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Severi dimensions for unicuspidal curves

Ethan Cotterill Instituto de Matemática, UFF Rua Mário Santos Braga, S/N, 24020-140 Niterói RJ, Brazil [email protected] Vinícius Lara Lima Departamento de Matemática, ICEx, UFMG Av. Antônio Carlos 6627, 30123-970 Belo Horizonte MG, Brazil [email protected]  and  Renato Vidal Martins Departamento de Matemática, ICEx, UFMG Av. Antônio Carlos 6627, 30123-970 Belo Horizonte MG, Brazil [email protected]
Abstract.

We study parameter spaces of linear series on projective curves in the presence of unibranch singularities, i.e. cusps; and to do so, we stratify cusps according to value semigroup. We show that generalized Severi varieties of maps 1n\mathbb{P}^{1}\rightarrow\mathbb{P}^{n} with images of fixed degree and arithmetic genus are often reducible whenever n3n\geq 3. We also prove that the Severi variety of degree-dd maps with a hyperelliptic cusp of delta-invariant gdg\ll d is of codimension at least (n1)g(n-1)g inside the space of degree-dd holomorphic maps 1n\mathbb{P}^{1}\rightarrow\mathbb{P}^{n}; and that for small gg, the bound is exact, and the corresponding space of maps is the disjoint union of unirational strata. Finally, we conjecture a generalization for unicuspidal rational curves associated to an arbitrary value semigroup.

Key words and phrases:
linear series, rational curves, singular curves, semigroups
1991 Mathematics Subject Classification:
Primary 14H20, 14H45, 14H51, 20Mxx

1. Introduction

Rational curves are essential tools for classifying complex algebraic varieties. It is less well-known, however, that singular rational curves in projective space are often interesting in and of themselves. Rational curves of fixed degree dd in n\mathbb{P}^{n} are parameterized by an open subset of the Grassmannian 𝔾(d,n)\mathbb{G}(d,n); and singular rational curves arise from special intersections of (dn1)(d-n-1)-dimensional projection centers of rational normal curves with elements of their osculating flags in particular points. Precisely how this arises is often obscure, and in general a singularity is not uniquely determined by the ramification data encoded by these intersection numbers. One of the aims of this paper is to shed light on the conditions beyond ramification that determine a unibranch singularity, and in the process produce a relatively explicit description of the associated parameter spaces of unicuspidal rational curves.

The situation when n=2n=2 has been studied extensively, and in this case the geometry is relatively well-behaved. Zariski [12] first established an upper bound for the dimension of any given component of the Severi variety Md,g2M^{2}_{d,g} of plane curves of fixed degree dd and genus gg, and showed that whenever the upper bound is achieved, a general curve in that component is nodal. Zariski’s result subsequently played an important role in Harris’ celebrated proof [10] of the irreducibility of Md,g2M^{2}_{d,g}; an upshot of their work is that every curve indexed by a point of Md,g2M^{2}_{d,g} lies in the closure of the irreducible sublocus of Md,g2M^{2}_{d,g} that parameterizes gg-nodal rational curves. However irreducibility, and the dominating role of the nodal locus, simultaneously fail in a particularly simple way when one replaces Md,g2M^{2}_{d,g} by Md,gnM^{n}_{d,g}, the “Severi variety” of degree-dd morphisms 1n\mathbb{P}^{1}\rightarrow\mathbb{P}^{n} of degree dd and arithmetic genus gg. Indeed, as we saw in [6], it is easy to construct examples of Severi varieties Md,gnM^{n}_{d,g} with components of strictly-larger dimension than that of the gg-nodal locus as soon as n8n\geq 8. Each of the excess components produced in [6] parameterizes rational unicuspidal curves for which the corresponding value semigroup is of a particular type, which we christened γ\gamma^{\ast}-hyperelliptic by analogy with Fernando Torres’ γ\gamma-hyperelliptic semigroups [11].

In this paper, we take a closer look at rational unicuspidal curves whose value semigroup S{\rm S} is γ\gamma-hyperelliptic. The simplest case is that of γ=0\gamma=0, in which the underlying cusps are hyperelliptic, meaning simply that 2S2\in{\rm S}. We show that when dgd\gg g, a hyperelliptic cusp of genus gg imposes at least (n1)g(n-1)g independent conditions on rational curves of degree dd in n\mathbb{P}^{n}; moreover, we expect this lower bound to be sharp. This result should be compared against the benchmark codimension (n2)g(n-2)g of the space of degree-dd rational curves with gg (simple) nodes. Our analysis is predicated on a systematic implementation of a scheme for counting conditions associated with cusps described in [6], for which we also give a graphical interpretation at the level of the Dyck path of the corresponding value semigroup. More precisely, our strategy is to fix the local ramification profile, making a linear change of basis if necessary so that the parameterizing functions of our rational curves are ordered according to their vanishing orders in the preimage of the cusp. We can then write down explicitly those conditions beyond ramification that characterize the cusp, and the upshot of this is an explicit dominant rational map from an affine space to each stratum of fixed ramification profile; in particular, each of these strata is unirational.

Going beyond the hyperelliptic case, we give an explicit lower bound for the codimension of the space Md,g;SγnM^{n}_{d,g;{\rm S}_{\gamma}} of unicuspidal rational curves of fixed degree dgd\gg g with a γ\gamma-hyperelliptic cusp of genus gg and of maximal weight, inside the space MdnM^{n}_{d} of all degree-dd rational curves in n\mathbb{P}^{n}. Torres showed that when gγg\gg\gamma, such cusps are precisely those with value semigroup Sγ=22,2γ+1+2g4γ+1{\rm S}_{\gamma}=2\langle 2,2\gamma+1\rangle+\langle 2g-4\gamma+1\rangle. We conjecture that our bound computes the exact codimension of Md,g;SγnM^{n}_{d,g;{\rm S}_{\gamma}} in MdnM^{n}_{d}, and we give some computational as well as qualitative evidence for this. Motivated by our results for γ\gamma-hyperelliptic cusps of maximal weight, we also give a conjectural combinatorial formula for the codimension of the locus Md,g;SnM^{n}_{d,g;{\rm S}} of rational curves with cusps of arbitrary type S{\rm S}. The existence of such a combinatorial formula, albeit conjectural, aligns with the basic mantra (which we borrow from the study of compactified Jacobians of cusps) that the topology of Md,g;SnM^{n}_{d,g;{\rm S}} is controlled by S{\rm S} itself. It is also of practical utility. Indeed, we leverage this formula to obtain many new examples of unexpectedly-large Severi varieties associated with γ\gamma-hyperelliptic value semigroups S{\rm S} of minimal weight.

The smaller nn is, however, the more difficult it becomes to produce Severi varieties Md,g;SnM^{n}_{d,g;{\rm S}} of codimension strictly less than (n2)g(n-2)g. Breaking this impasse forced us to rethink our basic organizational protocol for unicuspidal rational curves; and to focus on their stratification according to ramification profile as opposed to value semigroup. Indeed, any Severi variety Md,g;SnM^{n}_{d,g;{\rm S}} of codimension strictly less than (n2)g(n-2)g necessarily contains a generic ramification stratum with the same property. Accordingly, understanding the behavior of the value semigroup S{\rm S} attached to a generic parameterization with given ramification profile is crucial. We show that whenever dgd\gg g and n3n\geq 3, the Severi varieties Md,g;SnM^{n}_{d,g;{\rm S}} obtained from generic cusps are nearly always of unexpectedly small codimension whenever their ramification profiles comprise sequences of consecutive even numbers. We anticipate that an approach based on limit linear series [9] will show that the same codimension estimates remain operative when we substitute Md,g;SnM^{n}_{d,g;{\rm S}} by the space of linear series of degree dd and rank nn on a general curve of arbitrary genus whose images have a cusp of type S{\rm S}.

1.1. Conventions

We work over \mathbb{C}. By rational curve we always mean a projective curve of geometric genus zero; at times, it will be convenient to conflate a curve with a morphism that describes its normalization. A cusp is a unibranch (curve) singularity. We denote by MdnM^{n}_{d} the space of nondegenerate morphisms f:1nf:\mathbb{P}^{1}\rightarrow\mathbb{P}^{n} of degree d>0d>0. Here each morphism is identified with the set of coefficients of its homogeneous parameterizing polynomials, so MdnM^{n}_{d} is a space of frames over an open subset of 𝔾(n,d)\mathbb{G}(n,d). We denote by Md,gnMdnM^{n}_{d,g}\subset M^{n}_{d} the subvariety of morphisms whose images have arithmetic genus g>0g>0. These curves are necessarily singular. Clearly, Md,gnM^{n}_{d,g} contains all curves with gg simple nodes or gg simple cusps.

In this paper, we will invoke a number of standard tools from linear series and singularities. Accordingly, let PC:=f(1)nP\in C:=f(\mathbb{P}^{1})\subset\mathbb{P}^{n} be a cusp. Near PP, the morphism ff is prescribed by a map f:t(f1(t),,fn(t))f:t\mapsto(f_{1}(t),\dots,f_{n}(t)) of power series, or equivalently, by a map of rings

ϕ:R:=[[x1,,xn]][[t]]xifi(t).\displaystyle\begin{matrix}\phi:&R:=\mathbb{C}[[x_{1},\dots,x_{n}]]&\longrightarrow&\mathbb{C}[[t]]\\ &x_{i}&\longmapsto&f_{i}(t).\end{matrix}

Let vt:[[t]]v_{t}:\mathbb{C}[[t]]\rightarrow\mathbb{N} denote the standard valuation induced by the assignment t1t\mapsto 1. Let S:=vt(ϕ(R)){\rm S}:=v_{t}(\phi(R)) denote the numerical value semigroup of PP. The tt-adic valuation vtv_{t} computes the vanishing order in PP of elements of the local algebra of the cusp, so hereafter we will refer to tt-valuations and PP-vanishing orders interchangeably. The (local) genus of the singularity at PP is δP:=#(S)\delta_{P}:=\#(\mathbb{N}\setminus{\rm S}), and the (global arithmetic) genus of CC is the sum of all of these local contributions:

g=PCδP.g=\sum_{P\in C}\delta_{P}.

We focus exclusively on unicuspidal rational curves, whose singularities are unibranch singletons. Abusively, we will use Md,g;SnM^{n}_{d,g;{\rm S}} to refer to the subvariety of Md,gnM^{n}_{d,g} that parameterizes unicuspidal genus-gg rational curves with value semigroup S{\rm S}. The variety Md,g;SnM^{n}_{d,g;{\rm S}} is further stratified according to the strictly-increasing sequence of vanishing orders 𝐤=(k0,k1,,kn){\bf k}=(k_{0},k_{1},\dots,k_{n}) in t=0t=0 of linear combinations of the local sections 1,f1(t),,fn(t)1,f_{1}(t),\dots,f_{n}(t) that parameterize the cusp. Hereafter, we always assume that k0=0k_{0}=0. Specifying these vanishing orders is equivalent to specifying a ramification profile 𝐤(0,1,,n){\bf k}-(0,1,\dots,n) that measures their deviation relative to the generic sequence. As a matter of convenience, we will abusively conflate these two notions. Accordingly, we let Md,g;S,𝐤nMd,g;SnM^{n}_{d,g;{\rm S},{\bf k}}\subset M^{n}_{d,g;{\rm S}} denote the subvariety of unicuspidal curves with ramification profiles 𝐤{\bf k} in the preimages of their respective cusps.

It will often be convenient to think of the genus of a cusp as an invariant of the associated numerical semigroup S{\rm S}. Similarly, the weight of a cusp is defined in terms of the associated value semigroup by

W=WS:=i=1gi(g+12)W=W_{{\rm S}}:=\sum_{i=1}^{g}\ell_{i}-\binom{g+1}{2}

where 1<<g\ell_{1}<\dots<\ell_{g} denote the gg elements of S\mathbb{N}\setminus{{\rm S}}.

Given a nonnegative integer γ\gamma, a numerical semigroup S{\rm S} is γ\gamma-hyperelliptic if it contains exactly γ\gamma even elements in the interval [2,4γ][2,4\gamma], and 4γ+2S4\gamma+2\in{\rm S}. Note that when γ=0\gamma=0, the first condition is vacuous, while the second condition stipulates that 2S2\in{\rm S}: in this situation, S{\rm S} is simply hyperelliptic. A useful fact is that every numerical semigroup is γ\gamma-hyperelliptic for a unique value of γ\gamma, i.e., numerical semigroups are naturally stratified according to hyperellipticity degree.

1.2. Roadmap

A more detailed synopsis of the material following this introduction is as follows. In Section 2, we prove Theorem 2.1, which gives a lower bound on the codimension of the locus of rational curves f=(fi)i=0n:1nf=(f_{i})_{i=0}^{n}:\mathbb{P}^{1}\rightarrow\mathbb{P}^{n} with hyperelliptic cusps as a function of the vanishing orders of the parameterizing functions fif_{i} in the cusps’ preimages. Theorem 2.1 implies that the codimension of the locus of curves with a hyperelliptic cusp of genus gg is at least (n1)g(n-1)g; to prove it, we produce an explicit packet of polynomials in the fif_{i} that impose independent conditions on their coefficients. Roughly speaking, these polynomials are of the simplest possible type suggested by the arithmetic structure of the value semigroup S=2,2g+1{\rm S}=\langle 2,2g+1\rangle. Proposition 2.5 establishes that whenever g7g\leq 7, these polynomials generate all nontrivial conditions imposed by a hyperelliptic cusp of genus gg, and therefore, that the space of rational curves with hyperelliptic cusps has codimension exactly (n1)g(n-1)g and that each of its subsidiary fixed-ramification strata is unirational in this regime. Our argument is computer-based; however, to obtain a result for all gg, it would suffice to prove that the pattern detailed in Table 1 persists in general.

In Section 3 we turn our focus to (rational curves with) γ\gamma-hyperelliptic cusps of maximal weight, which naturally generalize the hyperelliptic cusps considered in Section 2. In Theorem 3.1, we obtain an explicit lower bound for the codimension of rational curves with genus-gg γ\gamma-hyperelliptic cusps of maximal weight, whenever gγg\gg\gamma. We use the arithmetic structure of the underlying semigroup Sγ{\rm S}_{\gamma} to produce an explicit packet of polynomials in the parameterizing functions fif_{i} of our curves, which in turn impose independent conditions on the coefficients of the fif_{i}. We conjecture that these conditions are in fact a complete set of conditions imposed by γ\gamma-hyperelliptic cusps of Sγ{\rm S}_{\gamma} type, and in Example 3.5 we provide evidence for this; see especially Table 2. Our analysis leads directly to Conjecture 3.6, which gives a value-theoretic prediction for the codimension of Md,g;SnM^{n}_{d,g;{\rm S}} in general, whenever this space is nonempty. Our Theorem 3.8 establishes that the prediction made by Conjecture 3.6 for the codimension is at least a lower bound.

In Subsection 3.1, we study (unicuspidal rational curves with) γ\gamma-hyperelliptic value semigroups S{\rm S} of minimal weight. These include, in particular, the γ\gamma^{\ast}-hyperelliptic examples studied in [6]. In Proposition 3.11, we exhaustively classify the minimally-ramified strata of such mapping spaces when the target dimension nn is at most 7, and as a result we find twenty-one new Severi varieties which should be unexpectedly large; we are able to verify this with Macaulay2 in thirteen cases by certifying that our set of conditions is exhaustive, before running out of computing power. These include the first-known examples with six- and seven-dimensional targets. Assuming the validity of Conjecture 3.6, in Proposition 3.13 we produce new infinite families of unexpectedly large Severi varieties in every target dimension (resp., genus) 6 (resp., 21) or larger. In Subsection 3.2, on the other hand, we unconditionally construct infinitely many unexpectedly large Severi varieties from generic cusps with ramification profiles of the form (2m,2m+2,,2m+2n2)(2m,2m+2,\dots,2m+2n-2) whenever n3n\geq 3. In particular, our results are optimal in the ambient target dimension. At present we are not able to compute the exact genera of such Severi varieties when n4n\geq 4; see Theorem 3.14 for a precise statement. However, when n=3n=3 we manage to determine the corresponding generic semigroup (and its genus) explicitly; our Theorem 3.16 shows, in particular, that its genus growth is quadratic in mm.

1.3. Acknowledgements

We are grateful to Dori Bejleri, Nathan Kaplan, Nathan Pflueger, and Joe Harris for helpful conversations, to the anonymous referee for helpful comments on the exposition, and to Fernando Torres both for initiating the geometric study of the semigroups that bear his name and for his interest in this ongoing project. We dedicate this paper to his memory. The third named author is supported by CNPq grant 305240/2018-8.

2. Counting conditions imposed by hyperelliptic cusps

Cusps form a naturally distinguished (simple) class of singularities. Accordingly, it makes sense to ask for dimension estimates for rational curves with at-worst cusps as singularities. In this section, we prove the following result for unicuspidal rational curves, when the cusps in question are hyperelliptic.

Theorem 2.1.

Given a vector 𝐤:=(k0,,kn)0n+1{\bf k}:=(k_{0},\ldots,k_{n})\in\mathbb{N}_{\geq 0}^{n+1}, let 𝒱𝐤:=Md,g;2,2g+1,𝐤nMd,gn\mathcal{V}_{\bf{k}}:=M^{n}_{d,g;\langle 2,2g+1\rangle,{\bf k}}\subset M^{n}_{d,g}. Suppose, moreover, that n2gn\leq 2g and dmax(n,2g2)d\geq\max(n,2g-2), and that 𝒱𝐤\mathcal{V}_{\bf k}\neq\emptyset; then

cod(𝒱𝐤,Mdn)(n1)g+i=2n(ki2i).{\rm cod}(\mathcal{V}_{{\bf k}},M^{n}_{d})\geq(n-1)g+\sum_{i=2}^{n}\left(\frac{k_{i}}{2}-i\right).

In particular, the variety 𝒱:=Md,g;2,2g+1n\mathcal{V}:=M^{n}_{d,g;\langle 2,2g+1\rangle} of rational curves with a unique singularity of hyperelliptic cuspidal type is of codimension at least (n1)g(n-1)g in MdnM^{n}_{d}.

Remark 2.2.

The condition dnd\geq n is imposed by the requirement that our rational curves be nondegenerate, while the condition n2gn\leq 2g is an artifact of our method of proof (though likely this assumption may be removed). It is less clear what a reasonable lower threshold for the degree as a function of the genus should be; however, the assumption that d2g2d\geq 2g-2 includes the (canonical) case in which d=2g2d=2g-2 and n=g1n=g-1. Note that 𝒱𝐤\mathcal{V}_{\bf k} is nonempty if and only if k0=0k_{0}=0, k1=2k_{1}=2, and the remaining kik_{i}, i=2,,ni=2,\dots,n belong to 2,2g+1\langle 2,2g+1\rangle.

Proof.

Let CC denote the image of a morphism f:1nf:\mathbb{P}^{1}\rightarrow\mathbb{P}^{n} corresponding to a point of 𝒱\mathcal{V}. Then CC ramifies at PP to order

(1) rP=i=1n(kii)r_{P}=\sum_{i=1}^{n}(k_{i}-i)

and we have

(2) cod(𝒱𝐤,Mdn)=rP+bP1{\rm cod}(\mathcal{V}_{\bf k},M^{n}_{d})=r_{P}+b_{P}-1

in which bPb_{P} denotes the number of independent conditions beyond ramification, and the 1-1 on the right-hand side of (2) arises from varying the preimage of PP along 1\mathbb{P}^{1}.

Here we may assume k0=0k_{0}=0 and k1=2k_{1}=2 without loss of generality. In view of (1) and (2), it suffices to show that each fif_{i}, i=2,,ni=2,\dots,n produces at least gki2g-\frac{k_{i}}{2} conditions beyond ramification. We may further suppose that ki<2gk_{i}<2g, i=1,,ni=1,\dots,n, since whenever ki2gk_{i}\geq 2g for some ii, each of the fjf_{j}’s with jij\geq i produces at least gg ramification conditions. In light of our assumption that n2gn\leq 2g this means, in particular, that every kik_{i} is even.

Without loss of generality, we may also assume that f1(P)=(0:1)1f^{-1}(P)=(0:1)\in\mathbb{P}^{1}, and that the cusp supported in PP is parameterized by tt-power series (f1,,fn)(f_{1},\dots,f_{n}), where

(3) f1=t2+a1,3t3+a1,4t4+f2=tk2+a2,k2+1tk2+1+a2,k2+2tk2+2+fn=tkn+an,kn+1tkn+1+an,kn+2tkn+2+\begin{split}f_{1}&=t^{2}+a_{1,3}t^{3}+a_{1,4}t^{4}+\cdots\\ f_{2}&=t^{k_{2}}+a_{2,k_{2}+1}t^{k_{2}+1}+a_{2,k_{2}+2}t^{k_{2}+2}+\cdots\\ &\ \ \ \ \ \ \vdots\\ f_{n}&=t^{k_{n}}+a_{n,k_{n}+1}t^{k_{n}+1}+a_{n,k_{n}+2}t^{k_{n}+2}+\cdots\end{split}

for suitable complex coefficients ai,ja_{i,j}. Note that the power series fif_{i} in (3) is equal to the quotient of the iith and 0th global parameterizing functions introduced previously.

We now recursively define

Fi:=fif1ki2,Fi,1:=Fi, and Fi,j:=Fi,j1([tki+2(j1)]Fi,j1)f1ki2+j1F_{i}:=f_{i}-f_{1}^{\frac{k_{i}}{2}},F^{\ast}_{i,1}:=F_{i},\text{ and }F^{\ast}_{i,j}:=F^{\ast}_{i,j-1}-([t^{k_{i}+2(j-1)}]F^{\ast}_{i,j-1})f_{1}^{\frac{k_{i}}{2}+j-1}

for every 2in2\leq i\leq n and 2jgki/22\leq j\leq g-k_{i}/2. The odd number ki+2j1k_{i}+2j-1 is a gap of the value semigroup of the hyperelliptic cusp, so the coefficient of [tki+2j1]Fi,j[t^{k_{i}+2j-1}]F^{\ast}_{i,j} must vanish. Let Ci,jC_{i,j} denote the polynomial in the coefficients of fif_{i} and f1f_{1} associated with the vanishing condition [tki+2j1]Fi,j=0[t^{k_{i}+2j-1}]F^{\ast}_{i,j}=0. Those coefficients of fif_{i} that appear in Ci,jC_{i,j} run from ai,ki+1a_{i,k_{i}+1} to ai,ki+2j1a_{i,k_{i}+2j-1}; and Ci,jC_{i,j} is linear in the variables ai,ki+2j1a_{i,k_{i}+2j-1}. It follows that the equations Ci,j=0C_{i,j}=0 are algebraically independent; and for every i2i\geq 2, there are gki2g-\frac{k_{i}}{2} independent conditions beyond ramification, as required. ∎

Example 2.3.

In Theorem 2.1, we showed that bPi=2n(gi)b_{P}\geq\sum_{i=2}^{n}(g-i). In this example we detail the case in which n=4n=4 and g=7g=7, in order to show that our lower bound on bPb_{P} is often an equality. It will motivate the following two results, and will serve as a template for the proofs of several others. Our strategy is predicated on producing a set of elements in the local algebra of a hyperelliptic cusp that algebraically generate all conditions beyond ramification; we call these GG-polynomials. To prove that GG-polynomials algebraically generate the set of conditions beyond ramification, we begin with a “universal” element FF in the local algebra, thought of as a polynomial in those nn-tuples of power series (f1,,fn)(f_{1},\dots,f_{n}) that parameterize elements of Md,g;S,𝐤nM^{n}_{d,g;{\rm S},{\bf k}} near their respective cusps. We then argue inductively on the tt-adic valuations of these power series; as the valuation of FF necessarily belongs to S{\rm S}, gaps of S{\rm S} enforce algebraic conditions on the coefficients of the parameterizing series fif_{i}.

More precisely, let S=2,15{\rm S}=\langle 2,15\rangle and 𝐤=(2,4,6,8){\bf k}=(2,4,6,8). Near the cusp, the corresponding universal parameterization is defined by power series

f1\displaystyle f_{1} =t2+a1,3t3+a1,4t4+\displaystyle=t^{2}+a_{1,3}t^{3}+a_{1,4}t^{4}+\cdots
f2\displaystyle f_{2} =t4+a2,5t5+a2,6t6+\displaystyle=t^{4}+a_{2,5}t^{5}+a_{2,6}t^{6}+\cdots
f3\displaystyle f_{3} =t6+a3,7t7+a3,8t8+\displaystyle=t^{6}+a_{3,7}t^{7}+a_{3,8}t^{8}+\cdots
f4\displaystyle f_{4} =t8+a4,9t9+a4,10t10+\displaystyle=t^{8}+a_{4,9}t^{9}+a_{4,10}t^{10}+\cdots

Now any F𝒪PF\in\mathcal{O}_{P} is of the form

(4) F=E+G+H+IF=E+G+H+I

where E,F,G[f1,,f4]E,F,G\in\mathbb{C}[f_{1},\ldots,f_{4}] have tt-adic valuations less than or equal to 2g12g-1, and II belongs to the conductor ideal of 𝒪P\mathcal{O}_{P}111It is well-known that every element of 𝒪P\mathcal{O}_{P} with valuation 2g2g belongs to II, so a decomposition of FF as in (4) always exists.. In particular, we have

E\displaystyle E :=α(0)+α(1)f1;\displaystyle:=\alpha_{(0)}+\alpha_{(1)}f_{1};
G\displaystyle G :=i=24α(i)fi+j=26α(1j)f1j; and\displaystyle:=\sum\limits^{4}_{i=2}\alpha_{(i)}f_{i}+\sum\limits_{j=2}^{6}\alpha_{(1^{j})}f_{1}^{j};\text{ and }
H\displaystyle H :=α(2,1)f1f2+α(2,12)f12f2+α(3,1)f1f3+α(22)f22+α(3,12)f12f3+α(2,13)f13f2+\displaystyle:=\alpha_{(2,1)}f_{1}f_{2}+\alpha_{(2,1^{2})}f_{1}^{2}f_{2}+\alpha_{(3,1)}f_{1}f_{3}+\alpha_{(2^{2})}f_{2}^{2}+\alpha_{(3,1^{2})}f_{1}^{2}f_{3}+\alpha_{(2,1^{3})}f_{1}^{3}f_{2}+
α(22,1)f1f22+α(4,1)f1f4+α(3,2)f2f3+α(2,14)f14f2+α(3,13)f13f3+α(4,12)f12f4+\displaystyle\ \alpha_{(2^{2},1)}f_{1}f_{2}^{2}+\alpha_{(4,1)}f_{1}f_{4}+\alpha_{(3,2)}f_{2}f_{3}+\alpha_{(2,1^{4})}f_{1}^{4}f_{2}+\alpha_{(3,1^{3})}f_{1}^{3}f_{3}+\alpha_{(4,1^{2})}f_{1}^{2}f_{4}+
α(22,12)f12f22+α(3,2,1)f1f2f3+α(23)f23+α(4,2)f2f4+α(32)f32.\displaystyle\ \alpha_{(2^{2},1^{2})}f_{1}^{2}f_{2}^{2}+\alpha_{(3,2,1)}f_{1}f_{2}f_{3}+\alpha_{(2^{3})}f_{2}^{3}+\alpha_{(4,2)}f_{2}f_{4}+\alpha_{(3^{2})}f_{3}^{2}.

To iteratively produce algebraic constraints beyond ramification, we now argue as follows. If α(0)=0\alpha_{(0)}=0 (resp. α(0)=α(1)=0\alpha_{(0)}=\alpha_{(1)}=0) in (4), we immediately deduce that FF has valuation at least 22 (resp., 44), as 11 (resp., 33) belongs to S\mathbb{N}\setminus{\rm S} and as such is disallowed as a vanishing order. Similarly, terms in the conductor ideal contribute no conditions; so without loss of generality, we may assume that E=I=0E=I=0. Accordingly, we may rewrite FF as

F\displaystyle F :=α(2)f2+α(12)f12\displaystyle:=\alpha_{(2)}f_{2}+\alpha_{(1^{2})}f_{1}^{2}
+α(3)f3+α(13)f13+α(2,1)f1f2\displaystyle\ +\alpha_{(3)}f_{3}+\alpha_{(1^{3})}f_{1}^{3}+\alpha_{(2,1)}\ f_{1}f_{2}
+α(4)f4+α(14)f14+α(2,12)f12f2+α(3,1)f1f3+α(22)f22\displaystyle\ +\alpha_{(4)}f_{4}+\alpha_{(1^{4})}f_{1}^{4}+\alpha_{(2,1^{2})}f_{1}^{2}f_{2}+\alpha_{(3,1)}f_{1}f_{3}+\alpha_{(2^{2})}f_{2}^{2}
+α(15)f15+α(3,12)f12f3+α(2,13)f13f2+α(22,1)f1f22+α(4,1)f1f4+α(3,2)f2f3\displaystyle\ +\alpha_{(1^{5})}f_{1}^{5}+\alpha_{(3,1^{2})}f_{1}^{2}f_{3}+\alpha_{(2,1^{3})}f_{1}^{3}f_{2}+\alpha_{(2^{2},1)}f_{1}f_{2}^{2}+\alpha_{(4,1)}f_{1}f_{4}+\alpha_{(3,2)}f_{2}f_{3}
+α(16)f16+α(2,14)f14f2+α(3,13)f13f3+α(4,12)f12f4+α(22,12)f12f22+α(3,2,1)f1f2f3\displaystyle\ +\alpha_{(1^{6})}f_{1}^{6}+\alpha_{(2,1^{4})}f_{1}^{4}f_{2}+\alpha_{(3,1^{3})}f_{1}^{3}f_{3}+\alpha_{(4,1^{2})}f_{1}^{2}f_{4}+\alpha_{(2^{2},1^{2})}f_{1}^{2}f_{2}^{2}+\alpha_{(3,2,1)}f_{1}f_{2}f_{3}
+α(23)f23+α(4,2)f2f4+α(32)f32\displaystyle\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ +\alpha_{(2^{3})}f_{2}^{3}+\alpha_{(4,2)}f_{2}f_{4}+\alpha_{(3^{2})}f_{3}^{2}

in which each line in the above diagram corresponds to a homogeneous summand of fixed valuation.

We now expand FF as a power series in tt. The initial part of the expansion reads

F=(α(2)+α(12))t4+(a2,5α(2)+2a1,3α(12))t5+O(t6)F=(\alpha_{(2)}+\alpha_{(1^{2})})t^{4}+(a_{2,5}\alpha_{(2)}+2a_{1,3}\alpha_{(1^{2})})t^{5}+O(t^{6})

so that vt(F)>4v_{t}(F)>4 if and only if

ϕ1(α(2),α(12)):=α(2)+α(12)=0.\phi_{1}(\alpha_{(2)},\alpha_{(1^{2})}):=\alpha_{(2)}+\alpha_{(1^{2})}=0.

Accordingly, we set α(12)=1(α(2)):=α(2)\alpha_{(1^{2})}=\ell_{1}(\alpha_{(2)}):=-\alpha_{(2)}; and, therefore, the coefficient of t5t^{5} above becomes

ψ1(α(2)):=α(2)(a2,52a1,3).\psi_{1}(\alpha_{(2)}):=\alpha_{(2)}(a_{2,5}-2a_{1,3}).

The

fact that 55 is a gap now forces ψ1=0\psi_{1}=0 for every α(2)\alpha_{(2)}\in\mathbb{C}, i.e., that

G1=0G_{1}=0

where G1:=a2,52a1,3G_{1}:=a_{2,5}-2a_{1,3}; up to multiplication by constant, this is the unique condition imposed by the fact that 5S5\notin{\rm S}.

In

order to capture the essence of the method, we will no longer explicitly record the polynomials but simply mention which coefficients αλ\alpha_{\lambda} are involved at each step.

In

a second step, we write

F=ψ1t5+ϕ2t6+ψ2t7+O(t8)F=\psi_{1}t^{5}+\phi_{2}t^{6}+\psi_{2}t^{7}+O(t^{8})

and we impose ϕ2=0\phi_{2}=0, which in turn allows us to rewrite ψ2\psi_{2} as

ψ2=α(2)G2+α(3)G3+α(2,1)G1.\psi_{2}=\alpha_{(2)}G_{2}+\alpha_{(3)}G_{3}+\alpha_{(2,1)}G_{1}.

The upshot is that through step two of our procedure, the polynomials GG are responsible for all of the conditions imposed on the coefficients of the parameterizing functions fif_{i}. Indeed, G1=0G_{1}=0 is the unique condition arising from step one, so the new conditions in step two are G2=0G_{2}=0 and G3=0G_{3}=0.

More generally, at step ss of our procedure, we write

F=ψs1t2s+1+ϕst2s+2+ψs+1t2s+3+O(t2s+4)F=\psi_{s-1}t^{2s+1}+\phi_{s}t^{2s+2}+\psi_{s+1}t^{2s+3}+O(t^{2s+4})

and set ϕs=0\phi_{s}=0; then ψs=0\psi_{s}=0 is forced, and this allows us to rewrite ψs\psi_{s} as a linear combination of polynomials in the coefficients of the parameterizing functions fif_{i}.

Referencing the induced decomposition F=G+HF=G+H, we call those polynomial conditions produced by GG (resp., HH) as we iterate our procedure GG-polynomials (resp., HH-polynomials). The following table gives a precise description of each of these sets of polynomials in the coefficients of the fif_{i}; the upshot is that the HH-polynomials are contained in the set of GG-polynomials.

G-polynomials H-polynomials
Gap α(2)\alpha_{(2)} α(3)\alpha_{(3)} α(4)\alpha_{(4)} α(2,1)\alpha_{(2,1)} α(3,1)\alpha_{(3,1)} α(4,1)\alpha_{(4,1)}
55 G1G_{1}
77 G2G_{2} G3G_{3} G1G_{1}
99 G4G_{4} G5G_{5} G6G_{6} G2G_{2} G3G_{3}
1111 G7G_{7} G8G_{8} G9G_{9} G4G_{4} G5G_{5} G6G_{6}
1313 G10G_{10} G11G_{11} G12G_{12} G7G_{7} G8G_{8} G9G_{9}
Table 1. GG- and HH-polynomials for hyperelliptic cusps

More precisely, the conditions imposed by the GG’s (whose scalar multipliers are the variables α(2)\alpha_{(2)}, α(3)\alpha_{(3)}, α(4)\alpha_{(4)}) are systematically reproduced (at precisely one later step) by the HH’s (whose scalar multipliers are α(2,1)\alpha_{(2,1)}, α(3,1)\alpha_{(3,1)}, α(4,1)\alpha_{(4,1)}). All available empirical evidence suggests that this same pattern persists for arbitrary values of gg and nn; proving that this holds in general, which in turn would imply a version of Proposition 2.5 without hypotheses on gg, is an interesting problem.

In Figure 1, we give a graphical interpretation of the conditions imposed by the GG’s, i.e., by the polynomials Fi=Fi,1F_{i}=F^{\ast}_{i,1} and their inductively derived children Fi,jF^{\ast}_{i,j}, j2j\geq 2. Graphically speaking, the index ii specifies a column, while the index jj specifies a number of upward steps from the Dyck path that codifies the semigroup. This graphical interpretation generalizes naturally to the case of γ\gamma-hyperelliptic cusps, as we will see later (compare Figure 2 below).

Refer to caption
Figure 1. Conditions contributing to bPb_{P} and rPr_{P} for rational curves with a hyperelliptic cusp when g=7g=7 and n=4n=4.
Lemma 2.4.

The polynomials of the form G=i=2nα(i)fi+j=k2/2g1α(1j)f1jG=\sum\limits^{n}_{i=2}\alpha_{(i)}f_{i}+\sum\limits_{j=k_{2}/2}^{g-1}\alpha_{(1^{j})}f_{1}^{j} impose exactly i=2n(gki2)\sum_{i=2}^{n}\left(g-\frac{k_{i}}{2}\right) independent conditions beyond ramification.

Proof.

In the general case, when the parameterizing functions fif_{i} have arbitrary even PP-vanishing orders, we write

f1\displaystyle f_{1} =t2+a1,3t3+a1,4t4+\displaystyle=t^{2}+a_{1,3}t^{3}+a_{1,4}t^{4}+\cdots
f2\displaystyle f_{2} =tk2+a2,k2+1tk2+1+a2,k2+2tk2+2+\displaystyle=t^{k_{2}}+a_{2,k_{2}+1}t^{k_{2}+1}+a_{2,k_{2}+2}t^{k_{2}+2}+\cdots
f3\displaystyle f_{3} =tk3+a3,k3+1tk3+1+a3,k3+2tk3+2+\displaystyle=t^{k_{3}}+a_{3,k_{3}+1}t^{k_{3}+1}+a_{3,k_{3}+2}t^{k_{3}+2}+\cdots
\displaystyle\ \ \ \ \ \ \vdots
fn\displaystyle f_{n} =tkn+an,kn+1tkn+1+an+1,kn+2tkn+2+\displaystyle=t^{k_{n}}+a_{n,k_{n}+1}t^{k_{n}+1}+a_{n+1,k_{n}+2}t^{k_{n}+2}+\cdots

and we set li:=ki/2l_{i}:=k_{i}/2, di:=li+1li1d_{i}:=l_{i+1}-l_{i}-1 for all 2in12\leq i\leq n-1, and dn:=gln1d_{n}:=g-l_{n}-1. As a shorthand, we will write αi\alpha_{i} (resp., βi\beta_{i}) in place of α(i)\alpha_{(i)} (resp., α(1i))\alpha_{(1^{i})}) in what follows. We then have

(5) G\displaystyle G =(α2+βl2)t2l2+(α2a2,2l2+1+βl2l2a1,3)t2l2+1+\displaystyle=(\alpha_{2}+\beta_{l_{2}})t^{2l_{2}}+(\alpha_{2}a_{2,2l_{2}+1}+\beta_{l_{2}}l_{2}a_{1,3})t^{2l_{2}+1}+\cdots
(6) +βl2+1t2(l2+1)+βl2+1(l2+1)a1,3t2(l2+1)+1+\displaystyle\ \ \ \ \ +\beta_{l_{2}+1}t^{2(l_{2}+1)}+\beta_{l_{2}+1}(l_{2}+1)a_{1,3}t^{2(l_{2}+1)+1}+\cdots
\displaystyle\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \vdots
(7) +βl2+d2t2(l2+d2)+βl2+d2(l2+d2)a1,3t2(l2+d2)+1+\displaystyle\ \ \ \ \ +\beta_{l_{2}+d_{2}}t^{2(l_{2}+d_{2})}+\beta_{l_{2}+d_{2}}(l_{2}+d_{2})a_{1,3}t^{2(l_{2}+d_{2})+1}+\cdots
(8) +(α3+βl3)t2l3+(α3a3,2l3+1+βl3l3a1,3)t2l3+1+\displaystyle\ \ \ \ \ \ \ \ +(\alpha_{3}+\beta_{l_{3}})t^{2l_{3}}+(\alpha_{3}a_{3,2l_{3}+1}+\beta_{l_{3}}l_{3}a_{1,3})t^{2l_{3}+1}+\cdots
+βl3+1t2(l3+1)+βl3+1(l3+1)a1,3t2(l3+1)+1+\displaystyle\ \ \ \ \ \ \ \ +\beta_{l_{3}+1}t^{2(l_{3}+1)}+\beta_{l_{3}+1}(l_{3}+1)a_{1,3}t^{2(l_{3}+1)+1}+\cdots
\displaystyle\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \vdots
+βl3+d3t2(l3+d3)+βl3+d3(l3+d3)a1,3t2(l3+d3)+1+\displaystyle\ \ \ \ \ \ \ \ +\beta_{l_{3}+d_{3}}t^{2(l_{3}+d_{3})}+\beta_{l_{3}+d_{3}}(l_{3}+d_{3})a_{1,3}t^{2(l_{3}+d_{3})+1}+\cdots
\displaystyle\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \vdots
\displaystyle\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \vdots
+(αn+βln)t2ln+(αnan,2ln+1+βlnlna1,3)t2ln+1+\displaystyle\ \ \ \ \ \ \ \ \ \ +(\alpha_{n}+\beta_{l_{n}})t^{2l_{n}}+(\alpha_{n}a_{n,2l_{n}+1}+\beta_{l_{n}}l_{n}a_{1,3})t^{2l_{n}+1}+\cdots
+βln+1t2(ln+1)+βln+1(ln+1)a1,3t2(ln+1)+1+\displaystyle\ \ \ \ \ \ \ \ \ \ +\beta_{l_{n}+1}t^{2(l_{n}+1)}+\beta_{l_{n}+1}(l_{n}+1)a_{1,3}t^{2(l_{n}+1)+1}+\cdots
\displaystyle\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \vdots
+βln+dnt2(ln+dn)+βln+dn(ln+dn)a1,3t2(ln+dn)+1+.\displaystyle\ \ \ \ \ \ \ \ \ \ +\beta_{l_{n}+d_{n}}t^{2(l_{n}+d_{n})}+\beta_{l_{n}+d_{n}}(l_{n}+d_{n})a_{1,3}t^{2(l_{n}+d_{n})+1}+\cdots.

The

gaps of the semigroup S{\rm S} of PP determine conditions beyond ramification, inasmuch as they may never arise as PP-vanishing orders of elements of 𝒪P\mathcal{O}_{P}. Our method consists in forcing vanishing to successively higher orders; the steps of the associated process are indexed by gaps of S{\rm S}. In the first step we start with the gap 2l2+12l_{2}+1, which is the first gap that appears as an exponent in our putative expansion of GG with generic coefficients. Accordingly we choose

(9) βl2=α2\beta_{l_{2}}=-\alpha_{2}

in order to eliminate the term of degree 2l22l_{2}. The term of degree 2l2+12l_{2}+1 now must vanish, which forces

α2G1=0\alpha_{2}G_{1}=0

where G1=a2,2l2+1l2a1,3G_{1}=a_{2,2l_{2}+1}-l_{2}a_{1,3}. In particular, G1=0G_{1}=0 is the unique condition enforced by the gap 2l2+12l_{2}+1. Moreover, the coefficient of each monomial tkt^{k} appearing in line (5) is computed by a linear form 1,k(α2)\ell_{1,k}(\alpha_{2}) in α2\alpha_{2}.

Similarly

, in a second step indexed by the gap 2(l2+1)+12(l_{2}+1)+1, we set

(10) βl2+1=1,2(l2+1)(α2)\beta_{l_{2}+1}=-\ell_{1,2(l_{2}+1)}(\alpha_{2})

in order to eliminate the term of degree 2(l2+1)2(l_{2}+1). Eliminating the term in degree 2(l2+1)+12(l_{2}+1)+1 now forces

βl2+1(l2+1)a1,3+1,2(l2+1)+1(α2)=0\beta_{l_{2}+1}(l_{2}+1)a_{1,3}+\ell_{1,2(l_{2}+1)+1}(\alpha_{2})=0

which in turn implies that

α2G2=0\alpha_{2}G_{2}=0

where G2G_{2} is a polynomial on the coefficients of the (parameterizing functions of the) curve. So we obtain 1 additional condition, namely, G2=0G_{2}=0. Moreover, in light of (10), we see that any coefficient of a monomial tkt^{k} appearing in line (6) is computed by a linear form 2,k(α2)\ell_{2,k}(\alpha_{2}).

More generally,

each step through the (d2+1)(d_{2}+1)th (indexed by the gap 2(l2+d2)+12(l_{2}+d_{2})+1) produces one additional independent condition; and the coefficients of the powers tkt^{k} in every line until and including (8) are computed by linear forms 3,k(α2),,d2+1,k(α2)\ell_{3,k}(\alpha_{2}),\ldots,\ell_{d_{2}+1,k}(\alpha_{2}).

At

the (d2+2)(d_{2}+2)th step, we set

(11) βl3=α3i=1d2+1i,2l3(α2)\beta_{l_{3}}=-\alpha_{3}-\sum_{i=1}^{d_{2}+1}\ell_{i,2l_{3}}(\alpha_{2})

in order to eliminate the term of degree 2l32l_{3}. This, in turn, forces

(α3a3,2l3+1+βl3l3a1,3)+i=1d2+1i,2l3+1(α2)=0(\alpha_{3}a_{3,2l_{3}+1}+\beta_{l_{3}}l_{3}a_{1,3})+\sum_{i=1}^{d_{2}+1}\ell_{i,2l_{3}+1}(\alpha_{2})=0

in order to obtain vanishing in degree 2l3+12l_{3}+1. We now obtain

α2Gd2+2+α3Gd2+3=0\alpha_{2}G_{d_{2}+2}+\alpha_{3}G_{d_{2}+3}=0

where Gd2+2G_{d_{2}+2} and Gd2+3G_{d_{2}+3} are polynomials in the coefficients of (the parameterizing functions of) the curve. So we get 2 additional conditions, namely Gd2+2=0G_{d_{2}+2}=0 and Gd2+3=0G_{d_{2}+3}=0. We see, moreover, that every coefficient of a monomial tkt^{k} in line (8) is computed by a linear form l3,k(α2,α3)\ell_{l_{3},k}(\alpha_{2},\alpha_{3}): indeed, any such coefficient depends a priori on α3\alpha_{3} and βl3\beta_{l_{3}}, but according to (11), βl3\beta_{l_{3}} depends linearly on the α2\alpha_{2} and α3\alpha_{3}.

Iterating our selection procedure

ultimately yields at most i=2n(i1)(di+1)\sum_{i=2}^{n}(i-1)(d_{i}+1) conditions, generated by the GiG_{i}’s at every step. Here

i=2n(i1)(di+1)=i=2n1(i1)(li+1li)+(n1)(gln)=i=2n1(i1)(ki+1ki2)+(n1)(gkn2)=i=2n(gki2).\begin{split}\sum_{i=2}^{n}(i-1)(d_{i}+1)&=\sum_{i=2}^{n-1}(i-1)(l_{i+1}-l_{i})+(n-1)(g-l_{n})\\ &=\sum_{i=2}^{n-1}(i-1)\left(\frac{k_{i+1}-k_{i}}{2}\right)+(n-1)\left(g-\frac{k_{n}}{2}\right)\\ &=\sum_{i=2}^{n}\left(g-\frac{k_{i}}{2}\right).\end{split}

The argument above shows that the polynomials GG impose at most i=2n(gki2)\sum_{i=2}^{n}\left(g-\frac{k_{i}}{2}\right) algebraically independent conditions beyond ramification. On the other hand, the proof of Theorem 2.1 establishes that there are at least this number of algebraically independent conditions, all imposed by the polynomials FiF_{i} and Fi,jF_{i,j}^{*}. But as the FiF_{i} and Fi,jF_{i,j}^{*} are GG-polynomials, we conclude that the GG-polynomials impose exactly i=2n(gki2)\sum_{i=2}^{n}\left(g-\frac{k_{i}}{2}\right) algebraically independent conditions beyond ramification.

Proposition 2.5.

Let 𝒱\mathcal{V} be the variety of rational curves with a unique singularity that is a hyperelliptic cusp. Suppose that n2gn\leq 2g and dmax(n,2g2)d\geq\max(n,2g-2); then

cod(𝒱,Mdn)=(n1)g{\rm cod}(\mathcal{V},M^{n}_{d})=(n-1)g

and each fixed-ramification substratum 𝒱𝐤𝒱\mathcal{V}_{\bf k}\subset\mathcal{V} is unirational of codimension (n1)g+i=2n(ki2i)(n-1)g+\sum_{i=2}^{n}\left(\frac{k_{i}}{2}-i\right) whenever g7g\leq 7.

Proof.

We verified using Macaulay2 that the set of HH-polynomials is contained in the set of GG-polynomials for every 3ng13\leq n\leq g-1 whenever 4g74\leq g\leq 7; see [1, ancillary file]. This means, in turn, that the algebra of conditions imposed by hyperelliptic cusps is generated by the leading coefficients Ci,jC_{i,j} of the polynomials Fi,jF^{\ast}_{i,j} introduced in the proof of Theorem 2.1. The unirationality of 𝒱𝐤\mathcal{V}_{\bf k} now follows from the fact that each Ci,jC_{i,j} is linear in the variable ai,ki+2j1=[ki+2j1]fia_{i,k_{i}+2j-1}=[k_{i}+2j-1]f_{i} of the “universal” parameterization ff with ramification profile 𝐤{\bf k}. ∎

Remark 2.6.

The area of the rectangle determined by columns 2 through nn of our Dyck diagram (of conditions contributing to bPb_{P} and rPr_{P}) is precisely (n1)g(n-1)g, and in our graphical interpretation all of the corresponding boxes are marked; cf. Figure 1.

3. Counting conditions imposed by γ\gamma-hyperelliptic cusps

In this section, using (the proof of) Theorem 2.1 as a template, we establish a lower bound on the number of conditions imposed on rational curves by a γ\gamma-hyperelliptic cusp of genus gg whose value semigroup is of maximal weight. Fernando Torres proved [11] that whenever gγg\gg\gamma, the unique numerical semigroup with this property is Sg,γ=4,4γ+2,2g4γ+1{\rm S}_{g,\gamma}=\langle 4,4\gamma+2,2g-4\gamma+1\rangle.

Theorem 3.1.

Let 𝒱Sg,γ:=Md,g;Sg,γnMd,gn\mathcal{V}_{{\rm S}_{g,\gamma}}:=M^{n}_{d,g;{\rm S}_{g,\gamma}}\subset M^{n}_{d,g} denote the subvariety consisting of rational curves with a single singularity PP that is a γ\gamma-hyperelliptic cusp with value semigroup Sg,γ{\rm S}_{g,\gamma}, γ>0\gamma>0. Assume as before that n2gn\leq 2g, dmax(2g2,n)d\geq\max(2g-2,n) and, moreover, that g4γ+2g\geq 4\gamma+2. Then

cod(𝒱Sg,γ,Mdn)(n1)gδnγ(2γ+nj3)δnγ+1(3γj2)\begin{split}{\rm cod}(\mathcal{V}_{{\rm S}_{g,\gamma}},M^{n}_{d})&\geq(n-1)g-\delta_{n\leq\gamma}(2\gamma+n-j^{\ast\ast}-3)-\delta_{n\geq\gamma+1}(3\gamma-j^{\ast\ast}-2)\end{split}

where δ\delta is Dirac’s delta and jj^{\ast\ast} is either the unique nonnegative integer for which g(6γ2j1,6γ2j+1]g\in(6\gamma-2j^{\ast\ast}-1,6\gamma-2j^{\ast\ast}+1] or else j=1j^{\ast\ast}=-1.

Remark 3.2.

The hypothesis that g4γ+2g\geq 4\gamma+2 is made in order to ensure that 8γ+42g8\gamma+4\leq 2g, which slightly simplifies the exposition below. Note that 2g4γ+1>4γ+22g-4\gamma+1>4\gamma+2, i.e. g4γ+1g\geq 4\gamma+1, is automatic, because Sg,γ{\rm S}_{g,\gamma} is γ\gamma-hyperelliptic by assumption.

Proof.

The analysis required to produce a lower codimension bound is more delicate than in the γ=0\gamma=0 case, because of the structure of the underlying semigroup Sg,γ{\rm S}_{g,\gamma}. We work locally near a γ\gamma-hyperelliptic cusp PP of a curve [C]𝒱Sg,γ[C]\in\mathcal{V}_{{\rm S}_{g,\gamma}} with PP-vanishing order vector 𝐤=(k0,,kn){\bf k}=(k_{0},\dots,k_{n}); that is, [C][C] belongs to 𝒱𝐤:=Md,g;Sg,γ,𝐤n\mathcal{V}_{{\bf k}}:=M^{n}_{d,g;{\rm S}_{g,\gamma},{\bf k}}. Without loss of generality, we may assume k0=0k_{0}=0, k1=4k_{1}=4, and that kj=4γ+2k_{j^{\ast}}=4\gamma+2 for some positive integer jγ+1j^{\ast}\leq\gamma+1. Abusively, hereafter we refer to the local incarnation of ff as (f1(t),,fn(t))(f_{1}(t),\dots,f_{n}(t)), in which fi=tki+ki+1ai,tf_{i}=t^{k_{i}}+\sum_{\ell\geq k_{i}+1}a_{i,\ell}t^{\ell} for all i=1,,ni=1,\dots,n, for some local coordinate tt centered in PP. The arithmetic structure of Sg,γ{\rm S}_{g,\gamma} interacts with the parameterization ff underlying CC via the following device.

Definition 3.3.

Given a distinct set of natural numbers k1,,knk_{1},\dots,k_{n}, a decomposition of ss\in\mathbb{N} with respect to k1,,knk_{1},\dots,k_{n} is an equation

(12) s=m1k1++mnkns=m_{1}k_{1}+\ldots+m_{n}k_{n}

with non-negative integer coefficients mj,j=1,,nm_{j},j=1,\dots,n. Its underlying partition is (k1m1,,knmn)(k_{1}^{m_{1}},\dots,k_{n}^{m_{n}}). A decomposition as in (12) is reducible whenever some proper sub-sum of the right-hand side of (12) decomposes with respect to k1,,knk_{1},\dots,k_{n}; otherwise it is irreducible.

The following auxiliary notion will also be useful.

Definition 3.4.

Given an element ss of a numerical semigroup S{\rm S}, we set

ρ(s):=#{r>s|rS}.\rho(s):=\#\{r>s\,|\,r\not\in{\rm S}\}.

Case 1:

𝐤{\bf k} consists entirely of even integers. As in the γ=0\gamma=0 case, we have

cod(𝒱𝐤,Mdn)=rP+bP1{\rm cod}(\mathcal{V}_{\bf k},M^{n}_{d})=r_{P}+b_{P}-1

where rP=i=1n(kii)r_{P}=\sum_{i=1}^{n}(k_{i}-i) is the ramification of ff, and bPb_{P} is the number of independent conditions beyond ramification imposed by Sg,γ{\rm S}_{g,\gamma} on ff. These conditions beyond ramification are induced by polynomials in the fif_{i} indexed by irreducible decompositions of elements sSg,γs\in{\rm S}_{g,\gamma} with parts k1,,knk_{1},\dots,k_{n}.

Subcase 1.1: s4γs\leq 4\gamma. Note that ss is a multiple of 4 in this range. When s{k2,,kj1}s\notin\{k_{2},\dots,k_{j^{\ast}-1}\}, ss admits a unique irreducible decomposition with respect to k1,,knk_{1},\dots,k_{n}, whose underlying partition is (4s/4)(4^{s/4}); ss then gives zero net contribution to the codimension of 𝒱𝐤\mathcal{V}_{\bf k}. Now say s=kjs=k_{j} for some j[2,j1]j\in[2,j^{\ast}-1]. Then ss contributes (at least) ρ(s)\rho(s) independent conditions to bPb_{P}. To see this, we begin much as in the γ=0\gamma=0 case by setting Fj:=fjf1kj4F_{j}:=f_{j}-f_{1}^{\frac{k_{j}}{4}}. Then vt(Fj)v_{t}(F_{j}) is at least kj+1k_{j}+1, which belongs to Sg,γ\mathbb{N}\setminus{\rm S_{g,\gamma}} and is thereby precluded. By the same logic, we have

(13) [tkj+1]Fj=[tkj+2]Fj==[tkj1]Fj=0[t^{k_{j}+1}]F_{j}=[t^{k_{j}+2}]F_{j}=\dots=[t^{k_{j}^{\ast}-1}]F_{j}=0

where kjk_{j}^{\ast} is the smallest element of Sg,γ{\rm S}_{g,\gamma} strictly greater than kjk_{j}. Independence of the linear vanishing conditions (13) is clear. On the other hand, once the conditions (13) have been imposed, we have vt(Fj)=kjv_{t}(F_{j})=k_{j}^{\ast}, since the remaining nonzero coefficients of FjF_{j} are generic. If kj<4γk_{j}<4\gamma, we now iterate this procedure, setting Fj:=Fj[tkj]Fjf1kj4F_{j}^{\ast}:=F_{j}-[t^{k_{j}^{\ast}}]F_{j}\cdot f_{1}^{\frac{k_{j}^{\ast}}{4}}. Replacing FjF_{j} by FjF_{j}^{\ast} and kjk_{j} by kjk_{j}^{\ast} yields a set of vanishing conditions analogous to (13). On the other hand, if kj=4γk_{j}=4\gamma, then kj=kj=4γ+2k_{j}^{\ast}=k_{j^{\ast}}=4\gamma+2, and we set Fj:=Fj[t4γ+2]FjfjF_{j}^{\ast}:=F_{j}-[t^{4\gamma+2}]F_{j}\cdot f_{j^{\ast}}, whose leading term must vanish. We then iterate by replacing FjF_{j} by FjF_{j}^{\ast} and subtracting a scalar multiple of any monomial in powers of f1f_{1} and fjf_{j^{\ast}} with valuation equal to that of (the new version of) FjF_{j}. Our procedure continues in this way until all gaps of Sg,γ{\rm S}_{g,\gamma} greater than kjk_{j} and less than 2g4γ2g-4\gamma have been exhausted, and the conditions obtained are algebraically independent; indeed, the linear part of the condition imposed by a given gap q>kjSg,γq\in\mathbb{N}_{>k_{j}}\setminus{\rm S}_{g,\gamma} is precisely aj,qkj4a1,q+4kja_{j,q}-\frac{k_{j}}{4}a_{1,q+4-k_{j}}, so new variables appear linearly in the coefficients that are required to vanish at every step.

Our iterative procedure may be interpreted graphically with respect to the Dyck path 𝒫\mathcal{P} associated with Sg,γ{\rm S}_{g,\gamma} inside its g×gg\times g bounding box. There is a horizontal step in 𝒫\mathcal{P} labeled by kjk_{j}; so kjk_{j} singles out a column in the Dyck diagram, and ρ(kj)\rho(k_{j}) is the vertical distance to the top of that column. In particular, we have ρ(kj)=g34kj\rho(k_{j})=g-\frac{3}{4}k_{j}; at first glance, it might seem natural to guess that the contribution of s=kjs=k_{j} to rP+bPr_{P}+b_{P} is g+(14kjj)g+(\frac{1}{4}k_{j}-j). Note, in particular, that this contribution is at least gg, with equality if and only if kj=4jk_{j}=4j.

While this is indeed a useful approximation it is not quite correct, as 2g4γ+1Sg,γ2g-4\gamma+1\in{\rm S}_{g,\gamma} is not realizable as a positive linear combination of k1,,knk_{1},\dots,k_{n}. The upshot of this is that it is impossible to continue inductively walking up the Dyck column indexed by kjk_{j} simply by adding monomials in f1,,fnf_{1},\dots,f_{n} to FjF_{j}, FjF_{j}^{\ast} at each stage, since no monomial in f1,,fnf_{1},\dots,f_{n} has valuation equal to 2g4γ+12g-4\gamma+1. Rather, in order to continue ascending the column indexed by kjk_{j} “past” 2g4γ+12g-4\gamma+1, it is necessary to leverage the other columns, and their inductively-constructed polynomials. We will return to this issue momentarily.

Subcase 1.2: 4γ+2s4\gamma+2\leq s and s8γ+4s\neq 8\gamma+4. In this range, ss again admits either 22 or 11 distinct irreducible decompositions with respect to k1,,knk_{1},\dots,k_{n}, depending upon whether ss belongs to {kj+1,,kn}\{k_{j^{\ast}+1},\dots,k_{n}\} or not. If s{kj+1,,kn}s\notin\{k_{j^{\ast}+1},\dots,k_{n}\}, then ss gives zero net contribution to the codimension of 𝒱𝐤\mathcal{V}_{\bf k}; so without loss of generality we may assume s=kjs=k_{j} for some j[j+1,n]j\in[j^{\ast}+1,n]. Then ss has irreducible decompositions with underlying partitions (kj)(k_{j}) and (4kj4)(4^{\frac{k_{j}}{4}}) (resp., (4γ+2,4kj(4γ+2)4)(4\gamma+2,4^{\frac{k_{j}-(4\gamma+2)}{4}})) depending upon whether kjk_{j} is divisible by 4 or not. Correspondingly, we define Fj:=fjf1kj4F_{j}:=f_{j}-f_{1}^{\frac{k_{j}}{4}} (resp., Fj:=fjfjf1kj(4γ+2)4F_{j}:=f_{j}-f_{j^{\ast}}f_{1}^{{\frac{k_{j}-(4\gamma+2)}{4}}}). We now inductively “walk” up the column of the Dyck diagram indexed by kjk_{j} following the same inductive procedure as in Subcase 1.1. To a first approximation, it is useful to imagine that every gap of Sg,γ{\rm S}_{g,\gamma} strictly greater than kjk_{j} imposes a condition that depends linearly on a previously-unseen variable, and there are ρ(kj)\rho(k_{j}) of these. The precise value of ρ(kj)\rho(k_{j}) depends on how large kjk_{j} is relative to 2g4γ+12g-4\gamma+1; writing kj=4γ+2k_{j}=4\gamma+2\ell for some 0\ell\geq 0, we have

ρ(kj)=(g3γ)δ<g4γ+m=0γ1(γm)δg4γ+2mg4γ+2m+1.\rho(k_{j})=(g-3\gamma-\ell)\delta_{\ell<g-4\gamma}+\sum_{m=0}^{\gamma-1}(\gamma-m)\delta_{g-4\gamma+2m\leq\ell\leq g-4\gamma+2m+1}.

If kjk_{j} is divisible by 4, the linear part of the condition indexed by q>kjSg,γq\in\mathbb{N}_{>k_{j}}\setminus{\rm S}_{g,\gamma} is aj,qkj4a1,q+4kja_{j,q}-\frac{k_{j}}{4}a_{1,q+4-k_{j}} as in Subcase 1.1 above; otherwise, the linear part of the condition indexed by q>kjSg,γq\in\mathbb{N}_{>k_{j}}\setminus{\rm S}_{g,\gamma} is aj,qkj(4γ+2)4a1,q+4kjaj,4γ+2+qkja_{j,q}-\frac{k_{j}-(4\gamma+2)}{4}a_{1,q+4-k_{j}}-a_{j^{\ast},4\gamma+2+q-k_{j}}. The aggregate contribution ρ(kj)+kjj\rho(k_{j})+k_{j}-j of s=kjs=k_{j} to rP+bPr_{P}+b_{P} is

(g+γ+j)δ<g4γ+m=0γ1(5γ+2mj)δg4γ+2mg4γ+2m+1g(g+\gamma+\ell-j)\delta_{\ell<g-4\gamma}+\sum_{m=0}^{\gamma-1}(5\gamma+2\ell-m-j)\delta_{g-4\gamma+2m\leq\ell\leq g-4\gamma+2m+1}\geq g

in which equality holds if and only if j=γ+mj=\gamma+\ell-m^{\ast}, where mm^{\ast} is either the unique integer for which [g4γ+2m,g4γ+2m+1]\ell\in[g-4\gamma+2m^{\ast},g-4\gamma+2m^{\ast}+1], or else m=0m^{\ast}=0.

However, just as in Subcase 1.1, the preceding argument needs to be adjusted because 2g4γ+12g-4\gamma+1 is not realizable as a positive sum of k1,,knk_{1},\dots,k_{n}, so the iterative procedure by which we walk up the column indexed by kjk_{j} needs to be adjusted to explain those conditions induced by gaps greater than 2g4γ+12g-4\gamma+1. We will implement this adjustment in a unified way across all subcases following our preliminary analysis of Subcase 1.3.

Subcase 1.3: s=8γ+4s=8\gamma+4. In this subcase, ss admits either 3 or 2 distinct irreducible decompositions with respect to k1,,knk_{1},\dots,k_{n}, depending upon whether or not ss belongs to {kj+1,,kn}\{k_{j^{\ast}+1},\dots,k_{n}\}. The underlying partitions are (42γ+1)(4^{2\gamma+1}), (4γ+2)2(4\gamma+2)^{2}, and possibly (8γ+4)(8\gamma+4), if kj=8γ+4k_{j}=8\gamma+4 for some jj. Correspondingly we set G:=fj2f12γ+1G:=f_{j^{\ast}}^{2}-f_{1}^{2\gamma+1}; and if kj=8γ+4k_{j}=8\gamma+4, we further set Fj:=fjf12γ+1F_{j}:=f_{j}-f_{1}^{2\gamma+1}. As before, we inductively walk up the column of the Dyck diagram indexed by ss, perturbing GG and FjF_{j} by monomials in f1,,fnf_{1},\dots,f_{n} at each step. The valuations of the resulting polynomials continue inscreasing until they reach 2g4γ2g-4\gamma, at which stage no further iteration is possible, as no monomial in f1,,fnf_{1},\dots,f_{n} has valuation equal to 2g4γ+12g-4\gamma+1. Nevertheless, as a heuristic it is useful to provisionally ignore this obstruction and correct for the overcounting afterwards; in this idealization, each of the (inductively perturbed versions of) GG and FjF_{j} (when s=kjs=k_{j}) would contribute ρ(8γ+4)\rho(8\gamma+4) algebraically independent conditions, with linear parts of the form 2aj,q4γ2(2γ+1)a1,q8γ2a_{j^{\ast},q-4\gamma-2}-(2\gamma+1)a_{1,q-8\gamma} and aj,q(2γ+1)a1,q8γa_{j,q}-(2\gamma+1)a_{1,q-8\gamma} for all q>8γ+4Sg,γq\in\mathbb{N}_{>8\gamma+4}\setminus{\rm S}_{g,\gamma}, respectively. The value of ρ(8γ+4)\rho(8\gamma+4) depends on how large gg is relative to γ\gamma; namely,

ρ(8γ+4)=δg6γ+2(g5γ2)+j=0γ1(g5γ1+j)δ6γ2j1<g6γ2j+1.\rho(8\gamma+4)=\delta_{g\geq 6\gamma+2}(g-5\gamma-2)+\sum_{j=0}^{\gamma-1}(g-5\gamma-1+j)\delta_{6\gamma-2j-1<g\leq 6\gamma-2j+1}.

In this idealization, when s{kj+1,,kn}s\notin\{k_{j^{\ast}+1},\dots,k_{n}\}, ss contributes g5γ1+jg-5\gamma-1+j^{\ast\ast} to rP+bPr_{P}+b_{P}. When s=kjs=k_{j} for some jj, ss contributes

2(g5γ1+j)+(8γ+4j)=2g2γ+2+2jj2g5γ1+j2(g-5\gamma-1+j^{\ast\ast})+(8\gamma+4-j)=2g-2\gamma+2+2j^{\ast\ast}-j\geq 2g-5\gamma-1+j^{\ast\ast}

to rP+bPr_{P}+b_{P}, in which the inequality is equality if and only if j=3γ+3+jj=3\gamma+3+j^{\ast\ast}.

Conditions beyond 2g4γ+12g-4\gamma+1. Because the minimal generator 2g4γ+12g-4\gamma+1 of Sg,γ{\rm S}_{g,\gamma} does not belong to 𝐤{\bf k}, no monomial in the parameterizing functions fi,i=1,,nf_{i},i=1,\dots,n has tt-valuation 2g4γ+12g-4\gamma+1. In order to continue ascending the Dyck column indexed by a given element sSg,γs\in{\rm S}_{g,\gamma} (and a pair of irreducible decompositions of ss, that we fix at the outset) “beyond” 2g4γ+12g-4\gamma+1, we perturb the inductively-constructed polynomial FsF^{s} of valuation 2g4γ2g-4\gamma by (any) one of the inductively-constructed polynomials FsF^{s^{\prime}} of valuation 2g4γ2g-4\gamma from a column labeled by a distinct element sSg,γs^{\prime}\in{\rm S}_{g,\gamma}. More precisely, we replace FsF^{s} by FsFsF^{s}-F^{s^{\prime}} and then continue our iterative process just as before, increasing the valuation of our polynomial by adding scalar multiples of monomials in f1,,fnf_{1},\dots,f_{n} at each step. When we do so for every column labeled by some sSg,γs\in{\rm S}_{g,\gamma} that admits at least two irreducible decompositions, the net effect is that the lower bound on the codimension predicted by our naive idealization drops by ρ(2g4γ+1)=γ\rho(2g-4\gamma+1)=\gamma; cf. Theorem 3.8 and its proof below.

Minimizing the total number of conditions.

Case 2: 𝐤{\bf k} contains odd entries. Our analysis of conditions imposed by elements sSg,γs\in{\rm S}_{g,\gamma} is identical to that in Case 1 whenever ss is even or strictly less than the minimal odd valuation kj^k_{\widehat{j}}. Note that kj^2g4γ+1k_{\widehat{j}}\geq 2g-4\gamma+1, and clearly 2g4γ+1>4γ+22g-4\gamma+1>4\gamma+2 because g4γ+2g\geq 4\gamma+2. The element s=kj^s=k_{\widehat{j}} contributes kj^j^k_{\widehat{j}}-\widehat{j} algebraically independent ramification conditions to rP+bPr_{P}+b_{P}. Note that kj^j^gγk_{\widehat{j}}-\widehat{j}\geq g-\gamma, with equality if and only if kj^=2g4γ+1k_{\widehat{j}}=2g-4\gamma+1 and 𝐤{\bf k} includes all positive elements of Sg,γ{\rm S}_{g,\gamma} less than or equal to 2g4γ+12g-4\gamma+1. On the other hand, whenever s>kj^s>k_{\widehat{j}} and ss is odd, ss admits either 2 or 1 irreducible decompositions with respect to k1,,knk_{1},\dots,k_{n}, depending upon whether or not s=kjs=k_{j} for some jj. Once more, we may suppose without loss of generality that s=kjs=k_{j}; then ss contributes ρ(kj)+kjj\rho(k_{j})+k_{j}-j algebraically independent conditions to rP+bPr_{P}+b_{P}. By virtually the same argument as before, the total number of conditions arising from the parameterization is minimized when the valuation entries kjk_{j} determine a consecutive sequence of elements in Sg,γ{\rm S}_{g,\gamma}, with the caveat that the unique element s=8γ+4s=8\gamma+4 eligible to admit 3 irreducible decompositions might be skipped. Given an odd valuation kj=2g4γ+1+4k_{j}=2g-4\gamma+1+4\ell, where [0,γ1]\ell\in[0,\gamma-1], we have ρ(kj)=γ\rho(k_{j})=\gamma-\ell and therefore

ρ(kj)+kjj=2g3γ+1+3jg\rho(k_{j})+k_{j}-j=2g-3\gamma+1+3\ell-j\geq g

with equality if and only if j=g3γ+1+3j=g-3\gamma+1+3\ell, which means precisely that 𝐤{\bf k} includes all positive elements of Sg,γ{\rm S}_{g,\gamma} less than or equal to 2g4γ+1+42g-4\gamma+1+4\ell.

Aggregating codimension-minimizing conditions. When n3γ+1n\leq 3\gamma+1, every entry kjk_{j} of 𝐤{\bf k} is strictly smaller than 8γ+48\gamma+4. Accordingly, we see that cod(𝒱Sg,γ,Mdn){\rm cod}(\mathcal{V}_{{\rm S}_{g,\gamma}},M^{n}_{d}) is at least

(n2)g+3+(4γ+2n)+(g5γ1+j)γ1=(n1)g(2γ+n3j) if nγ; and (n2)g+3+(4γ+2(γ+1))+(g5γ1+j)γ1=(n1)g(3γ2j) if γ+1n3γ+1.\begin{split}(n-2)g+3+(4\gamma+2-n)+(g-5\gamma-1+j^{\ast\ast})-\gamma-1=(n-1)g-(2\gamma+n-3-j^{\ast\ast})\\ \text{ if }n\leq\gamma;\text{ and }\\ (n-2)g+3+(4\gamma+2-(\gamma+1))+(g-5\gamma-1+j^{\ast\ast})-\gamma-1=(n-1)g-(3\gamma-2-j^{\ast\ast})\\ \text{ if }\gamma+1\leq n\leq 3\gamma+1.\end{split}

But, if n3γ+2n\geq 3\gamma+2, cod(𝒱Sg,γ,Mdn){\rm cod}(\mathcal{V}_{{\rm S}_{g,\gamma}},M^{n}_{d}) is bounded below

(n3)g+3+(4γ+2(γ+1))+(2g5γ1+j)γ1=(n1)g(3γ2j), if kj=8γ+4 for some j.\begin{split}(n-3)g+3+(4\gamma+2-(\gamma+1))+(2g-5\gamma-1+j^{\ast\ast})-\gamma-1=(n-1)g-(3\gamma-2-j^{\ast\ast}),\\ \text{ if }k_{j}=8\gamma+4\text{ for some }j.\end{split}

We conclude that, whenever nγ+1n\geq\gamma+1,

cod(𝒱Sg,γ,Mdn)(n1)g(3γ2j).{\rm cod}(\mathcal{V}_{{\rm S}_{g,\gamma}},M^{n}_{d})\geq(n-1)g-(3\gamma-2-j^{\ast\ast}).

.

Example 3.5.

Let n=4n=4, g=11g=11, and γ=2\gamma=2, so that S=4,10,15{\rm S}=\langle 4,10,15\rangle is the corresponding γ\gamma-hyperelliptic semigroup of maximal weight; we will show that when 𝐤{\bf k} is chosen in such a way to minimize the number of conditions in Theorem 3.1, these conditions are in fact exhaustive. To this end, let f=(f2,f4,f5,f6)f=(f_{2},f_{4},f_{5},f_{6}) denote a general element of 𝒱(4,8,10,12)\mathcal{V}_{(4,8,10,12)}, where [ti]fj=aj,i[t^{i}]f_{j}=a_{j,i}; and let FF denote an arbitrary element of [f1,f2,f3,f4]\mathbb{C}[f_{1},f_{2},f_{3},f_{4}]. Without loss of generality we may assume, as in Example 2.3, that vt(F)4v_{t}(F)\geq 4. We then have

F\displaystyle F =α(4)f4+α(2,2)f22\displaystyle=\alpha_{(4)}f_{4}+\alpha_{(2,2)}f_{2}^{2}
+α(5)f5\displaystyle\ +\alpha_{(5)}f_{5}
+α(6)f6+α(4,2)f2f4+α(23)f23\displaystyle\ +\alpha_{(6)}f_{6}+\alpha_{(4,2)}f_{2}f_{4}+\alpha_{(2^{3})}f_{2}^{3}
+α(5,2)f2f5\displaystyle\ +\alpha_{(5,2)}f_{2}f_{5}
+α(24)f24+α(4,22)f22f4+α(42)f42+α(6,2)f2f6\displaystyle\ +\alpha_{(2^{4})}f_{2}^{4}+\alpha_{(4,2^{2})}f_{2}^{2}f_{4}+\alpha_{(4^{2})}f_{4}^{2}+\alpha_{(6,2)}f_{2}f_{6}
+α(5,22)f22f5+α(5,4)f4f5\displaystyle\ +\alpha_{(5,2^{2})}f_{2}^{2}f_{5}+\alpha_{(5,4)}f_{4}f_{5}
+α(25)f25+α(4,23)f23f4+α(6,4)f4f6+α(52)f52+α(6,22)f22f6+α(42,2)f2f42\displaystyle\ +\alpha_{(2^{5})}f_{2}^{5}+\alpha_{(4,2^{3})}f_{2}^{3}f_{4}+\alpha_{(6,4)}f_{4}f_{6}+\alpha_{(5^{2})}f_{5}^{2}+\alpha_{(6,2^{2})}f_{2}^{2}f_{6}+\alpha_{(4^{2},2)}f_{2}f_{4}^{2}

in which the αλ\alpha_{\lambda} are complex coefficients and the iith line in the above diagram corresponds to the homogeneous component of FF of fixed valuation 2i<2g2i<2g.

Expanding FF as a power series in tt, grouping terms of fixed valuation together, and implementing the method already applied in Example  2.3 and Lemma 2.4, we obtain

F=ψs1t4s3+ϕst4s2+ψst4s1+ϕs+1t4s+ψs+1t4s+1+O(t4s+2)F=\psi_{s-1}t^{4s-3}+\phi_{s}t^{4s-2}+\psi_{s}t^{4s-1}+\phi_{s+1}t^{4s}+\psi_{s+1}t^{4s+1}+O(t^{4s+2})

at step s>3s>3, and set ϕs=ψs=ϕs+1=0\phi_{s}=\psi_{s}=\phi_{s+1}=0, which in turn allows us to rewrite ψs+1\psi_{s+1} as a linear combination of polynomials in the coefficients of the parameterizing functions fif_{i}.

By requiring FF to vanish to higher and higher order and recording the polynomials GiG_{i} obtained at each step, we build the following table, in which the multipliers c1c_{1}, c2c_{2} and c3c_{3} are polynomials in the ai,ja_{i,j}, and GG- and HH-polynomials reference the decomposition F=G+HF=G+H, where

G=α(4)f4+α(22)f22+α(5)f5+α(6)f6+α(23)f23+α(5,2)f2f5+α(24)f24+α(25)f25+α(52)f52.G=\alpha_{(4)}f_{4}+\alpha_{(2^{2})}f_{2}^{2}+\alpha_{(5)}f_{5}+\alpha_{(6)}f_{6}+\alpha_{(2^{3})}f_{2}^{3}+\alpha_{(5,2)}f_{2}f_{5}+\alpha_{(2^{4})}f_{2}^{4}+\alpha_{(2^{5})}f_{2}^{5}+\alpha_{(5^{2})}f_{5}^{2}.
G-polynomials H-polynomials
Gap α(4)\alpha_{(4)} α(6)\alpha_{(6)} α(52)\alpha_{(5^{2})} α(4,2)\alpha_{(4,2)} α(6,2)\alpha_{(6,2)} α(42)\alpha_{(4^{2})} α(5,4)\alpha_{(5,4)}
9 G1G_{1}
11 G2G_{2}
13 G3G_{3} G4G_{4} G1G_{1}
17 G5G_{5} G3G_{3} G4G_{4}
21 G6+c1G7G_{6}+c_{1}G_{7} G7G_{7} G5G_{5} c2G7c_{2}G_{7} c3G7c_{3}G_{7}
Table 2. GG- and HH-polynimials for γ\gamma-hyperelliptic cusps

Much as in the hyperelliptic case, the algebra generated by the GG-polynomials in this example is precisely that generated by the polynomials FF and FF^{\ast} distinguished by the inductive process of Theorem 3.1; see Figure 2 for a graphical representation. Inasmuch as every numerical semigroup S{\rm S} is γ\gamma-hyperelliptic for some γ\gamma, it seems natural to speculate that an analogous phenomenon persists for arbitrary S{\rm S}.

Refer to caption
Figure 2. Conditions contributing to bPb_{P} and rPr_{P} for Sg,γ{\rm S}_{g,\gamma} when g=11g=11, γ=2\gamma=2, and n=4n=4. The dark red boxes do not contribute, i.e., they correspond to a correction to account for the fact that 2g4γ+1Span(𝐤)2g-4\gamma+1\notin\rm{Span}({\bf k}). In this case γ=1\gamma^{\ast\ast}=1.

In order to make this precise, we require one additional device, which will correct for possible “syzygetic” redundancies among the polynomials FF and FF^{\ast} that will lead to over-counting otherwise. Namely, let s1<<sps_{1}<\dots<s_{p} denote the nonzero elements of S{\rm S} strictly less than the conductor, and let {(knmj,n,,k1mj,1):j=1,,ψ(si)}\{(k_{n}^{m_{j,n}},\dots,k_{1}^{m_{j,1}}):j=1,\dots,\psi(s_{i})\} denote the set of partitions underlying irreducible decompositions of sis_{i}, i=1,,pi=1,\dots,p. For each sis_{i}, let vsi,j:=(mj,n,,mj,1)v_{s_{i},j}:=(m_{j,n},\dots,m_{j,1}) denote the exponent vector of the jjth indexing partition, j=1,,ψ(si)j=1,\dots,\psi(s_{i}). Let V=V(E)V=V(E) denote the vector matroid on

E:={vs1,2vs1,1,,vs1,ψ(s1)vs1,1;;vsp,2vsp,1,,vsp,ψ(sp)vsp,1}.E:=\{v_{s_{1},2}-v_{s_{1},1},\ldots,v_{s_{1},\psi(s_{1})}-v_{s_{1},1};\,\ldots\ \ldots\,;v_{s_{p},2}-v_{s_{p},1},\ldots,v_{s_{p},\psi(s_{p})}-v_{s_{p},1}\}.

Denote the circuits of VV by C1,,CqC_{1},\ldots,C_{q} and for each i=1,,qi=1,\dots,q, let s(i)s(i) be the largest semigroup element among s1,,sps_{1},\dots,s_{p} for which vs(i),jvs(i),1Civ_{s(i),j}-v_{s(i),1}\in C_{i} for some jj. The syzygetic defect of ff with respect to 𝐤{\bf k} is

D(𝐤):=i=1qρ(s(i)).D({\bf k}):=\sum_{i=1}^{q}\rho(s(i)).

Finally, given sSs\in{\rm S}, let ρ(s):=#{r>s:rS}\rho(s):=\#\{r>s:r\not\in{\rm S}\}, let ψ(s)\psi(s) denote the number of irreducible decompositions with respect to (k1,,kn)(k_{1},\dots,k_{n}), and let φ(s):=max(ψ(s)1,0)\varphi(s):=\max(\psi(s)-1,0). We always assume the ramification profile 𝐤=(0,k1,,kn){\bf k}=(0,k_{1},\dots,k_{n}) in the cusp is fixed in advance.

Conjecture 3.6.

Given a vector 𝐤=(0,k1,,kn)0n+1{\bf k}=(0,k_{1},\ldots,k_{n})\in\mathbb{N}_{\geq 0}^{n+1}, let 𝒱𝐤Md,g;Sn\mathcal{V}_{\bf k}\subset M^{n}_{d,g;{\rm S}} denote the subvariety parameterizing maps f:1nf:\mathbb{P}^{1}\rightarrow\mathbb{P}^{n} with a unique cusp with semigroup S{\rm S} and ramification profile 𝐤{\bf k}. Let {si}i=1\{s_{i}^{\ast}\}_{i=1}^{\ell} denote the set of minimal generators of S{\rm S} strictly less than the conductor that do not appear as entries of 𝐤{\bf k}; let m=min(,sSφ(s))m=\min(\ell,\sum_{s\in{\rm S}}\varphi(s)); and suppose d=deg(f)max(n,2g2)d=\deg(f)\geq\max(n,2g-2). Then

(14) cod(𝒱𝐤,Mdn)=i=1n(kii)+sS[2g]φ(s)ρ(s)i=1mρ(si)D(𝐤)1.{\rm cod}(\mathcal{V}_{\bf k},M^{n}_{d})=\sum_{i=1}^{n}(k_{i}-i)+\sum_{s\in{\rm S}\cap[2g]}\varphi(s)\rho(s)-\sum_{i=1}^{m}\rho(s^{\ast}_{i})-D({\bf k})-1.
Remark 3.7.

Certifying whether 𝒱𝐤\mathcal{V}_{\bf{k}} is nonempty in general is slightly delicate, inasmuch as it amounts to the assertion that the value semigroup of a general parameterization with ramification profile 𝐤\bf{k} contains every element of the underlying value semigroup 𝐒{\bf S}. On the other hand, whenever 𝒱𝐤\mathcal{V}_{\bf{k}} is nonempty, establishing that its codimension inside MdnM^{n}_{d} is at least the value predicted by the right-hand side of (14) is relatively straightforward.

Theorem 3.8.

With notation and hypotheses as in Conjecture 3.6, we have

(15) cod(𝒱𝐤,Mdn)i=1n(kii)+sS[2g]φ(s)ρ(s)i=1mρ(si)D(𝐤)1{\rm cod}(\mathcal{V}_{\bf k},M^{n}_{d})\geq\sum_{i=1}^{n}(k_{i}-i)+\sum_{s\in{\rm S}\cap[2g]}\varphi(s)\rho(s)-\sum_{i=1}^{m}\rho(s^{\ast}_{i})-D({\bf k})-1

whenever 𝒱𝐤\mathcal{V}_{\bf k} is nonempty.

Proof.

The argument closely follows that used in proving Theorem 3.1. We start by treating the special case in which every minimal generator belongs to 𝐤{\bf k}. Accordingly, let ff denote the “universal” parameterization of 𝒱𝐤\mathcal{V}_{\bf k}, represented by parameterizing functions fi=tki+ai,ki+1tki+1+O(tki+2)f_{i}=t^{k_{i}}+a_{i,k_{i+1}}t^{k_{i}+1}+O(t^{k_{i}+2}), i=1,,ni=1,\dots,n. Given sSs\in{\rm S}, first assume that s+1Ss+1\in\mathbb{N}\setminus{\rm S}. Given any two partitions (knmn,,k1m1)(k_{n}^{m_{n}},\dots,k_{1}^{m_{1}}) and (knmn,,k1m1)(k_{n}^{m_{n}^{\prime}},\dots,k_{1}^{m_{1}^{\prime}}) underlying distinct irreducible decompositions of ss, the binomial F:=i=1nfimii=1fimiF:=\prod_{i=1}^{n}f_{i}^{m_{i}}-\prod_{i=1}f_{i}^{m_{i}^{\prime}} imposes a nontrivial condition on the coefficients of ff, namely that

(16) lc(F)=i(mimi)ai,ki+1=0\text{lc}(F)=\sum_{i}(m_{i}-m_{i}^{\prime})a_{i,k_{i+1}}=0

where lc(F)\text{lc}(F) denotes the leading coefficient of FF. Similarly, if s+1Ss+1\in{\rm S}, choose an irreducible decomposition (knmn′′,,k1m1′′)(k_{n}^{m_{n}^{\prime\prime}},\dots,k_{1}^{m_{1}^{\prime\prime}}) of s+1s+1, and set

F(1):=Flc(F)i=1nfimi′′=Fi(mimi)ai,ki+1i=1nfimi′′.F^{(1)}:=F-\text{lc}(F)\prod_{i=1}^{n}f_{i}^{m_{i}^{\prime\prime}}=F-\sum_{i}(m_{i}-m_{i}^{\prime})a_{i,k_{i+1}}\prod_{i=1}^{n}f_{i}^{m_{i}^{\prime\prime}}.

The crucial point is that

lc(F(1))=i(mimi)ai,ki+2+Q1\text{lc}(F^{(1)})=\sum_{i}(m_{i}-m_{i}^{\prime})a_{i,k_{i+2}}+Q_{1}

where the quadratic term Q1Q_{1} is nonlinear in the parameterizing coefficients ai,ja_{i,j}, and will be irrelevant for our purposes. Indeed, if s+2Ss+2\in\mathbb{N}\setminus{\rm S}, we obtain a condition, namely lc(F(1))=0\text{lc}(F^{(1)})=0, whose linear part closely resembles (16) and involves as-yet unseen variables, namely ai,ki+2a_{i,k_{i+2}}; if not, we choose an irreducible decomposition (knmn′′′,,k1m1′′′)(k_{n}^{m_{n}^{\prime\prime\prime}},\dots,k_{1}^{m_{1}^{\prime\prime\prime}}) of s+2s+2, and set F(2):=F(1)lc(F(1))i=1nfimi′′′F^{(2)}:=F^{(1)}-\text{lc}(F^{(1)})\prod_{i=1}^{n}f_{i}^{m_{i}^{\prime\prime\prime}}. Continuing in this way, we inductively walk up the column indexed by ss in the Dyck diagram associated with the pair (S,f)({\rm S},f), in the process recording the linear parts of the conditions associated with each of the elements of S\mathbb{N}\setminus{\rm S} strictly larger than ss.

Note that these linear parts depend only on the pair of irreducible decompositions of ss we singled out at the outset. Moreover, if they are linearly independent, then their associated nonlinear conditions are algebraically independent. To push this logic further, let {(knmi,n,,k1mi,1):i=1,,ψ(s)}\{(k_{n}^{m_{i,n}},\dots,k_{1}^{m_{i,1}}):i=1,\dots,\psi(s)\} denote the set of partitions underlying irreducible decompositions of ss, and let vs,j:=(mj,1,,mj,n)v_{s,j}:=(m_{j,1},\dots,m_{j,n}) denote the jjth exponent vector, j=1,,ψ(s)j=1,\dots,\psi(s). We now fix a choice of reference exponent vector vs,1v_{s,1}. Each difference vs,jvs,1v_{s,j}-v_{s,1}, j1j\neq 1 indexes an initial pair of irreducible decompositions of ss, and is associated with ρ(s)\rho(s) conditions encountered while inductively walking up the column of the Dyck diagram indexed by ss. Let V(s)V(s) denote the span of the vectors vs,jvs,1v_{s,j}-v_{s,1}, 2jψ(s)2\leq j\leq\psi(s).

Now let s1<<sps_{1}<\dots<s_{p} denote the nonzero elements of S{\rm S} strictly less than the conductor, and let VS:=i=1pV(si)V_{\rm S}:=\sum_{i=1}^{p}V(s_{i}). The set of circuits of the vector matroid VV referenced in the statement of Conjecture 3.6 indexes a minimal set of linear dependencies among elements of VSV_{\rm S}. As a result, the output of our inductive procedure includes ρ(s(i))\rho(s(i)) redundant linear expressions in the parameterizing coefficients associated with the maximal semigroup element s(i)s(i) implicated in a given circuit CiC_{i}; and the total number of linearly independent expressions is precisely sSφ(s)ρ(s)D(𝐤)\sum_{s\in{\rm S}}\varphi(s)\rho(s)-D({\bf k}).

To modify the above argument in the presence of minimal generators si𝐤s_{i}^{\ast}\notin{\bf k}, we proceed as follows. Fix a nonzero element sSs\in{\rm S} for which φ(s)>0\varphi(s)>0. Fix the reference irreducible decomposition indexed by vs,1v_{s,1} as above; let s(1)s^{(1)} denote the largest element in S{\rm S} that belongs to Span(𝐤)\text{Span}({\bf k}) yet is less than s1s_{1}^{\ast}; and let Fvs,js(1)F^{s^{(1)}}_{v_{s,j}}, j=2,,ψ(s)j=2,\dots,\psi(s) denote the polynomial with tt-valuation s(1)s^{(1)} inductively constructed in the inductive “column-walking” process associated with the decomposition of ss labeled by vs,jv_{s,j}. If φ(s)=1\varphi(s)=1, there is a single inductive process, labeled by vs,2v_{s,2}, and it terminates. Otherwise, for j=3,,ψ(s)j=3,\dots,\psi(s) we set Gvs,j:=Fvs,js(1)Fvs,2s(1)G_{v_{s,j}}:=F^{s^{(1)}}_{v_{s,j}}-F^{s^{(1)}}_{v_{s,2}}. We are now left with φ(s)1\varphi(s)-1 inductive column-walking processes operative in column ss, whose associated linear conditions are the linear parts of the coefficients of Gvs,jG_{v_{s,j}}, j=3,,ψ(s)j=3,\dots,\psi(s) of terms with tt-valuation greater than s(1)s^{(1)}. For each of these processes, we continue ascending the column indexed by ss, perturbing by monomials in f1,,fnf_{1},\dots,f_{n} at each step until either the column is exhausted, or else we produce polynomials Gvs,js(2)G^{s^{(2)}}_{v_{s,j}} with tt-valuation equal to the largest element s(2)Ss^{(2)}\in{\rm S} that belongs to Span(𝐤s1)\text{Span}({\bf k}\sqcup s_{1}^{\ast}) yet is less than s2s_{2}^{\ast}. If φ(s)=2\varphi(s)=2, our unique inductive process terminates. Otherwise, for j=4,,ψ(s)j=4,\dots,\psi(s) we set Hvs,j:=Gvs,jFvs,3s(1)H_{v_{s,j}}:=G_{v_{s,j}}-F^{s^{(1)}}_{v_{s,3}} and continue proceeding upwards. We conclude by induction on the number of minimal generators of S{\rm S} not in 𝐤{\bf k}. ∎

Example 3.9.

An instructive case is that of S=8,10,12;25,29{\rm S}=\langle 8,10,12;25,29\rangle and 𝐤=(8,10,12){\bf k}=(8,10,12). There are precisely two nonzero elements of S[2g]{\rm S}\cap[2g] for which φ>0\varphi>0 and ρ>0\rho>0, namely s=20s=20 and s=24s=24. Theorem 3.8 predicts that the column indexed s=20s=20 (resp., n=24n=24) contributes 42=24-2=2 (resp., 21=12-1=1) conditions beyond ramification, where the corrections arise from the minimal generators 25 and 29 that do not belong to 𝐤{\bf k}. Macaulay2 [1] confirms that Conjecture 3.6 holds in this case, i.e., that the algebraic conditions produced by our iterative procedure and enumerated by Theorem 3.8 are exhaustive.

Remark 3.10.

In every case that we have computed, the exponent vectors vs,jv_{s,j}, j=1,,sj=1,\dots,s are linearly independent, and thus dimV(s)=φ(s)\dim V(s)=\varphi(s). It seems likely this is a general feature of sets of irreducible partitions with fixed size. In our context, it implies that syzygetic dependencies only occur among conditions associated with distinct columns in the Dyck diagram.

3.1. Rational curves with γ\gamma-hyperelliptic singularities of minimal weight

One immediate upshot of Theorem 3.1 is that the codimension of a Severi variety Md,g;SnM^{n}_{d,g;{\rm S}} is never unexpectedly small, i.e., strictly less than (n2)g(n-2)g, whenever S{\rm S} is equal to the γ\gamma-hyperelliptic semigroup Sg,γ{\rm S}_{g,\gamma} of maximal weight. On the other hand, in [6, Thm 2.3] we produced a particular infinite class of mapping spaces Md,g;SnM^{n}_{d,g;{\rm S}} of unexpectedly small codimension; the associated semigroups S{\rm S} are γ\gamma-hyperelliptic semigroups of minimal weight, and the projective targets of the underlying parameterizations are of dimension n8n\geq 8.

More precisely, say that S{\rm S} is a γ\gamma-hyperelliptic semigroup of minimal weight, for some γ0\gamma\geq 0. This means precisely that the associated Dyck path 𝒫\mathcal{P} is a staircase with steps of unit height and width, or equivalently, that S=Sg,γ{\rm S}={\rm S}^{\ast}_{g,\gamma}, where

Sg,γ:=2γ+2,2γ+4,,2g2γ,2g2γ+1,2g2γ+2,.{\rm S}^{\ast}_{g,\gamma}:=\langle 2\gamma+2,2\gamma+4,\dots,2g-2\gamma,2g-2\gamma+1,2g-2\gamma+2,\dots\rangle.

Our result [6, Thm 2.3] establishes that when g=3γ+4g=3\gamma+4 and n=γ+1n=\gamma+1, the minimal-ramification stratum 𝒱(2γ+2,2γ+4,,2γ+2n)Md,g;Sg,γn\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)}\subset M^{n}_{d,g;{\rm S}^{\ast}_{g,\gamma}} is unexpectedly large whenever n8n\geq 8. It is natural to ask whether fixing S=Sg,γ{\rm S}={\rm S}^{\ast}_{g,\gamma} while varying the genus gg and target dimension nn leads to other excess examples 𝒱(2γ+2,2γ+4,,2γ+2n)\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)} when nn belongs to the critical interval [3,7][3,7].

On the other hand, if nγn\leq\gamma, then 𝒱(2γ+2,2γ+4,,2γ+2n)\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)} is in fact empty; indeed, no value s[2γ+2n+2,4γ+2]s\in[2\gamma+2n+2,4\gamma+2] can be realized by a polynomial in the fif_{i}, i=1,,ni=1,\dots,n if these have valuation vector (2γ+2,2γ+4,,2γ+2n)(2\gamma+2,2\gamma+4,\dots,2\gamma+2n). Our final result handles the remaining cases, in which n[3,7]n\in[3,7] and γn1\gamma\leq n-1.

Proposition 3.11.

Assume that n2gn\leq 2g, dmax(2g2,n)d\geq\max(2g-2,n), and 3n73\leq n\leq 7.Then either 𝒱(2γ+2,2γ+4,,2γ+2n)\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)} is empty, or else

cod(𝒱(2γ+2,2γ+4,,2γ+2n),Mdn)(n2)g\text{\rm cod}(\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)},M^{n}_{d})\geq(n-2)g

with the following twenty-one exceptions:

  • n{6,7}n\in\{6,7\}, γ=5\gamma=5, and g[21,24]g\in[21,24]; or

  • n=7n=7, γ=6\gamma=6, and g[23,35]g\in[23,35].

Of these exceptions, thirteen certifiably underlie Severi varieties with excess components222As we explain below, we can check explicitly with Macaulay2 that the conditions furnished by Theorem 3.8 are in fact exhaustive in all of the exceptional cases for which either γ=5\gamma=5 or γ=6\gamma=6 and g27g\leq 27..

Proof.

In light of Theorem 2.1 and the discussion above, we may assume γ[1,n1]\gamma\in[1,n-1]. We have

(17) rP=j=2γ+12γ+nj=2nγ+(n+12)r_{P}=\sum_{j=2\gamma+1}^{2\gamma+n}j=2n\gamma+\binom{n+1}{2}

while

(18) ρ(2γ+2k)=g2γk\rho(2\gamma+2k)=g-2\gamma-k

for all k=1,,g2γk=1,\dots,g-2\gamma. Further note that the set of minimal generators less than the conductor 2g2γ2g-2\gamma and not belonging to the ramification profile is empty; ρ(s)=0\rho(s)=0 whenever s2g2γs\geq 2g-2\gamma; and for every k=1,,g2γ1k=1,\dots,g-2\gamma-1 we have

ψ(2γ+2k)=ψn,γ(γ+k;γ+1,γ+2,,γ+n)\psi(2\gamma+2k)=\psi_{n,\gamma}(\gamma+k;\gamma+1,\gamma+2,\dots,\gamma+n)

where ψn,γ(t;γ+1,γ+2,,γ+n)\psi_{n,\gamma}(t;\gamma+1,\gamma+2,\dots,\gamma+n) denotes the number of irreducible decompositions of tt with respect to γ+1,γ+2,,γ+n\gamma+1,\gamma+2,\dots,\gamma+n. Now let ψ~n,γ(t):=max(ψ(t;γ+1,γ+2,,γ+n)1,0)\widetilde{\psi}_{n,\gamma}(t):=\max(\psi(t;\gamma+1,\gamma+2,\dots,\gamma+n)-1,0). Applying Theorem 3.8 in tandem with (17) and (18), we are reduced to showing that

(19) (n2)g2nγ+(n+12)1+k=1g2γ1(g2γk)ψ~n,γ(γ+k)D(𝐤).(n-2)g\leq 2n\gamma+\binom{n+1}{2}-1+\sum_{k=1}^{g-2\gamma-1}(g-2\gamma-k)\widetilde{\psi}_{n,\gamma}(\gamma+k)-D({\bf k}).

Our basic strategy, outside of the twenty-one exceptional cases, will be to find jj values of these tt for which the associated values of ψ~n,γ(t)\widetilde{\psi}_{n,\gamma}(t) sum to at least (n2+j)(n-2+j) (and higher in cases with nonzero syzygetic defect).

Case: n=3n=3.

In light of (17), the estimate (19) follows trivially whenever g<6γ+6g<6\gamma+6; so without loss of generality, we assume g6γ+6g\geq 6\gamma+6. Note that ψ~3,γ(2γ+4)1\widetilde{\psi}_{3,\gamma}(2\gamma+4)\geq 1; indeed, 2γ+42\gamma+4 has irreducible decompositions with underlying partitions (γ+3,γ+1)(\gamma+3,\gamma+1) and (γ+2)2(\gamma+2)^{2}. The required estimate (19) follows immediately.

Case: n=4n=4.

This time, we may assume g4γ+5g\geq 4\gamma+5 without loss of generality. The estimate (19) follows from the facts that ψ~4,γ(2γ+4)1\widetilde{\psi}_{4,\gamma}(2\gamma+4)\geq 1, ψ~5,γ(2γ+5)1\widetilde{\psi}_{5,\gamma}(2\gamma+5)\geq 1, and that there are no syzygetic dependencies among the irreducible decompositions of 2γ+42\gamma+4 and 2γ+52\gamma+5 with underlying partitions (γ+2)2(\gamma+2)^{2}, (γ+3,γ+1)(\gamma+3,\gamma+1) and (γ+3,γ+2)(\gamma+3,\gamma+2), (γ+4,γ+1)(\gamma+4,\gamma+1), respectively.

Case: n=5n=5.

We may assume g103γ+143g\geq\frac{10}{3}\gamma+\frac{14}{3} without loss of generality. As a result, the right-hand side of (19) is at least

κ5(g,γ):=10γ+14+k=143γ+113(g2γk)ψ~5,γ(γ+k)D(𝐤).\kappa_{5}(g,\gamma):=10\gamma+14+\sum_{k=1}^{\lceil\frac{4}{3}\gamma+\frac{11}{3}\rceil}(g-2\gamma-k)\widetilde{\psi}_{5,\gamma}(\gamma+k)-D({\bf k}).

Obtaining the required 3g3g conditions now depends on the value of γ\gamma itself.

  • When γ=1\gamma=1, we compute κ5(g,1)3g+6\kappa_{5}(g,1)\geq 3g+6 using the facts that ψ~5,1(k+1)1\widetilde{\psi}_{5,1}(k+1)\geq 1 when k=3,4,5k=3,4,5, and that there are no syzygetic dependencies among the irreducible decompositions of 4,5, and 6 with underlying partitions (22)(2^{2}), (4)(4); (3,2)(3,2), (5)(5); and (23)(2^{3}), (6)(6), respectively.

  • When γ=2\gamma=2, we compute κ5(g,2)=3g+7\kappa_{5}(g,2)=3g+7 using the facts that ψ~5,2(k+2)=1\widetilde{\psi}_{5,2}(k+2)=1 when k=4,5,6k=4,5,6, and that there are no syzygetic dependencies among the irreducible decompositions of 6,7, and 8 with underlying partitions (32),(6)(3^{2}),(6); (4,3),(7)(4,3),(7); and (42),(5,3)(4^{2}),(5,3), respectively.

  • When γ=3\gamma=3, we compute κ5(g,3)=3g+6\kappa_{5}(g,3)=3g+6 using the facts that ψ~5,3(k+3)=1\widetilde{\psi}_{5,3}(k+3)=1 when k=5,7,8k=5,7,8, and that there are no syzygetic dependencies among the irreducible decompositions of 8,10, and 11 with underlying partitions (42),(8)(4^{2}),(8); (52),(6,4)(5^{2}),(6,4); and (6,5),(7,4)(6,5),(7,4), respectively.

  • When γ=4\gamma=4, we compute κ5(g,4)=2g+21\kappa_{5}(g,4)=2g+21 using the facts that ψ~5,4(k+4)=1\widetilde{\psi}_{5,4}(k+4)=1 when k=8,9k=8,9; in particular, we obtain the required estimate whenever g21g\leq 21. Now say g22g\geq 22. Note that ψ~5,4(14)1\widetilde{\psi}_{5,4}(14)\geq 1, and that there are no syzygetic dependencies among the irreducible decompositions of 12, 13, and 14 with underlying partitions (62),(7,5)(6^{2}),(7,5); (8,5),(7,6)(8,5),(7,6); and (9,5),(8,6)(9,5),(8,6), respectively. It follows that the right-hand side of (19) is at least κ(g,4)+(g2γ10)=3g+3\kappa(g,4)+(g-2\gamma-10)=3g+3.

Case: n=6n=6.

We may assume g3γ+5g\geq 3\gamma+5; the right-hand side of (19) is then at least

κ6(g,γ):=12γ+20+k=1γ+4(g2γk)ψ~6,γ(γ+k)D(𝐤).\kappa_{6}(g,\gamma):=12\gamma+20+\sum_{k=1}^{\gamma+4}(g-2\gamma-k)\widetilde{\psi}_{6,\gamma}(\gamma+k)-D({\bf k}).
  • When γ=1\gamma=1, we compute κ6(g,1)=4g+7\kappa_{6}(g,1)=4g+7 using the facts that ψ~6,1(k+1)=1\widetilde{\psi}_{6,1}(k+1)=1 for k=3,4k=3,4, ψ~6,1(6)=2\widetilde{\psi}_{6,1}(6)=2, and that the corresponding collection of irreducible decompositions (whose underlying partitions are (22),(4)(2^{2}),(4); (3,2),(5)(3,2),(5); and (4,2),(32),(6)(4,2),(3^{2}),(6)) has zero syzygetic defect.

  • When γ=2\gamma=2, we compute κ6(g,2)=4g+7\kappa_{6}(g,2)=4g+7 using the facts that ψ~6,2(k+2)=1\widetilde{\psi}_{6,2}(k+2)=1 for k=4,5k=4,5, ψ~6,2(8)=2\widetilde{\psi}_{6,2}(8)=2, and that the corresponding collection of irreducible decompositions (whose underlying partitions are (32),(6)(3^{2}),(6); (4,3),(7)(4,3),(7); and (42),(5,3),(8)(4^{2}),(5,3),(8)) has zero syzygetic defect.

  • When γ=3\gamma=3, we compute κ6(g,3)=3g+20\kappa_{6}(g,3)=3g+20 using the facts that ψ~6,3(k+3)=1\widetilde{\psi}_{6,3}(k+3)=1 for k=5,6,7k=5,6,7, and that the corresponding collection of irreducible decompositions (with underlying partitions (42),(8)(4^{2}),(8); (5,4),(9)(5,4),(9); and (52),(6,4)(5^{2}),(6,4)) has zero syzygetic defect. Thus we have produced at least 4g4g conditions whenever g20g\leq 20. Assume g21g\geq 21; we deduce that the right-hand side of (19) is at least 4g+64g+6 from the facts that ψ~6,3(11)=1\widetilde{\psi}_{6,3}(11)=1, and that the corresponding irreducible decompositions with underlying partitions (7,4),(6,5)(7,4),(6,5) are independent of the others already listed.

  • When γ=4\gamma=4, we use the fact that ψ~6,4(k+4)=1\widetilde{\psi}_{6,4}(k+4)=1 for k=6,8k=6,8 and that the corresponding irreducible decompositions are independent, i.e. have zero syzygetic defect, to compute κ6(g,4)=2g+38\kappa_{6}(g,4)=2g+38, which is strictly less than 4g4g if and only if g20g\geq 20. Assume g20g\geq 20; using the facts that ψ~6,4(13)=1\widetilde{\psi}_{6,4}(13)=1 and ψ~6,4(14)=2\widetilde{\psi}_{6,4}(14)=2 and that the collection of irreducible decompositions with underlying partitions (52),(10)(5^{2}),(10); (62),(7,5)(6^{2}),(7,5); (7,6),(8,5)(7,6),(8,5); and (72),(9,5),(8,6)(7^{2}),(9,5),(8,6) has zero syzygetic defect, we deduce that the right-hand side of (19) is at least κ6(g,4)+2g35=4g+3\kappa_{6}(g,4)+2g-35=4g+3.

  • When γ=5\gamma=5, we use the fact that ψ~6,5(9)=1\widetilde{\psi}_{6,5}(9)=1 to compute κ6(g,5)=g+61\kappa_{6}(g,5)=g+61, which is strictly less than 4g4g if and only if g21g\geq 21. Now assume g25g\geq 25; we will turn to the (exceptional) cases g=21,22,23,24g=21,22,23,24 in a moment. To bound the right-hand side of (19), we use the facts that ψ~6,5(15)=1\widetilde{\psi}_{6,5}(15)=1 counts (one minus) the irreducible decompositions with underlying partitions (8,7)(8,7), (9,6)(9,6); ψ~6,5(16)=2\widetilde{\psi}_{6,5}(16)=2 counts the irreducible decompositions corresponding to (10,6),(9,7),(82)(10,6),(9,7),(8^{2}); ψ~6,5(17)=2\widetilde{\psi}_{6,5}(17)=2 counts the irreducible decompositions corresponding to (9,8),(10,7),(11,6)(9,8),(10,7),(11,6); ψ~6,5(18)=3\widetilde{\psi}_{6,5}(18)=3 counts the irreducible decompositions corresponding to (92),(10,8),(11,7),(63)(9^{2}),(10,8),(11,7),(6^{3}); and ψ~6,5(19)=2\widetilde{\psi}_{6,5}(19)=2 counts the irreducible decompositions corresponding to (10,9),(11,8),(7,62)(10,9),(11,8),(7,6^{2}). The new wrinkle here is that the syzygetic defect is not zero; rather, there are five nontrivial linear dependencies which together account for a correction of 5g1135g-113. It follows that the right-hand side of (19) is at least 6g496g-49, which is greater than 4g4g because g25g\geq 25.

    Finally, if g=21g=21, the only irreducible decompositions that are operative are those corresponding to partitions of 15 as above; accordingly, the syzygetic defect is zero and the right-hand side of (19) becomes 2g+41=832g+41=83. Similarly, if g=22g=22, g=23g=23, or g=24g=24, we also allow for decompositions of 16, 17, and 18, and the number of syzygetic linear dependencies is one, two, or four, respectively, so the right-hand side of (19) becomes 3g+20=863g+20=86, 4g2=904g-2=90, or 5g25=955g-25=95, respectively. Calculations with Macaulay2 [1] certify that these are the actual codimensions of the corresponding loci 𝒱𝐤\mathcal{V}_{\bf k}.

Case: n=7n=7.

We may assume g145γ+275g\geq\frac{14}{5}\gamma+\frac{27}{5}; the right-hand side of (19) is then at least

κ7(g,γ):=14γ+27+k=145γ+225(g2γk)ψ~7,γ(γ+k)D(𝐤).\kappa_{7}(g,\gamma):=14\gamma+27+\sum_{k=1}^{\lceil\frac{4}{5}\gamma+\frac{22}{5}\rceil}(g-2\gamma-k)\widetilde{\psi}_{7,\gamma}(\gamma+k)-D({\bf k}).
  • When γ=1\gamma=1, we compute κ7(g,1)=4g+16\kappa_{7}(g,1)=4g+16 using the facts that ψ~7,1(k+1)=1\widetilde{\psi}_{7,1}(k+1)=1 for k=3,4,6k=3,4,6 and ψ~7,1(6)=2\widetilde{\psi}_{7,1}(6)=2, and that the corresponding irreducible decompositions with underlying partitions (22),(4)(2^{2}),(4); (3,2),(5)(3,2),(5); (22,3),(7)(2^{2},3),(7); and (32),(23),(6)(3^{2}),(2^{3}),(6) are independent. In particular, it follows that the right-hand side of (19) is at least 5g+85g+8.

  • When γ=2\gamma=2, we count much as in the γ=1\gamma=1 case. It is easy to see that ψ~7,2(k+2)=1\widetilde{\psi}_{7,2}(k+2)=1 for k=4,5k=4,5 and ψ~7,2(8)=2\widetilde{\psi}_{7,2}(8)=2, and that the corresponding collections of irreducible decompositions with underlying partitions (32),(6)(3^{2}),(6); (4,3),(7)(4,3),(7); and (42),(5,3),(8)(4^{2}),(5,3),(8) are independent. It follows that κ7(g,2)=4g+18\kappa_{7}(g,2)=4g+18, which is at least 5g5g when g18g\leq 18. On the other hand, if g19g\geq 19 we use ψ~7,2(7)=2\widetilde{\psi}_{7,2}(7)=2 and that the corresponding irreducible decompositions indexed by (33),(5,4),(9)(3^{3}),(5,4),(9) are independent of the others to conclude that the right-hand side of (19) is at least 5g+75g+7.

  • When γ=3\gamma=3, we compute κ7(g,3)=4g+20\kappa_{7}(g,3)=4g+20 using the facts that ψ~7,3(k+3)=1\widetilde{\psi}_{7,3}(k+3)=1 for k=5,6k=5,6, ψ~7,3(10)=2\widetilde{\psi}_{7,3}(10)=2, and that the corresponding collections of irreducible decompositions indexed by (42),(8)(4^{2}),(8); (5,4),(9)(5,4),(9); and (6,4),(52),(10)(6,4),(5^{2}),(10) are independent. In particular, we obtain at least 5g5g conditions whenever g20g\leq 20. If g21g\geq 21, we use ψ~7,3(8)=1\widetilde{\psi}_{7,3}(8)=1 and the fact that the irreducible decompositions (7,4),(6,5)(7,4),(6,5) are independent of the others already listed to conclude that the right-hand side of (19) is at least 5g+65g+6.

  • When γ=4\gamma=4, we compute κ7(g,4)=3g+38\kappa_{7}(g,4)=3g+38 using the facts that ψ~7,4(k+4)=1\widetilde{\psi}_{7,4}(k+4)=1 for k=6,7,8k=6,7,8 and that the corresponding collections of irreducible decompositions indexed by (52),(10)(5^{2}),(10); (6,5),(11)(6,5),(11); and (7,5),(62)(7,5),(6^{2}) are independent. Consequently, we obtain at least 5g5g conditions whenever g19g\leq 19. If g20g\geq 20, there are additional conditions arising from the irreducible decompositions indexed by (7,6),(8,5)(7,6),(8,5); and (72),(8,6),(9,5)(7^{2}),(8,6),(9,5) and counted by ψ~7,4(13)=1\widetilde{\psi}_{7,4}(13)=1 and ψ~7,4(14)=2\widetilde{\psi}_{7,4}(14)=2, respectively. These are not independent of the others; rather, there is a single linear relation, which produces a syzygetic defect of g2γ10=g18g-2\gamma-10=g-18. It follows that the right-hand side of (19) is at least 5g+35g+3.

  • When γ=5\gamma=5, we compute κ7(g,5)=2g+61\kappa_{7}(g,5)=2g+61 using the facts that ψ~7,5(k+5)=1\widetilde{\psi}_{7,5}(k+5)=1 for k=7,9k=7,9 and that the corresponding collections of irreducible decompositions indexed by (62),(12)(6^{2}),(12) and (72),(8,6)(7^{2}),(8,6) are independent. Consequently, we obtain at least 5g5g conditions whenever g20g\leq 20. Now assume g25g\geq 25. To bound the right-hand side of (19), we use the facts that ψ~7,5(15)=1\widetilde{\psi}_{7,5}(15)=1 counts irreducible decompositions indexed by (9,6),(8,7)(9,6),(8,7); ψ~7,5(16)=2\widetilde{\psi}_{7,5}(16)=2 counts irreducible decompositions indexed by (10,6),(9,7),(82)(10,6),(9,7),(8^{2}); ψ~7,5(17)=2\widetilde{\psi}_{7,5}(17)=2 counts irreducible decompositions indexed by (11,6),(10,7),(9,8)(11,6),(10,7),(9,8); ψ~7,5(18)=3\widetilde{\psi}_{7,5}(18)=3 counts irreducible decompositions indexed by (63),(11,7),(10,8),(92)(6^{3}),(11,7),(10,8),(9^{2}); and ψ~7,5(19)=2\widetilde{\psi}_{7,5}(19)=2 counts irreducible decompositions indexed by (7,62),(11,8),(10,9)(7,6^{2}),(11,8),(10,9). By the same calculation carried out previously when n=6n=6 and γ=5\gamma=5, the associated syzygetic defect is 5g1135g-113. It follows that the right-hand side of (19) is at least 7g497g-49, which is greater than 5g5g because g25g\geq 25.

    Similarly, if g=21g=21, the right-hand side of (19) becomes 3g+41=1043g+41=104; while if g=22g=22, g=23g=23, or g=24g=24, it becomes 4g+20=1084g+20=108, 5g2=1135g-2=113, or 6g25=1196g-25=119, respectively.

  • Finally, when γ=6\gamma=6, we use the fact that ψ~7,6(16)=1\widetilde{\psi}_{7,6}(16)=1 counts irreducible decompositions of 16 indexed by (9,7),(82)(9,7),(8^{2}) to compute κ7(g,6)=g+89\kappa_{7}(g,6)=g+89, which is at least 5g5g whenever g22g\leq 22. Now say g29g\geq 29. To bound the right-hand side of (19), we use the facts that ψ~7,6(17)=1\widetilde{\psi}_{7,6}(17)=1 counts irreducible decompositions indexed by (10,7)(10,7), (9,8)(9,8); ψ~7,6(18)=2\widetilde{\psi}_{7,6}(18)=2 counts irreducible decompositions indexed by (11,7)(11,7), (10,8)(10,8), (92)(9^{2}); ψ~7,6(19)=2\widetilde{\psi}_{7,6}(19)=2 counts irreducible decompositions indexed by (12,7)(12,7), (11,8)(11,8), (10,9)(10,9); ψ~7,6(20)=3\widetilde{\psi}_{7,6}(20)=3 counts irreducible decompositions indexed by (13,7)(13,7), (12,8)(12,8), (11,9)(11,9), (102)(10^{2}); ψ~7,6(21)=3\widetilde{\psi}_{7,6}(21)=3 counts irreducible decompositions indexed by (73)(7^{3}), (13,8)(13,8), (12,9)(12,9), (11,10)(11,10); ψ~7,6(22)=3\widetilde{\psi}_{7,6}(22)=3 counts irreducible decompositions indexed by (8,72)(8,7^{2}), (13,9)(13,9), (12,10)(12,10), (112)(11^{2}); and ψ~7,6(23)=2\widetilde{\psi}_{7,6}(23)=2 counts irreducible decompositions indexed by (72,9)(7^{2},9), (82,7)(8^{2},7), (13,10)(13,10), (12,11)(12,11).333In the last case, the fact that ψ~7,6(23)\widetilde{\psi}_{7,6}(23) is two less than the number of underlying partitions arises because the decomposition 8+8+7=7+7+98+8+7=7+7+9 is reducible. It is, moreover, easy to check that for every integer k[11,15]k\in[11,15], there is exactly one irreducible decomposition of k+6k+6 counted by ψ~7,6(k+6)\widetilde{\psi}_{7,6}(k+6) that is independent of the irreducible decompositions counted by ψ~7,6(10)\widetilde{\psi}_{7,6}(10), ψ~7,6(11)\widetilde{\psi}_{7,6}(11), …, ψ~7,6(k+5)\widetilde{\psi}_{7,6}(k+5). It follows that the right-hand side of (19) is at least

    κ7(g,6)+k=1115(g12k)=6g36\kappa_{7}(g,6)+\sum_{k=11}^{15}(g-12-k)=6g-36

    which is greater than 5g5g precisely when g36g\geq 36. Furthermore, it is easy to check explicitly that no irreducible decomposition of k+6k+6 counted by ψ~7,6(k+6)\widetilde{\psi}_{7,6}(k+6) is independent of the irreducible decompositions counted by ψ~7,6(10)\widetilde{\psi}_{7,6}(10), ψ~7,6(11)\widetilde{\psi}_{7,6}(11), …, ψ~7,6(k+5)\widetilde{\psi}_{7,6}(k+5) for integers k[16,22]k\in[16,22], so Conjecture 3.6 predicts that the codimension of 𝒱(14,16,,26)\mathcal{V}_{(14,16,\dots,26)} is precisely (6g36)(6g-36) for all g[29,35]g\in[29,35].

    Similarly, the right-hand side of (19) is precisely 112 when g=23g=23; 114 when g=24g=24; 117 when g=25g=25; 121 when g=26g=26; 126 when g=27g=27; and 133 when g=28g=28. Macaulay2 [1] certifies the actual codimensions of the corresponding loci 𝒱𝐤\mathcal{V}_{\bf k} whenever g27g\leq 27; we anticipate this can be pushed further with a more sophisticated implementation.

Remark 3.12.

We suspect that Conjecture 3.6 should persist for arbitrary choices of algebraically-closed base fields, in the same way that the irreducibility of the classical Severi variety of plane curves persists [4]. If true, this should be easy to verify in each instance for which Conjecture 3.6 may be checked by computer.

To close this subsection, we show how to modify the construction of [6, Thm 2.3] to obtain new infinite families of Severi varieties of unexpectedly small codimension, assuming the validity of Conjecture 3.6.

Proposition 3.13.

Let 𝒱(2γ+2,2γ+4,,2γ+2n)\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)} denote the (generic stratum of a) Severi variety with underlying value semigroup Sg,γ{\rm S}^{\ast}_{g,\gamma} as above. Now assume that n=γ+1n=\gamma+1, d2g2d\geq 2g-2, and that g=3γ+6g=3\gamma+6 (resp., g=3γ+8g=3\gamma+8) for some nonnegative integer γ5\gamma\geq 5. Assume that Conjecture 3.6 holds; then 𝒱(2γ+2,2γ+4,,2γ+2n)\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)} is of codimension 52γ2+72γ+3\frac{5}{2}\gamma^{2}+\frac{7}{2}\gamma+3 (resp., 52γ2+72γ+10\frac{5}{2}\gamma^{2}+\frac{7}{2}\gamma+10) in MdnM^{n}_{d}. In particular, 𝒱(2γ+2,2γ+4,,2γ+2n)\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)} is of codimension strictly less than (n2)g(n-2)g in MdnM^{n}_{d}.

Proof.

Assuming that Conjecture 3.6 holds, the right-hand side of (19) computes the codimension of 𝒱=𝒱(2γ+2,2γ+4,,2γ+2n)\mathcal{V}=\mathcal{V}_{(2\gamma+2,2\gamma+4,\dots,2\gamma+2n)} in MdnM^{n}_{d}.

Case: g=3γ+6g=3\gamma+6.

The right-hand side of (19) is equal to

52γ2+72γ+k=1γ+5(γ+6k)ψ~γ+1,γ(γ+k)D(𝐤).\frac{5}{2}\gamma^{2}+\frac{7}{2}\gamma+\sum_{k=1}^{\gamma+5}(\gamma+6-k)\widetilde{\psi}_{\gamma+1,\gamma}(\gamma+k)-D({\bf k}).

The desired conclusion in this case follows immediately from the facts that ψ~γ+1,γ(γ+k)=0\widetilde{\psi}_{\gamma+1,\gamma}(\gamma+k)=0 for kγ+3k\leq\gamma+3, while ψ~γ+1,γ(γ+k)=1\widetilde{\psi}_{\gamma+1,\gamma}(\gamma+k)=1 for k=γ+4,γ+5k=\gamma+4,\gamma+5. The fact that D(𝐤)=0D({\bf k})=0, in particular, is clear.

Case: g=3γ+8g=3\gamma+8.

This time, the right-hand side of (19) is equal to

52γ2+72γ+k=1γ+7(γ+8k)ψ~γ+1,γ(γ+k)D(𝐤).\frac{5}{2}\gamma^{2}+\frac{7}{2}\gamma+\sum_{k=1}^{\gamma+7}(\gamma+8-k)\widetilde{\psi}_{\gamma+1,\gamma}(\gamma+k)-D({\bf k}).

We use the facts that ψ~γ+1,γ(k)=0\widetilde{\psi}_{\gamma+1,\gamma}(k)=0 for kγ+3k\leq\gamma+3, while ψ~γ+1,γ(2γ+4)=1\widetilde{\psi}_{\gamma+1,\gamma}(2\gamma+4)=1 counts the irreducible decompositions indexed by ((γ+2)2),((γ+3),(γ+1))((\gamma+2)^{2}),((\gamma+3),(\gamma+1)); ψ~γ+1,γ(2γ+5)=1\widetilde{\psi}_{\gamma+1,\gamma}(2\gamma+5)=1 counts the irreducible decompositions indexed by ((γ+3),(γ+2)),((γ+4),(γ+1))((\gamma+3),(\gamma+2)),((\gamma+4),(\gamma+1)); ψ~γ+1,γ(2γ+6)=2\widetilde{\psi}_{\gamma+1,\gamma}(2\gamma+6)=2 counts the irreducible decompositions indexed by (γ+5,γ+1),(γ+4,γ+2),((γ+3)2)(\gamma+5,\gamma+1),(\gamma+4,\gamma+2),((\gamma+3)^{2}); and ψ~γ+1,γ(2γ+7)=2\widetilde{\psi}_{\gamma+1,\gamma}(2\gamma+7)=2 counts the irreducible decompositions indexed by (γ+6,γ+1),(γ+5,γ+2),((γ+3)2)(\gamma+6,\gamma+1),(\gamma+5,\gamma+2),((\gamma+3)^{2}). The two linear dependencies among these together account for D(𝐤)=k=γ+6γ+7(g2γk)=3D({\bf k})=\sum_{k=\gamma+6}^{\gamma+7}(g-2\gamma-k)=3, and the desired conclusion follows. ∎

The upshot of Proposition 3.13, taken together with [6, Thm 2.3], is that we expect unexpectedly large Severi varieties to exist in every genus g21g\geq 21 and every projective target dimension n6n\geq 6.

3.2. Generic cusps with ramification (2m,2m+2,,2m+2n2)(2m,2m+2,\dots,2m+2n-2), n3n\geq 3

In this subsection, we study the value semigroup Sgen{\rm S}_{\rm gen} of a generic singularity with ramification profile equal to an nn-tuple of consecutive even numbers. Whenever n4n\geq 4, we are not able to determine Sgen{\rm S}_{\rm gen} explicitly; we still manage to show, however, that its structure forces the associated Severi variety Md,g;SgennM^{n}_{d,g;{\rm S}_{\rm gen}} to be unexpectedly large in general. When n=3n=3, we are able to determine Sgen{\rm S}_{\rm gen} explicitly and show that Md,g;SgennM^{n}_{d,g;{\rm S}_{\rm gen}} is usually unexpectedly large as a result.

Theorem 3.14.

Given positive integers n4n\geq 4 and mn+1m\geq n+1, let Sgen=Sgen(m,n){\rm S}_{\rm gen}={\rm S}_{\rm gen}(m,n) denote the value semigroup of a generic cusp in n\mathbb{C}^{n} with ramification profile (2m,2m+2,,2m+2n2)(2m,2m+2,\dots,2m+2n-2). We then have

{1,,2m1}{2m+1,2m+3,,4m+3}{2m+2n,2m+2n+2,,4m2}{4m+4n5,4m+4n3,,6m+3}Ggen\begin{split}&\{1,\dots,2m-1\}\sqcup\{2m+1,2m+3,\dots,4m+3\}\sqcup\{2m+2n,2m+2n+2,\dots,4m-2\}\\ &\sqcup\{4m+4n-5,4m+4n-3,\dots,6m+3\}\subset{\rm G}_{\rm gen}\end{split}

where Ggen=Sgen{\rm G}_{\rm gen}=\mathbb{N}\setminus{\rm S}_{\rm gen} denotes the complement of Sgen{\rm S}_{\rm gen}.

Proof.

Fix a choice of generic nn-tuple of power series f(t)=(f1(t),,fn(t))f(t)=(f_{1}(t),\dots,f_{n}(t)) with ramification profile (2m,2m+2,,2m+2n2)(2m,2m+2,\dots,2m+2n-2) in t=0t=0; without loss of generality, we may assume each of the parameterizing functions fi(t)f_{i}(t) has a monic lowest-order term. The generic value semigroup Sgen{\rm S}_{\rm gen} comprises all valuations realized by polynomials in the fi(t)f_{i}(t), i=1,,ni=1,\dots,n. It follows immediately that {1,,2m1}Ggen\{1,\dots,2m-1\}\subset{\rm G}_{\rm gen}. Similarly, we have

{2m+1,2m+3,,4m+3}{2m+2n,2m+2n+2,,4m2}Ggen\{2m+1,2m+3,\dots,4m+3\}\sqcup\{2m+2n,2m+2n+2,\dots,4m-2\}\subset{\rm G}_{\rm gen}

as the minimal valuation realized by a nonlinear polynomial in the fi(t)f_{i}(t) is vt(f22f1f3)=4m+5v_{t}(f_{2}^{2}-f_{1}f_{3})=4m+5. (Note that the latter equality is a consequence of genericity.) To conclude, it suffices to see that no element belonging to {4m+4n5,4m+4n3,,6m+3}\{4m+4n-5,4m+4n-3,\dots,6m+3\} is the valuation of a quadratic polynomial in the fi(t)f_{i}(t); indeed, by genericity, the largest odd valuation realized by such a quadratic polynomial is vt(fn12fn2fn)=4m+4n7v_{t}(f_{n-1}^{2}-f_{n-2}f_{n})=4m+4n-7. ∎

For our purposes, the crucial take-away of Theorem 3.14 is the following.

Corollary 3.15.

For every pair of positive integers n4n\geq 4 and m>76n+269m>\frac{7}{6}n+\frac{26}{9}, the corresponding Severi variety Md,g;SgennM^{n}_{d,g;{\rm S}_{\rm gen}} is of codimension strictly less than (n2)g(n-2)g in MdnM^{n}_{d} whenever dgd\gg g.

Proof.

By genericity, the only conditions imposed on holomorphic maps by Sgen{\rm S}_{\rm gen} arise from ramification in the preimage PP of the cusp, and there are

rP1=i=1n(2m+2i2)1=2mn+(n12)1r_{P}-1=\sum_{i=1}^{n}(2m+2i-2)-1=2mn+\binom{n-1}{2}-1

of these. On the other hand, Theorem 3.14 implies that

g5m3n+6g\geq 5m-3n+6

where g=#Ggeng=\#{\rm G}_{\rm gen} is the delta-invariant of a generic cusp with ramification (2m,2m+2,,2m+2n2)(2m,2m+2,\dots,2m+2n-2). Accordingly, it suffices to check that

(20) 2mn+(n12)1<(n2)(5m3n+6)2mn+\binom{n-1}{2}-1<(n-2)(5m-3n+6)

and this is ensured by our numerical hypotheses on mm and nn. ∎

When n=3n=3, we have to work harder to produce unexpectedly large Severi varieties; indeed, the inequality (20) never holds. To do so, we exploit a natural connection between generators of Sgen{\rm S}_{\rm gen} and solutions to linear diophantine equations that is particular to the n=3n=3 case.

Theorem 3.16.

For every positive integer mm, the value semigroup Sgen{\rm S}_{\rm gen} of a generic parameterization with ramification profile (2m,2m+2,2m+4)(2m,2m+2,2m+4) is equal to S0=2m,2m+2,2m+4,4m+5,(m+2)m+1{\rm S}^{0}=\langle 2m,2m+2,2m+4,4m+5,(m+2)m+1\rangle (resp., S1=2m,2m+2,2m+4,4m+5,(m+3)m+1{\rm S}^{1}=\langle 2m,2m+2,2m+4,4m+5,(m+3)m+1\rangle) if mm is even (resp., odd). In particular, Sgen{\rm S}_{\rm gen} is of genus 12m2+2m1\frac{1}{2}m^{2}+2m-1 (resp.,12m2+2m32\frac{1}{2}m^{2}+2m-\frac{3}{2}) if mm is even (resp., odd).

Proof.

Let f=(f1,f2,f3)f=(f_{1},f_{2},f_{3}) denote a generic power series map with ramification profile (2m,2m+2,2m+4)(2m,2m+2,2m+4) in t=0t=0; then fi=fi(t)f_{i}=f_{i}(t) is a power series with tt-adic valuation vi=2m+2i2v_{i}=2m+2i-2, i=1,2,3i=1,2,3. Now assume that mm is even. We begin by showing that S0Sgen{\rm S}^{0}\subset{\rm S}_{\rm gen}. Without loss of generality, assume that each fif_{i} has a monic term of lowest order. Genericity then implies that vt(f22f1f3)=4m+5v_{t}(f_{2}^{2}-f_{1}f_{3})=4m+5 belongs to Sgen{\rm S}_{\rm gen}. That is to say, the fact that 4m+5Sgen4m+5\in{\rm S}_{\rm gen} arises because the diophantine equation ma+(m+2)b=(m+1)cma+(m+2)b=(m+1)c admits a triple of nonnegative solutions (a,b,c)=(1,1,2)(a,b,c)=(1,1,2). Similarly, the diophantine equation ma+(m+1)b=(m+2)cma+(m+1)b=(m+2)c admits nonnegative solutions (a,b,c)=(m2+1,0,m2)(a,b,c)=(\frac{m}{2}+1,0,\frac{m}{2}), which implies that vt(f1m2+1f3m2)=m(m+2)+1v_{t}(f_{1}^{\frac{m}{2}+1}-f_{3}^{\frac{m}{2}})=m(m+2)+1 belongs to Sgen{\rm S}_{\rm gen}. It follows that S0Sgen{\rm S}^{0}\subset{\rm S}_{\rm gen}.

Note that the gap set G0=S0{\rm G}^{0}=\mathbb{N}\setminus{\rm S}^{0} is given by

G0={1,,2m1}{2m+1,2m+3,,4m+3}i=1m212{im+2i+1,,(i+1)m1}i=1m22{2(i+1)m+2(2i+1)+1,2(i+1)m+2(2i+1)+3,,2(i+2)m+3}{m2+2m1}.\begin{split}{\rm G}^{0}&=\{1,\dots,2m-1\}\bigsqcup\{2m+1,2m+3,\dots,4m+3\}\bigsqcup\bigsqcup_{i=1}^{\frac{m}{2}-1}2\{im+2i+1,\dots,(i+1)m-1\}\\ &\bigsqcup\bigsqcup_{i=1}^{\frac{m}{2}-2}\{2(i+1)m+2(2i+1)+1,2(i+1)m+2(2i+1)+3,\dots,2(i+2)m+3\}\bigsqcup\{m^{2}+2m-1\}.\end{split}

We now claim that no element gG0g\in{\rm G}^{0} is the valuation vv of a polynomial in the parameterizing functions fif_{i}, i=1,2,3i=1,2,3. Indeed, this is clear for every g{1,,2m1}g\in\{1,\dots,2m-1\}, as every such gg is strictly less than every viv_{i}; as well as for every g{2m+1,2m+3,,4m+3}g\in\{2m+1,2m+3,\dots,4m+3\}, since by construction 4m+54m+5 is the minimally realizable odd valuation. Similarly, our construction shows that each of the remaining elements gg, if equal to the valuation of a polynomial in the fif_{i}, is necessarily the valuation of the sum of at most two monomials in the fif_{i} (since there are no “triple ties” among valuations of monomials in this range). Moreover, since no gg belongs to 2m,2m+2,2m+4\langle 2m,2m+2,2m+4\rangle, this means that any realizable gg is necessarily the valuation of the sum of two monomials with equal valuation vv. Genericity of the fif_{i} then forces gg to be v+1v+1, where vv is a multiple of 4m+44m+4; as no gg fits this description, it follows that Sgen=S0{\rm S}_{\rm gen}={\rm S}^{0} when mm is even. As a result, Sgen{\rm S}_{\rm gen} has genus

g(m)=(2m1)+(m+2)+i=1m21(m2i1)+i=1m22(m2i+1)+1=12m2+2m1.g(m)=(2m-1)+(m+2)+\sum_{i=1}^{\frac{m}{2}-1}(m-2i-1)+\sum_{i=1}^{\frac{m}{2}-2}(m-2i+1)+1=\frac{1}{2}m^{2}+2m-1.

Assume now that mm is odd. Once again, vt(f22f1f3)=4m+5v_{t}(f_{2}^{2}-f_{1}f_{3})=4m+5 belongs to Sgen{\rm S}_{\rm gen}, as does vt(f1m+32f2f3m12)=(m+3)m+1v_{t}(f_{1}^{\frac{m+3}{2}}-f_{2}f_{3}^{\frac{m-1}{2}})=(m+3)m+1; so S1Sgen{\rm S}^{1}\subset{\rm S}_{\rm gen}. In this case the gap set G1=S1{\rm G}^{1}=\mathbb{N}\setminus{\rm S}^{1} is

G1={1,,2m1}{2m+1,2m+3,,4m+3}i=1m122{im+2i+1,,(i+1)m1}i=1m121{2(i+1)m+2(2i+1)+1,2(i+1)m+2(2i+1)+3,,2(i+2)m+3}.\begin{split}{\rm G}^{1}&=\{1,\dots,2m-1\}\bigsqcup\{2m+1,2m+3,\dots,4m+3\}\bigsqcup\bigsqcup_{i=1}^{\frac{m-1}{2}}2\{im+2i+1,\dots,(i+1)m-1\}\\ &\bigsqcup\bigsqcup_{i=1}^{\frac{m-1}{2}-1}\{2(i+1)m+2(2i+1)+1,2(i+1)m+2(2i+1)+3,\dots,2(i+2)m+3\}.\end{split}

An argument analogous to that used in the case of even mm shows that no element of G1{\rm G}^{1} is the valuation of a polynomial in the fif_{i}, which enables us to conclude that Sgen=S1{\rm S}_{\rm gen}={\rm S}^{1}. As a result, Sgen{\rm S}_{\rm gen} has genus

g(m)=(2m1)+(m+2)+i=1m12(m2i1)+i=1m121(m2i+1)=12m2+2m32.g(m)=(2m-1)+(m+2)+\sum_{i=1}^{\frac{m-1}{2}}(m-2i-1)+\sum_{i=1}^{\frac{m-1}{2}-1}(m-2i+1)=\frac{1}{2}m^{2}+2m-\frac{3}{2}.

Corollary 3.17.

For every positive integer m9m\geq 9, the corresponding Severi variety Md,g;Sgen3M^{3}_{d,g;{\rm S}_{\rm gen}} is of codimension strictly less than gg in Md3M^{3}_{d} whenever dgd\gg g.

Proof.

By genericity, the only conditions imposed on holomorphic maps 13\mathbb{P}^{1}\rightarrow\mathbb{P}^{3} of degree dd by Sgen{\rm S}_{\rm gen} arise from ramification in the preimage of the cusp; and there are rP1=6m1r_{P}-1=6m-1 of these. In light of Theorem 3.16, it therefore suffices to show that

6m1<12m2+2m326m-1<\frac{1}{2}m^{2}+2m-\frac{3}{2}

which is guaranteed by our hypothesis on mm. ∎

Remark 3.18.

We expect that the codimension estimates we have obtained for Severi varieties of rational unicuspidal curves, i.e., for linear series on 1\mathbb{P}^{1} with unicuspidal images, hold more generally for (varieties of) linear series on general curves of arbitrary genus. Indeed, to establish the algebraic independence of conditions imposed by cusps on linear series on a given smooth curve CC, it suffices to certify that certain evaluation maps from (sections of) line bundles to their associated jet bundles are surjective, and this is easy when CC is either rational or elliptic. On the other hand, when CC is general, it specializes in a flat family to a stable union C0C_{0} of rational and elliptic curves; and it is possible to explicitly relate the variety of linear series on CC to the variety of limit linear series [9] on C0C_{0}. To complete this argument, we would need a suitable generalization of the notion of “cusp” for limit linear series.

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