\). This leads to the Newton polygon R_{3,3}= conv{(0,0),(3,0),(0,3),(3,3)}. Singular surfaces lead to families of genus 4 curves of codimensions 1 and 2 that are supported on two other polygons [10, §6]. As we shall see in Theorem 7.1, \(\mathbb {M}_{P}\) has the expected dimension for each of the three polygons P. Furthermore, \(\mathbb {M}^{\text {planar}}_{4}\) is strictly contained in \( \operatorname{trop}\left(\underset{4}{\overset{\mathrm{planar}}{\mathcal{M}}}\right) \). Detailed computations that reveal our spaces for g=3,4,5 are presented in Sections ‘Genus three’, ‘Hyperelliptic curves’, ‘Genus four’, and ‘Genus five and beyond’.
We close this section by returning once more to classical algebraic geometry. Let \(\mathcal {T}_{g}\) denote the trigonal locus in the moduli space \(\mathcal {M}_{g}\). It is well known that \(\mathcal {T}_{g}\) is an irreducible subvariety of dimension 2g+1 when g≥5. For a proof, see [15, Proposition 2.3]. A recent theorem of Ma [25] states that \(\mathcal {T}_{g}\) is a rational variety for all g.
We note that Ma’s work, as well as the classical approaches to trigonal curves, are based on the fact that canonical trigonal curves of genus g are realized by a certain special polygon P. This is either the rectangle in Equation 17 or the trapezoid in Equation 18. These polygons appear in [10], Section 12, where they are used to argue that \(\mathcal {T}_{g}\) defines one of the irreducible components of \(\mathcal {M}_{g}^{\text {planar}}\), namely, \(\mathcal {M}_{P}\). The same P appear in the next section, where they serve to prove one inequality on the dimension in Theorem 1.1. The combinatorial moduli space \(\mathbb {M}_{P}\) is full-dimensional in the tropicalization of the trigonal locus. The latter space, denoted \( \operatorname{trop}\left({\mathcal{T}}_g\right) \), is contained in the space of trigonal metric graphs, by Baker’s Specialization Lemma [3, §2].
In general, \(\mathcal {M}_{g}^{\text {planar}}\) has many irreducible components other than the trigonal locus \(\mathcal {T}_{g}\). As a consequence, there are many skeleta in \(\mathbb {M}_{g}^{\text {planar}}\) that are not trigonal in the sense of metric graph theory. This is seen clearly in the top dimension for g=7, where \(\dim (\mathcal {T}_{7}) = 15\) but \(\dim \left (\mathcal {M}_{7}^{\text {planar}}\right) = 16\). The number 16 comes from the family of trinodal sextics in [10, §12].
Honeycombs
We now prove Theorem 1.1. This will be done using the special family of honeycomb curves. The material in this section is purely combinatorial. No algebraic geometry will be required.
The honeycomb triangulationΔ subdivides H_{a,b,c,d} into 2ad+2bd−(a^{2}+b^{2}+c^{2}+d^{2}) unit triangles.
If P=H_{a,b,c,d}, then its interior \( {P}_{\operatorname{int}} \) is a honeycomb polygon as well. Indeed, a translate of \(P_{\text{int}}\) can be obtained from P by decreasing the values of a,b,c,d by an appropriate amount.
Example4.1.
Let P=H_{5,4,2,5}. Note that \( {P}_{\operatorname{int}}={H}_{3,3,1,2}+\left(1,1\right) \). The honeycomb triangulation Δ of P is illustrated in Figure 3, together with a dual tropical curve and its skeleton. The bounded edge lengths in the tropical curve are labelled a through w. These lengths induce the edge lengths on the skeleton, via the formulas α=a+b+c+d, β=e+f, γ=g+h+i+j, δ=k+l+m, and ε=n+o+p. This is the map \(\kappa : \mathbb {R}^{23} \rightarrow \mathbb {R}^{12}\) in Equation 6.
The number \(\text {dim}(\mathbb {M}_{\Delta }) = 11\) is explained by the following lemma.
Lemma4.2.
Proof.
The honeycomb graph G consists of \( g=\#\left({P}_{\operatorname{int}}\cap {\mathbb{Z}}^2\right) \) hexagons. The hexagons associated with lattice points on the boundary of \( {P}_{\operatorname{int}} \) have vertices that are 2-valent in G. Such 2-valent vertices get removed, so these boundary hexagons become cycles with fewer than six edges. In the orthant \(\mathbb {R}_{\geq 0}^{3g-3}\) of all metrics on G, we consider the subcone of metrics \(\mathbb {M}_{\Delta }\) that arise from Δ. This is the image under κ of the transformed secondary cone λ(Σ(Δ)).
The cone λ(Σ(Δ)) is defined in \(\mathbb {R}^{E}_{\geq 0}\) by 2g linearly independent linear equations, namely, two per hexagon. These state that the sum of the lengths of any two adjacent edges equals that of the opposite sum. For instance, in Example 4.1, each of the five hexagons contributes two linear equations, listed in the columns of Equation 15. These equations can be chosen to have distinct leading terms, underlined in Equation 15. In particular, they are linearly independent.
two linear equations for each lattice point in the interior of \( {P}_{\operatorname{int}} \);
one linear equation for each lattice point in the relative interior of an edge of \( {P}_{\operatorname{int}} \);
no linear inequality from the vertices of \( {P}_{\operatorname{int}} \).
That these equations are independent follows from the triangular structure, as in Equation 15. Inside the linear space defined by these equations, the moduli cone \(\mathbb {M}_{\Delta }\) is defined by various linear inequalities all of which, are strict when the graph G comes from a tropical curve C in the interior of Σ(Δ).
Subtracting this codimension from 3g−3, we obtain the desired formula.
Proof of Theorem 1.1.
For the classical moduli space \(\mathcal {M}_{g}^{\text {planar}}\), the formula in Equation 4 was proved in [10]. That dimension is preserved under tropicalization. The inclusion of \(\mathbb {M}_{g}^{\text {planar}}\) in \( \operatorname{trop}\left(\underset{g}{\overset{\mathrm{planar}}{\mathcal{M}}}\right) \), in Equation 12, implies that the right-hand side in Equation 4 is an upper bound on \(\dim \left (\mathbb {M}_{g}^{\text {planar}}\right)\).
All g=2h+1 lattice points of this polygon lie on its boundary, and again \({\dim }(\mathbb {M}_{\Delta }) = 2g+1\).
For all g≥4 with g≠7, this matches the upper bound obtained from [10]. We conclude that \(\,\dim (\mathbb {M}_{P}) = \dim (\mathbb {M}_{g}) = 2g+1\,\) holds in all of these cases. For g=7, we take P=H_{4,4,2,6}. Then, \( {P}_{\operatorname{int}} \) is a hexagon with g=7 lattice points. From Lemma 4.2, we find dim(M_{Δ})=7+6+6−3=16, so this matches the upper bound. Finally, for g=3, we will see \(\text {dim}(M_{T_{4}}) = 6\) in Section ‘Genus three’. The case g=2 follows from the discussion in Example 2.5.
There are two special families of honeycomb curves: those arising from the triangles T_{d} for d≥4 and rectangles R_{d,e} for d,e≥3. The triangle T_{d} corresponds to curves of degree d in the projective plane \(\mathbb {P}^{2}\). Their genus is g=(d−1)(d−2)/2. The case d=4,g=3 will be our topic in Section ‘Genus three’. The rectangle R_{d,e} corresponds to curves of bidegree (d,e) in \(\mathbb {P}^{1} \times \mathbb {P}^{1}\). Their genus is g=(d−1)(e−1). The case d=e=3,g=4 appears in Section ‘Genus four’.
Proposition4.3.
In particular, the honeycomb triangulation defines a cone \(\mathbb {M}_{\Delta }\) of this maximal dimension.
Proof.
Subtracting from \(3g-3 = \dim (\mathbb {M}_{g})\), we get the desired formulas for \(\dim (\mathbb {M}_{P})\).
The above dimensions are those expected from algebraic geometry. Plane curves with Newton polygon T_{d} form a projective space of dimension \(\frac {1}{2}(d+2)(d+1)-1\) on which the 8-dimensional group PGL(3) acts effectively, while those with R_{d,e} form a space of dimension (d+1)(e+1)−1 on which the 6-dimensional group PGL(2)^{2} acts effectively. In each case, \(\dim (\mathcal {M}_{P})\) equals the dimension of the family of all curves minus the dimension of the group.
Genus three
Just like in classical algebraic geometry, \(\text {dim}\left (\mathbb {M}_{T_{4}}\right) = 6\) and \(\text {dim}\left (\mathbb {M}^{\text {planar}}_{3,\text {hyp}}\right) = 5\).
Although \(\mathbb {M}_{T_{4}}\) has dimension 6, it is not pure due to the realizable metrics on (111). It also misses one of the five cones in \(\mathbb {M}_{3}\): the graph (303) cannot be realized in \(\mathbb {R}^{2}\) by Proposition 8.3. The restriction of \(\mathbb {M}_{T_{4}}\) to each of the other cones is given by a finite union of convex polyhedral subcones, characterized by the following piecewise-linear formulas:
Theorem5.1.
- (000) is realizable if and only if max{x,y}≤u, max{x,z}≤v and max{y,z}≤w, where
at most two of the inequalities can be equalities, and
if two are equalities, then either x,y,z are distinct and the edge (among u,v,w) that connects the shortest two of x,y,z attains equality, or max{x,y,z} is attained exactly twice, and the edge connecting those two longest does not attain equality.
(020) is realizable if and only if v≤u, y≤z, and w+ max{v,y}≤x, and if the last inequality is an equality, then: v=u implies v<y<z, and y=z implies y<v<u.
- (111) is realizable if and only if w<x and$$\begin{array}{*{20}l} &\hspace*{24pt}(\,v+w = x \hbox{ and } v<u\,) \ \, \hbox{or}\ \, (\,v+w< x\leq v+3w \hbox{ and } v\leq u\,) \hbox{ or } \\ &\hspace*{65pt} (\,v+3w < x\leq v+4w \hbox{ and } v\leq u\leq 3v/2\,) \hbox{ or } \\ \!\! &(\,v+3w < x\leq v+4w \hbox{ and } 2v=u\,)\ \, \hbox{or}\ \, (\,v+4w< x\leq v+5w \hbox{ and } v=u\,). \end{array} $$(20)
(212) is realizable if and only if w<x≤2w.
To understand the qualifier ‘up to symmetry’ in Theorem 5.1, it is worthwhile to read off the automorphisms from the graphs in Figure 4. The graph (000) is the complete graph on four nodes. Its automorphism group is the symmetric group of order 24. The automorphism group of the graph (020) is generated by the three transpositions (uv), (yz), (wx) and the double transposition (uy)(vz). Its order is 16. The automorphism group of the graph (111) has order 4, and it is generated by (uv) and (wx). The automorphism group of the graph (212) is generated by (uz)(vy) and (wx) and has order 4. The automorphism group of the graph (303) is the symmetric group of order 6. Each of the five graphs contributes an orthant \(\mathbb {R}_{\geq 0}^{6}\) modulo the action of that symmetry group to the stacky fan \(\mathbb {M}_{3}\).
Proof of Theorem 5.1.
Dimensions of the 1,278 moduli cones\(\mathbb {M}_{\Delta }\) within\(\mathbb {M}_{T_{4}}\)
G∖dim | 3 | 4 | 5 | 6 | #Δ’s |
---|---|---|---|---|---|
(000) | 18 | 142 | 269 | 144 | 573 |
(020) | 59 | 216 | 175 | 450 | |
(111) | 10 | 120 | 95 | 225 | |
(212) | 15 | 15 | 30 | ||
Total | 18 | 211 | 620 | 429 | 1,278 |
For each of the 1,278 regular triangulations Δ, we checked that the inequalities stated in Theorem 5.1 are valid on the cone \(\,\mathbb {M}_{\Delta } = (\kappa \circ \lambda)(\Sigma (\Delta))\). This proves that the dense realizable part of \(\mathbb {M}_{T_{4}}\) is contained in the polyhedral space described by our constraints.
For the converse direction, we need to go through the four cases and construct a planar tropical realization of each metric graph that satisfies our constraints. We shall now do this.
There are several lower dimensional collections of graphs that we must show are achievable:
(i) y<x=u, max{x,z}<v, max{y,z}<w; (dim=5)
(ii) y=x=u, max{x,z}<v, max{y,z}<w; (dim=4)
(iii) z<y<x<v, u=x, w=y; (dim=4)
(iv) z<y<x<u, v=x, w=y; (dim=4)
(v) z<y=x=v=w<u. (dim=3)
(i) v<u, y<z, w+ max{v,y}=x; (dim=5)
(ii) u=v, y<z, w+ max{v,y}<x; (dim=5)
(iii) u=v, y=z, w+ max{v,y}<x; (dim=4)
(iv) u=v, v<y<z, w+ max{v,y}=x. (dim=4)
Type (111) is the most complicated. We begin by realizing the metric graphs that lie in \(\text {int}(\mathbb {M}_{T_{4},(111)})\). These arise from the second and third cases in the disjunction (Equation 20).
(i) v+w<x<v+5w, v=u; (dim=5)
(ii) v+w<x<v+4w, 2v=u; (dim=5)
(iii) v+w=x, v<u; (dim=5)
(iv) x=v+3w, v<u; (dim=5)
(v) x=v+4w, v<u≤3v/2; (dim=5)
(vi) x=v+5w, v=u; (dim=4)
(vii) x=v+4w, 2v=u. (dim=4)
The space \(\mathbb {M}_{T_{4}}\) is not pure dimensional because of the graphs (111) with u=v and v+4w<x<v+5w. These appear in the 5-dimensional \(\mathbb {M}_{\Delta }\) where Δ is the leftmost triangulation in Figure 10, but \(\mathbb {M}_{\Delta }\) is not contained in the boundary of any 6-dimensional \(\mathbb {M}_{\Delta '}\).
We close this section by suggesting an answer to the following question: What is the probability that a random metric graph of genus 3 can be realized by a tropical plane quartic?
This ratio is a rational number, which we computed from our data in Theorem 5.1.
Corollary5.2.
The rational number in (21) is 31/105. This means that, in the measure specified above, about 29.5% of all metric graphs of genus 3 come from tropical plane quartics.
Proof and Explanation.
The graph (303) is not realizable, since none of the 1,278 regular unimodular triangulations of the triangle T_{4} has this type. So, its probability is zero. For the other four trivalent graphs in Figure 4, we compute the volume of the realizable edge lengths, using the inequalities in Theorem 5.1. The result of our computations is the table
The probability that a uniformly sampled random point in the 5-simplex satisfies equation 22 is equal to 8/15. The desired probability (Equation 21) is the average of the five numbers in the table.
Notice that asking for those probabilities only makes sense since the dimension of the moduli space agrees with the number of skeleton edges. In view of Equation 4, this occurs for the three genera g=2,3,4. For g≥5, the number of skeleton edges exceeds the dimension of the moduli space. Hence, in this case, the probability that a random metric graph can be realized by a tropical plane curve vanishes a priori. For g=2, that probability is one; see Example 2.5. For g=4, that probability is less than 0.5% by Corollary 7.2 below.
Hyperelliptic curves
This finiteness property makes a computation of \(\mathbb {M}^{\text {planar}}_{g, \text {hyp}}\) feasible: compute \(\mathbb {M}_{E_{k}^{(g)}}\) for all k, and take the union. By [21, Proposition 3.4], all triangulations of hyperelliptic polygons are regular, so we need not worry about non-regular triangulations arising in the TOPCOM computations described in Section ‘Combinatorics and computations’. We next show that it suffices to consider the triangle:
Theorem6.1.
The equality holds even before taking closures of the spaces of realizable graphs. The spaces on the left-hand side and right-hand side of the inclusion in Equation 23 both have dimension 2g−1.
Before proving our theorem, we define \(\mathbb {M}_{g}^{\text {chain}}\). This space contains all metric graphs that arise from triangulating hyperelliptic polygons. Start with a line segment on g−1 nodes where the g−2 edges have arbitrary non-negative lengths. Double each edge so that the resulting parallel edges have the same length and attach two loops of arbitrary lengths at the endpoints. Now, each of the g−1 nodes is 4-valent. There are two possible ways to split each node into two nodes connected by an edge of arbitrary length. Any metric graph arising from this procedure is called a chain of genus g. Although there are 2^{g−1} possible choices in this procedure, some give isomorphic graphs. There are 2^{g−2}+2^{⌊(g−2)/2⌋} combinatorial types of chains of genus g. In genus 3, the chains are (020), (111), and (212) in Figure 4; and in genus 4, they are (020), (021), (111), (122), (202), and (223) in Section ‘Genus four’.
By construction, there are 2g−1 degrees of freedom for the edge lengths in a chain of genus g, so each such chain defines an orthant \(\mathbb {R}_{\geq 0}^{2g-1}\). We write \(\mathbb {M}^{\text {chain}}_{g}\) for the stacky subfan of \(\mathbb {M}_{g}\) consisting of all chains. Note that \(\mathbb {M}_{g}^{\text {chain}}\) is strictly contained in the space \(\mathbb {M}^{\text {hyp}}_{g}\) of all hyperelliptic metric graphs, seen in [12]. Hyperelliptic graphs arise by the same construction from any tree with g−1 nodes, whereas for chains that tree must be a line segment.
The main claim in Theorem 6.1 is that any metric graph arising from a maximal hyperelliptic polygon \(E_{k}^{(g)}\) also arises from the hyperelliptic triangle \(E^{(g)}_{g+2}\). Given a triangulation Δ of \(E_{k}^{(g)}\), our proof constructs a triangulation Δ^{′} of \(E^{(g)}_{g+2}\) that gives rise to the same collection of metric graphs, so that \(\mathbb {M}_{\Delta }=\mathbb {M}_{\Delta '}\), with equality holding even before taking closures. Before our proof, we illustrate this construction with the following example.
Example6.2.
Also pictured in Figure 13 is a triangulation Δ^{′} of \(E^{(3)}_{5}\). The skeleton Γ^{′} arising from Δ^{′} has the same combinatorial type as Γ, and the slopes emanating from the vertical edges have the same differences as in Γ. Combined with similar boundary behavior, this shows that Γ and Γ^{′} have the exact same achievable metrics. In other words, \(\mathbb {M}_{\Delta }=\mathbb {M}_{\Delta '}\), with equality even before taking closures of the realizable graphs.
Next, we add edges connecting the interior lattice points to the lower edge of the triangle. We will ensure that the outgoing slopes from the vertical edges in the Γ^{′} have the same difference as in Γ. For i=1,2,3, we connect (i,1) to all points between (2i+a_{i},0) and (2i+b_{i},0) where a_{i} is the difference between the reciprocals of the slopes of the leftmost edges from (i,1) to the upper and lower edges of R_{4,2} in Δ, and b_{i} is defined similarly but with the rightmost edges. Here, we take the reciprocal of ∞ to be 0. In the dual tropical curve, this translates to slopes emanating from vertical edges in the tropical curve having the same difference as from Δ.
Proof of Theorem 6.1.
The inclusion \(\mathbb {M}^{\text {planar}}_{g,\text {hyp}} \subseteq \mathbb {M}_{g}^{\text {chain}}\) holds because every unimodular triangulation of a hyperelliptic polygon is dual to a chain graph. Such a chain has 2g−1 edges, and hence \(\text {dim}\left (\mathbb {M}_{g}^{\text {chain}}\right) = 2g-1\). We also have \(\text {dim}\left (\mathbb {M}^{\text {planar}}_{g,\text {hyp}}\right) \geq 2g-1\) because Lemma 4.2 implies \(\text {dim}\left (\mathbb {M}_{R_{g+1,2}}\right) = 2g-1\). Hence, the inclusion implies the dimension statement.
It remains to prove the equality \(\mathbb {M}_{E^{(g)}_{g+2}} = \mathbb {M}^{\text {planar}}_{g,\text {hyp}}\). Given any triangulation Δ of a hyperelliptic polygon \(E_{k}^{(g)}\), we shall construct a triangulation Δ^{′} of \(E_{g+2}^{(g)}\) such that \(\mathbb {M}_{\Delta }=\mathbb {M}_{\Delta '}\). Our construction will show that the equality even holds at the level of smooth tropical curves.
We start constructing Δ^{′} by drawing g edges from (0,2) to the interior lattice points. The next g−1 edges of Δ^{′} are those that give it the same skeleton as Δ. This means that Δ^{′} has the edge (i,1)−(i+1,1) whenever that edge is in Δ, and Δ^{′} has the edge (0,2)−(2i+1,0) whenever (i,1)−(i+1,1) is not an edge in Δ. Here, i=1,…,g−1.
If n=0, then Δ^{′} includes the edge (0,1)−(1,1).
If n≥2, then Δ^{′} includes (0,1)−(1,1) and all edges (0,1)−(0,m) with 0≤m≤n.
If n=1 and (0,1)−(1,1) is an edge of Δ, then Δ^{′} includes (0,1)−(1,1) and (0,1)−(1,0).
If n=1 and (0,1)−(1,1) is not an edge Δ, then Δ^{′} includes (0,2)−(1,0) and (0,1)−(1,0).
Perform a symmetric construction around (g,1). These edge choices will give the same constraints on the 1^{st} and g^{th} loops as those imposed by Δ. This completes the proof.
We now return to genus g=3, our topic in Section ‘Genus three’, and we complete the computation of \(\mathbb {M}^{\text {planar}}_{3}\).
By Equation 19 and Theorem 6.1, it suffices to compute the 5-dimensional space \(\mathbb {M}_{E_{g+2}^{(g)}}\). An explicit computation as in Section ‘Combinatorics and computations’ reveals that the rectangle \(E^{(3)}_{1} = R_{4,2}\) realizes precisely the same metric graphs as the triangle \(E^{(3)}_{5}\). With this, Theorem 6.1 implies \(\mathbb {M}^{\text {planar}}_{3,\text {hyp}} = \mathbb {M}_{R_{4,2}}\). To complete the computation in Section ‘Genus three’, it thus suffices to analyze the rectangle R_{4,2}.
It was proved in [4] that \(\mathbb {M}_{R_{4,2}}\) and \(\mathbb {M}_{T_{4}}\) have disjoint interiors. Moreover, \(\mathbb {M}_{R_{4,2}}\) is not contained in \(\mathbb {M}_{T_{4}}\). This highlights a crucial difference between Equations 13 and 19. The former concerns the tropicalization of classical moduli spaces, so the hyperelliptic locus lies in the closure of the non-hyperelliptic locus. The analogous statement is false for tropical plane curves. To see that \(\mathbb {M}_{T_{4}}\) does not contain \(\mathbb {M}_{R_{4,2}}\), consider the (020) graph with all edge lengths equal to 1. By Theorems 5.1 and 6.3, this metric graph is in \(\mathbb {M}_{R_{4,2}}\) but not in \(\mathbb {M}_{T_{4}}\). What follows is the hyperelliptic analogue to the non-hyperelliptic Theorem 5.1.
Theorem6.3.
- (020) is realizable if and only if w=x, v≤u, v≤y≤z, and$$\begin{array}{*{20}l} &\hspace*{52pt} (y < v + 2w\,) \hbox{ or}\ \, (y =v + 2w \hbox{ and } y<z\,) \\ &\hbox{or}\ \, (y < v+3w \hbox{ and } u\leq 2v\,) \hbox{ or }\ \, (y = v+3w \hbox{ and } u\leq 2v \hbox{ and } y< z\,) \\ &\hspace*{2pt} \hbox{or}\ \, (y < v+4w \hbox{ and } u=v\,)\ \, \hbox{or}\ \, (\,y = v +4w \hbox{ and } u=v \hbox{ and } y< z\,). \end{array} $$(24)
(111) is realizable if and only if w=x and min{u,v}≤w.
(212) is realizable if and only if w=x.
Proof.
Dimensions of the moduli cones\(\mathbb {M}_{\Delta }\) forR_{4,2} and\(E^{(3)}_{5}\)
R_{4,2} | \({E^{(3)}_{5}}\) | |||||||
---|---|---|---|---|---|---|---|---|
G∖dim | 3 | 4 | 5 | #Δ’s | 3 | 4 | 5 | #Δ’s |
(020) | 42 | 734 | 1,296 | 2,072 | 42 | 352 | 369 | 763 |
(111) | 211 | 695 | 906 | 90 | 170 | 260 | ||
(212) | 127 | 127 | 25 | 25 | ||||
Total | 42 | 945 | 2,118 | 3,105 | 42 | 442 | 564 | 1,048 |
y<v+2w, u≠v, y≠z; (dim=5)
y=v+2w, u≠v, y≠z; (dim=5)
(y<v+3w, v<u<2v, y≠z) or (y<v+2w, u≠v, y<z<2y); (dim=5)
(y<v+3w, u=2v, y≠z) or (y<v+2w, u≠v, z=2y); (dim=4)
(y<v+3w, v<u<2v, y=z) or (y<v+4w, u=v, y<z<2z); (dim=4)
(y<v+3w, u=2v, y=z) or (y<v+4w, u=v, z=2y); (dim=3)
y=v+3w, v<u<2v, y≠z; (dim=4)
y=v+3w, u=2v, y≠z; (dim=3)
(y<v+4w, u=v, y≠z) or (y<v+2w, y=z, u≠v); (dim=3)
y<v+4w, u=v, y=z; (dim=3)
y=v+4w, u=v, y≠z. (dim=3)
Finally, for the graph (212), the single triangulation on the right in Figure 17 suffices.
Genus four
Up to their respective symmetries, the square \(Q^{(4)}_{1} = R_{3,3}\) has 5,941 unimodular triangulations, the triangle \(Q^{(4)}_{2}\) has 1,278 unimodular triangulations, and the triangle \(Q^{(4)}_{3}\) has 20 unimodular triangulations. We computed the cone \(\mathbb {M}_{\Delta }\) for each triangulation Δ, and we ran the pipeline of Section ‘Combinatorics and computations’. We summarize our findings as the main result of this section:
Theorem7.1.
The number of triangulations for the graphs of genus 4 and their moduli dimensions
G | \(\#\Delta _{Q^{(4)}_{1},G}\) | \({\#\Delta _{Q^{(4)}_{2},G}}\) | \({\#\Delta _{Q^{(4)}_{3},G}}\) | \({\dim \left (\mathbb {M}_{Q^{(4)}_{1},G}\right)}\) | \({\dim \left (\mathbb {M}_{Q^{(4)}_{2},G}\right)}\) | \({\dim \left (\mathbb {M}_{Q^{(4)}_{3},G}\right)}\) |
---|---|---|---|---|---|---|
(000)A | 1,823 | 127 | 12 | 9 | 8 | 7 |
(010) | 2,192 | 329 | 2 | 9 | 8 | 7 |
(020) | 351 | 194 | 9 | 8 | ||
(021) | 351 | 3 | 9 | 7 | ||
(030) | 334 | 23 | 1 | 9 | 8 | 7 |
(101) | 440 | 299 | 2 | 8 | 8 | 7 |
(111) | 130 | 221 | 8 | 8 | ||
(121) | 130 | 40 | 1 | 8 | 8 | 7 |
(122) | 130 | 11 | 8 | 7 | ||
(202) | 15 | 25 | 7 | 7 | ||
(212) | 30 | 6 | 1 | 7 | 7 | 7 |
(223) | 15 | 7 | ||||
(303) | 1 | 7 | ||||
Total | 5,941 | 1,278 | 20 |
The four non-realizable graphs are (000)B, (213), (314), and (405). This is obvious for (000)B, because K_{3,3} is not planar. The other three are similar to the genus 3 graph (303) and are ruled out by Proposition 8.3 below. The 13 realizable graphs G appear in the rows in Table 3. The first three columns correspond to the polygons \(Q^{(4)}_{1}\), \(Q^{(4)}_{2}\), and \(Q^{(4)}_{3}\). Each entry is the number of regular unimodular triangulations Δ of \(Q^{(4)}_{i}\) with skeleton G. The entry is blank if no such triangulation exists. Six of the graphs are realized by all three polygons, five are realized by two polygons, and two are realized by only one polygon. For instance, the graph (303) comes from a unique triangulation of the triangle \(Q^{(4)}_{3}\), shown on the right in Figure 18. Neither \(Q^{(4)}_{1}\) nor \(Q^{(4)}_{2}\) can realize this graph.
All cones\(\mathbb {M}_{\Delta }\) from triangulationsΔ of the three genus 4 polygons in Figure 18
\(\boldsymbol {Q^{(4)}_{1}}\) | \(\boldsymbol {Q^{(4)}_{2}}\) | \(\boldsymbol {Q^{(4)}_{3}}\) | |||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
G∖dim | 5 | 6 | 7 | 8 | 9 | 5 | 6 | 7 | 8 | 4 | 5 | 6 | 7 |
(000) | 103 | 480 | 764 | 400 | 76 | 5 | 52 | 60 | 10 | 1 | 6 | 3 | 2 |
(010) | 38 | 423 | 951 | 652 | 128 | 7 | 113 | 155 | 54 | 1 | 1 | ||
(020) | 3 | 32 | 152 | 128 | 36 | 53 | 100 | 41 | |||||
(021) | 3 | 32 | 152 | 128 | 36 | 1 | 2 | ||||||
(030) | 45 | 131 | 122 | 36 | 3 | 12 | 8 | 1 | |||||
(101) | 15 | 155 | 210 | 60 | 19 | 122 | 128 | 30 | 1 | 1 | |||
(111) | 10 | 80 | 40 | 52 | 126 | 43 | |||||||
(121) | 35 | 65 | 30 | 8 | 20 | 12 | 1 | ||||||
(122) | 10 | 80 | 40 | 1 | |||||||||
(202) | 15 | 25 | |||||||||||
(212) | 15 | 15 | 4 | 2 | 1 | ||||||||
(223) | 15 | ||||||||||||
(303) | 1 |
Equipped with these data, we can now extend the probabilistic analysis of Corollary 5.2 from genus 3 to genus 4. As before, we assume that all 17 trivalent graphs are equally likely and we fix the uniform distribution on each 8-simplex that corresponds to one of the 17 maximal cones in the 9-dimensional moduli space \(\mathbb {M}_{4}\). The five graphs that occur with positive probability are those with \(\dim \left (\mathbb {M}_{Q^{(4)}_{1},G}\right) = 9\). Full-dimensional realizations were seen in Figure 20. The result of our volume computations is the following table:
In contrast to the exact computation in Corollary 5.2, our probability computations for genus 4 rely on a Monte Carlo simulation, with 1 million random samples for each graph.
Corollary7.2.
Less than 0.5% of all metric graphs of genus 4 come from plane tropical curves. More precisely, the fraction is approximately \( \kern0.3em \operatorname{vol}\left(\underset{4}{\overset{\mathrm{planar}}{\mathbb{M}}}\right)/\operatorname{vol}\left({\mathbb{M}}_4\right)=0.004788 \).
By Theorem 6.1, \(\,\mathbb {M}^{\text {planar}}_{4,\text {hyp}} = \mathbb {M}_{E^{(g)}_{g+2}}\). This space is 7-dimensional, with six maximal cones corresponding to the chains (020), (021), (111), (122), (202), and (223). The graphs (213), (314), and (405) are hyperelliptic if given the right metric, but beyond not being chain graphs, these are not realizable in the plane even as combinatorial types by Proposition 8.3.
Genus five and beyond
The combinatorial complexity of trivalent graphs and of regular triangulations increases dramatically with g, and one has to be judicious in deciding what questions to ask and what computations to attempt. One way to start is to rule out families of trivalent graphs G that cannot possibly contribute to \(\mathbb {M}^{\text {planar}}_{g}\). Clearly, non-planar graphs G are ruled out. We begin this section by identifying another excluded class. Afterwards, we examine our moduli space for g=5, and we check which graphs arise from the polygons \(Q^{(5)}_{i}\) in Proposition 2.7.
Definition8.1.
A connected, trivalent, leafless graph G is called sprawling if there exists a vertex s of G such that G∖{s} consists of three distinct components.
Remark8.2.
Each component of G∖{s} must have genus at least one; otherwise, G would not have been leafless. The vertex s need not be unique. The genus 3 graph (303) in Figure 4 is sprawling, as are the genus 4 graphs (213), (314), and (405) in Figure 19.
Proposition8.3.
Sprawling graphs are never the skeletons of smooth tropical plane curves.
This was originally proven in [8], Prop. 4.1. We present our own proof for completeness.
Proof.
Suppose the skeleton of a smooth tropical plane curve C is a sprawling graph G with separating vertex s. After a change of coordinates, we may assume that the directions emanating from s are (1,1), (0,−1), and (−1,0). The curve C is dual to a unimodular triangulation Δ of a polygon \(P\subset \mathbb {R}^{2}\). Let T∈Δ be the triangle dual to s. We may take T=conv{(0,0),(0,1),(1,0)} after an appropriate translation of P. Let P_{1},P_{2},P_{3} be the subpolygons of P corresponding to the components of G∖{s}. After relabeling, we have P_{1}∩P_{2}={(0,1)}, P_{1}∩P_{3}={(0,0)}, and P_{2}∩P_{3}={(1,0)}. Each P_{i} has at least one interior lattice point, since each component of G∖{s} must have genus at least 1.
Remark8.4.
If G is sprawling, then \(\mathbb {M}^{\text {planar}}_{g}\cap \mathbb {M}_{G} \not =\emptyset \) because edge lengths can become zero on the boundary. However, it is only in taking closures of spaces of realizable graphs that this intersection becomes nonempty.
We applied the pipeline described in Section ‘Combinatorics and computations’ to all these triangulations. The outcome of our computations is the following result which is the genus 5 analogue to Theorem 7.1.
Theorem8.5.
Of the 71 trivalent graphs of genus 5, precisely 38 are realizable by smooth tropical plane curves. The four polygons satisfy \(\dim \left (\mathbb {M}_{Q^{(5)}_{i}}\right)=9,11,10,10\) for i=1,2,3,4.
The process we have carried out for genus g=3, 4, and 5 can be continued for g≥6. As the genus increases so does computing time, so it may be prudent to limit the computations to special cases of interest. For g=6, we might focus on the triangle \(Q^{(6)}_{1}=T_{5}\). This is of particular interest as it is the Newton polygon of a smooth plane quintic curve. This triangle has 561,885 regular unimodular triangulations up to symmetry.
Although T_{5} is interesting as the Newton polygon of plane quintics, it has the downside that \(\mathbb {M}_{T_{5}}\) is not full-dimensional inside \(\mathbb {M}_{6}^{\text {planar}}\). Proposition 4.3 implies that \(\dim \left (\mathbb {M}_{T_{5}}\right)=12\), while \( \dim \left (\mathbb {M}_{6}^{\text {planar}}\right)=13\), and this dimension is attained by the rectangle R_{3,4} as in Equation 17.
This might lead us to focus on full-dimensional polygons of genus g. By this, we mean polygons P whose moduli space \(\mathbb {M}_{P}\) has the dimension in Equation 4. For each genus from 3 to 5, our results show that there is a unique full-dimensional polygon, namely, T_{4}, R_{3,3}, and \(Q_{2}^{(5)}\). The proof of Theorem 1.1 furnishes an explicit example for each genus g≥6: take the rectangle in Equation 17 or the trapezoid in Equation 18 if g≠7; or the hexagon H_{4,4,2,6} if g=7. Calculations show that there are exactly two full-dimensional maximal polygons for g=6, namely, \(Q_{3}^{(6)}=R_{3,4}\) and \(Q_{4}^{(6)}\) from Proposition 2.7.
We conclude with several open questions.
Question8.6.
What is the relationship between \(\mathbb {M}_{P}\) and \(\mathcal {M}_{P}\)? In particular, does the equality \(\mbox{dim}(\mathbb {M}_{P}) = \text {dim}(\mathcal {M}_{P})\) hold for all P?
How many P with g interior lattice points give a full-dimensional \(\mathbb {M}_{P}\) inside \(\mathbb {M}_{g}^{\text {planar}}\)?
Is there a more efficient way of determining if a combinatorial graph of genus g appears in \(\mathbb {M}_{g}^{\text {planar}}\) than running the pipeline in Section ‘Combinatorics and computations’?
Acknowledgements
We thank Wouter Castryck and John Voight for helpful comments on a draft of this paper. SB was supported by a European Research Council grant SHPEF awarded to Olga Holtz. MJ received support from the Einstein Foundation Berlin and the Deutsche Forschungsgemeinschaft. RM and BS were supported by the US National Science Foundation.
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