alphaFeedback

WorksMathematics

On OpenAI's proof of the Nagata conjecture

AI contributions
  • ChatGPT Astra
View details

Abstract

These notes are an expanded account of my talk at UMass Amherst on OpenAI's remarkably simple proof of the Nagata conjecture. I hope they will be useful, especially to non-experts. The standard reduction to the normal cone and the collision of fat points into one monomial scheme reduce the problem to interpolation of monomial schemes on the normal ruled surface of a smooth plane cubic. The novelty is that the study of the asymptotics of theta functions as the cubic develops a node, together with interpolation duality, reduces the problem further to interpolation on a triangle of lattice points, which is straightforward. The same calculation determines the nef and pseudoeffective cones of a weighted blow-up of P2{\Bbb P}^2 at one point for very general local parameters when the ratio of weights is greater than nine.

Introduction

Nagata’s conjecture grows out of the elementary Lagrange interpolation problem. We work over C\mathbb{C}. Let x1,…,xrx_1,\ldots,x_r be distinct numbers. We are looking for a polynomial f(x)f(x) with f(xi)=cif(x_i)=c_i for every ii, where c1,…,crc_1,\ldots,c_r are prescribed values. There is a unique solution of degree at most r−1r-1:

f(x)=∑i=1rci∏t≠ix−xtxi−xt.f(x)=\sum_{i=1}^{r}c_i\prod_{t\ne i}\frac{x-x_t}{x_i-x_t}.

The following lemma generalizes Lagrange interpolation. It will be used in subsequent sections.

Lemma 1.1. Let S⊂C2S\subset\mathbb{C}^{2} be a finite set of points lying on distinct horizontal lines y=β0,…,y=βsy=\beta_0,\ldots,y=\beta_s, with NiN_i points on row ii. Number the rows so that N0≥⋯≥Ns>0N_0\ge\cdots\ge N_s>0. Set

I={(a,b)∈Z≥02:0≤b≤s, 0≤a<Nb},VI=Span⁡C{xayb:(a,b)∈I}.(1)I=\{(a,b)\in\mathbb{Z}_{\ge0}^{2}:0\le b\le s,\ 0\le a<N_b\},\qquad V_I=\operatorname{Span}_{\mathbb{C}}\{x^a y^b:(a,b)\in I\}. \tag*{(1)}

The set II is a Young diagram. Its rows, counted from the bottom, have lengths N0,…,NsN_0,\ldots,N_s. For any prescribed values on SS, there is a unique polynomial F(x,y)∈VIF(x,y)\in V_I taking those values.

Points S and Young diagram I

Figure 7.

Proof. Put Qi(y)=∏0≤t<i(y−βt)Q_i(y)=\prod_{0\leq t<i}(y-\beta_t) for 0≤i≤s0\leq i\leq s, so that Q0=1Q_0=1. We construct an interpolating polynomial of the form F=∑i=0sQi(y)hi(x)F=\sum_{i=0}^{s}Q_i(y)h_i(x) by choosing h0,…,hsh_0,\ldots,h_s successively with deg⁡hi<Ni\deg h_i<N_i. Adding Qi(y)hi(x)Q_i(y)h_i(x) preserves the values on rows labeled 0,…,i−10,\ldots,i-1, since QiQ_i vanishes there. On row ii, the nonzero factor Qi(βi)Q_i(\beta_i) reduces the remaining conditions to Lagrange interpolation in xx at NiN_i distinct first coordinates, determining hih_i uniquely. The polynomials xaQi(y)x^aQ_i(y), 0≤a<Ni0\leq a<N_i, form a basis of VIV_I: their leading terms in yy are xayix^ay^i, and the remaining monomials are indexed by II because Nt≥NiN_t\geq N_i for 0≤t<i0\leq t<i. This proves existence and uniqueness. □\square

Given points P1,…,Pr∈C2P_1,\ldots,P_r\in\mathbb{C}^2, prescribing values F(Pi)=ciF(P_i)=c_i for a polynomial FF of degree at most dd gives a system of linear equations in its coefficients, generally inhomogeneous. We now ask whether the associated homogeneous system F(Pi)=0F(P_i)=0 has a nonzero solution. Equivalently, we seek a plane algebraic curve F(x,y)=0F(x,y)=0 passing through these points.

Five points and a plane algebraic curve passing through them

Figure 8 (PDF p. 2).

The polynomials of total degree at most dd form a vector space with basis xaybx^ay^b, where a,b≥0a,b\geq0 and a+b≤da+b\leq d. Its dimension is

D=1+2+⋯+(d+1)=(d+22).D=1+2+\cdots+(d+1)=\binom{d+2}{2}.

Each condition F(Pi)=0F(P_i)=0 is one homogeneous linear equation in the coefficients. The corresponding r×Dr\times D matrix is called the evaluation matrix; its entry in row ii and the column indexed by xaybx^ay^b is the value of the monomial xaybx^ay^b at PiP_i. If r<Dr<D, there are fewer equations than unknowns, so a nonzero solution exists for every configuration of points. The converse requires a condition on their position: arbitrarily many points can lie on a curve of fixed positive degree. To prove that this system has the largest possible rank for general points, apply Lemma 1.1 to the triangular set

S=Td={(j,k)∈Z≥02:j+k≤d}.S=T_d=\{(j,k)\in\mathbb{Z}_{\geq0}^2:j+k\leq d\}.

Its row lengths are d+1,d,…,1d+1,d,\ldots,1, so I=TdI=T_d. Thus evaluation at these D=(d+22)D=\binom{d+2}{2} points is an isomorphism on polynomials of degree at most dd. The diagrams below show d=3d=3 and D=10D=10.

Points T3 and monomials of degree at most 3

Figure 9.

The entries of the evaluation matrix are polynomials in the point coordinates. For r≤Dr \le D, choose rr points of TdT_d; for r≥Dr \ge D, add r−Dr-D distinct points to TdT_d. In either case, the evaluation matrix has rank min⁡(r,D)\min(r,D), so one of its minors of this size is nonzero. This minor remains nonzero outside the zero set of a nonzero polynomial in the point coordinates. A property that holds outside such a set is said to hold for general points. The kernel therefore has dimension max⁡(D−r,0)\max(D-r,0), proving

there is a nonzero polynomial of degree at most dd vanishing at rr general points ⟺r<(d+22)\Longleftrightarrow r < \binom{d+2}{2}.

there is a nonzero polynomial of degree at most dvanishing at r general points⟺r<(d+22).(2)\text{there is a nonzero polynomial of degree at most }d \quad\text{vanishing at }r\text{ general points} \quad\Longleftrightarrow\quad r < \binom{d+2}{2}. \tag*{(2)}

We can also prescribe values of the partial derivatives. Prescribing a function’s values and first derivatives, for example, determines the tangent planes to its graph. These are again linear conditions on the polynomial’s coefficients. As before, we study the homogeneous system of linear equations, in which the prescribed values and derivatives are zero.

Fat points. A polynomial FF vanishes to order at least mm at P=(x0,y0)P=(x_0,y_0) if

∂a+bF∂xa∂yb∣(x,y)=(x0,y0)=0(a,b≥0, a+b<m).\left.\frac{\partial^{a+b}F}{\partial x^a\partial y^b}\right|_{(x,y)=(x_0,y_0)}=0 \qquad(a,b\ge0,\ a+b<m).

The ideal (x−x0,y−y0)m⊂C[x,y](x-x_0,y-y_0)^m \subset\mathbb{C}[x,y] consists of the polynomials satisfying these conditions and defines the fat point of multiplicity mm at PP. Evaluation at this fat point records the value of the polynomial along with all of its partial derivatives of order less than mm. Equivalently, it records the class of FF in the quotient ring C[x,y]/(x−x0,y−y0)m\mathbb{C}[x,y]/(x-x_0,y-y_0)^m, which is the coordinate algebra of the fat point. This ring has dimension (m+12)\binom{m+1}{2} over C\mathbb{C}, which is called the length of the fat point. The length is equal to the number of rows a fat point contributes to the evaluation matrix.

For a second proof of (2), take the fat point of multiplicity d+1d+1 at the origin. Its length is D=(d+22)D=\binom{d+2}{2}, and evaluation on polynomials of degree at most dd is an isomorphism: it simply records all coefficients of these polynomials. By Lemma 2.1, this fat point admits a flat deformation into DD distinct points. The entries of the evaluation matrix are regular in the deformation parameter. Its determinant is nonzero at the fat point and hence remains nonzero for nearby parameters. Evaluation at the resulting DD distinct points is therefore an isomorphism. For r<Dr<D, take a subset of these points; for r>Dr>D, add distinct points. The evaluation matrix has rank min⁡(r,D)\min(r,D) in either case, and the same is true for general points by the argument with minors above.

Imposing multiplicity mm at each of rr distinct points gives r(m+12)r\binom{m+1}{2} homogeneous linear conditions on the coefficients. Thus, for every configuration of points, a nonzero polynomial of degree at most dd vanishing to the prescribed orders exists whenever

(d+22)>r(m+12).\binom{d+2}{2}>r\binom{m+1}{2}.

If this inequality fails, a nonzero solution may still exist because the equations may be linearly dependent. For fixed rr, as dd and mm grow proportionally, the leading terms are d2/2d^2/2 and rm2/2rm^2/2. This suggests d/m=rd/m=\sqrt{r} as the boundary for the existence of such curves.

Theorem A (Nagata’s conjecture [15]). Let r≥10r \ge10. For very general points p1,…,pr∈P2p_1,\ldots,p_r \in\mathbb{P}^2, every nonzero homogeneous polynomial of degree dd vanishing to order at least m≥1m \ge1 at each pip_i satisfies

d>mr.d>m\sqrt{r}.

Here very general means outside a countable union of proper algebraic subsets of the configuration space. This allows the inequality to hold for every pair of integers dd, mm at the same configuration of points. The restriction r≥10r \ge10 is necessary: nine points always lie on a nonzero cubic. Nagata proved the conjecture when rr is a square [15, 16]; see [3 §2] for its history and related questions.

Scope of these notes. I began writing these notes while preparing my talk at UMass Amherst. They are not intended as a definitive account, and I claim no originality. I have reorganized and simplified the argument by working directly on the normal ruled surface of a smooth plane cubic, without performing elementary transformations of ruled surfaces. § 3 explains interpolation duality and proves the interpolation statement on a triangle of lattice points. § 4 realizes this interpolation matrix as a limit of matrices obtained by evaluating theta functions and their derivatives. § 5 transfers the problem to the plane and proves Nagata’s conjecture. § 6 applies the same construction to monomial valuations and determines the nef and pseudoeffective cones of weighted blow-ups of P2\mathbb{P}^2 for very general local parameters, when the ratio of weights is greater than nine. I chose to follow the approach using complex geometry in [17], rather than the algebraic approach developed in the companion manuscripts [18, 19, 20], which I have not studied in detail. The former is also closer in spirit to our discussions of Nagata’s conjecture and related topics, for example [27], during the Summer REU in Algebraic Geometry at UMass Amherst.

As I read the released manuscripts [21], I wondered whether I might be their first human reader. They seemed almost entirely unedited. While it is possible that the release served solely as a benchmark demonstrating to the investors that a large language model could solve very hard problems, I suspect that the company expected that the mathematical community, either out of curiosity or out of a sense of duty to the profession, would eventually sort out these contributions. Absorbing these arguments into mainstream mathematics and assessing their impact on our field will require a considerable editorial effort from the community. This work demands expertise and time, yet brings little of the recognition associated with original research. Like many others, I believe this approach harms our profession, especially the motivation and training of young people.

At the same time, I think these manuscripts are a stunning achievement. The model managed to connect the dots and solve the problems that many of the experts thought were out of reach. I think a wholesale re-evaluation of the mathematical corpus is currently underway, with the old underbrush of mathematical conjectures rapidly being burned in the AI fire. However, it is up to the mathematical community to figure out what mathematics will look like in the future.

I hope for closer, more respectful collaboration between frontier AI companies and the academic research community. The enormous financial resources available to these companies could support a substantial, independent foundation for research in mathematics and computer science. Such a foundation could offer research grants, graduate fellowships, and access to the best frontier models, especially to young scientists pursuing their own original research. It would give the community a role in shaping this research and sharing its benefits, rather than leaving the work to opaque in-house laboratories with little accountability for its effects on the profession. I believe this investment would also benefit the AI companies themselves in the long term. The foundation could follow the National Science Foundation’s model of peer review and provide sustained support for future generations of mathematicians and computer scientists.

Acknowledgements

Acknowledgements. I am grateful to the participants in the Reading Seminar in Algebraic Geometry and 2026 Summer REU in Algebraic Geometry at UMass Amherst for many helpful discussions. This work was supported by the National Science Foundation under grant DMS-2401387. These notes were edited and illustrated with ChatGPT Astra.

Staircase interpolation

The main result of this section is Proposition 2.4, which describes a vector space of polynomials in two variables that interpolates arbitrary values on a certain triangle of lattice points. We begin by reviewing monomial schemes defined by Young diagrams and their flat deformations. We then explain the duality between interpolation on lattice points and vanishing on monomial schemes.

Let I⊂Z≥02I \subset\mathbb{Z}_{\ge0}^{2} be a Young diagram; thus II is closed under decreasing either coordinate. The monomials indexed by points of Z≥02\mathbb{Z}_{\ge0}^{2} outside II span an ideal in C[w,y]\mathbb{C}[w,y] defining the finite scheme

ZI=Spec⁡C[w,y](yawb:(a,b)∉I).(3)Z_I = \operatorname{Spec} \frac{\mathbb{C}[w,y]}{(y^a w^b : (a,b) \notin I)}. \tag*{(3)}

It is supported at the origin. Its coordinate ring has a basis consisting of yawby^a w^b, (a,b)∈I(a,b) \in I, so ZIZ_I has length ∣I∣|I|. For the triangle I=TmI = T_m, ZIZ_I is the fat point of multiplicity m+1m+1, with ideal (w,y)m+1(w,y)^{m+1}.

Lemma 2.1 ([14 Lemma 18.10]). The scheme ZIZ_I is a flat limit of ∣I∣|I| distinct points. In particular, a fat point of multiplicity mm is a flat limit of (m+12)\binom{m+1}{2} distinct points.

We will need a closely related result. For positive integers rr, mm, consider the Young diagram

I={(a,b)∈Z≥02:ra+b<rm}.I = \{(a,b) \in\mathbb{Z}_{\ge0}^{2} : ra + b < rm\}.

We will realize ZIZ_I as a flat limit of rr fat points of multiplicity mm. Let XX be a smooth irreducible complex algebraic surface, B\mathcal{B} a line bundle on XX, and W⊂H0(X,B)W \subset H^0(X,\mathcal{B}) a finite-dimensional space of sections. Choose local holomorphic coordinates (w,y)(w,y) centered at a point of XX and a local frame of B\mathcal{B} near that point. In this chart, the monomials indexed by points outside II generate the ideal

IZ=(yawb:ra+b≥rm)=(wr,y)m.(4)\mathcal{I}_Z = (y^a w^b : ra+b \ge rm) = (w^r,y)^m. \tag*{(4)}

Thus ZZ is the scheme ZIZ_I of (3) in these coordinates. Its local algebra has a basis of yawby^a w^b, (a,b)∈I(a,b) \in I, and hence

length⁡(Z)=∣I∣=∑a=0m−1r(m−a)=rm(m+1)2.\operatorname{length}(Z) = |I| = \sum_{a=0}^{m-1} r(m-a) = \frac{rm(m+1)}{2}.

Let HF(w,y)H_F(w,y) be the local representative of F∈WF \in W in the chosen frame. In the normalized basis yawba!b!\frac{y^a w^b}{a!b!}, restriction to ZZ is the jet map

J:W⟶CI,(JF)a,b=∂a+bHF∂ya∂wb∣(w,y)=(0,0).(5)J : W \longrightarrow\mathbb{C}^{I}, \qquad(JF)_{a,b} = \left.\frac{\partial^{a+b}H_F}{\partial y^a \partial w^b}\right|_{(w,y)=(0,0)}. \tag*{(5)}

The collision of fat points in the following lemma is a special case of [7 §3.1, Proposition 5].

Lemma 2.2. The scheme ZZ is a flat limit of rr fat points of multiplicity mm with distinct supports. For rr general distinct points of XX, the restriction of WW to the union of the corresponding fat points has rank at least rank JJ. In particular, this restriction is injective if JJ is injective.

Proof. Choose distinct complex numbers c1,…,crc_1,\ldots,c_r and put Ps(w)=∏α=1r(w−scα)P_s(w)=\prod_{\alpha=1}^{r}(w-sc_\alpha), where ss is a parameter. The polynomial ideal (Ps(w),y)m(P_s(w),y)^m defines a finite flat family over the ss-line, as illustrated in Figure 1 (PDF p. 5). Indeed, there is an isomorphism of C[s]\mathbb{C}[s]-modules

Collision of four fat points into a monomial scheme

Figure 1 (PDF p. 5). The collision of fat points for r=4r = 4 and m=3m = 3.

C[s,w,y](Ps(w),y)m≅⨁a=0m−1C[s,w](Ps(w)m−a)ya.\frac{\mathbb{C}[s,w,y]}{(P_s(w),y)^m}\cong\bigoplus_{a=0}^{m-1}\frac{\mathbb{C}[s,w]}{(P_s(w)^{m-a})}y^a.

Since Ps(w)m−aP_s(w)^{m-a} is monic of degree r(m−a)r(m-a) in ww, polynomial division shows that the quotient on the left is free over C[s]\mathbb{C}[s] with basis yawby^aw^b, (a,b)∈I(a,b)\in I. Its rank is rm(m+1)/2rm(m+1)/2, proving finiteness and flatness [26 Tag 00NX]. Analytify this family and restrict the parameter ss to a sufficiently small disk DD about zero, so that its supports lie in the chosen coordinate chart. The chart identifies it with a finite flat family Z→D\mathcal{Z}\to D in XX. At s=0s=0, its ideal is (wr,y)m(w^r,y)^m, so the special fiber is ZZ. For s≠0s\ne0, the roots scαsc_\alpha are distinct. Near (scα,0)(sc_\alpha,0), the polynomial Ps(w)P_s(w) is w−scαw-sc_\alpha times a unit, so the local ideal is (w−scα,y)m(w-sc_\alpha,y)^m. Thus this fiber is the disjoint union of the required rr fat points.

Fix a basis of WW and use the normalized basis yawba!b!\frac{y^aw^b}{a!b!} of the coordinate algebra of the family. Restriction to the family is then represented by a matrix holomorphic in ss, whose value at s=0s=0 represents JJ. A nonzero minor of size rank JJ remains nonzero for small s≠0s\ne0. Thus some configuration of rr distinct fat points has restriction rank at least rank JJ. On the space of distinct rr-point configurations in XX, the restriction maps vary algebraically. The same argument with minors shows that the locus where the rank is at least rank JJ is Zariski open. It is nonempty by the construction, proving the assertion for general points.

Duality between interpolation and vanishing

Let S⊂Z2S\subset\mathbb{Z}^2 be a finite set of lattice points, and let II be a nonempty finite Young diagram. In Lemma 1.1, SS indexes evaluation points and II indexes the monomials used for interpolation. We now use SS to index Laurent monomials and II to specify vanishing along a monomial scheme supported at a single point. On the algebraic torus (C∗)2(\mathbb{C}^*)^2 with coordinates (ξ,η)(\xi,\eta), put VS=Span⁡C{ηjξk:(j,k)∈S}V_S=\operatorname{Span}_{\mathbb{C}}\{\eta^j\xi^k:(j,k)\in S\}. Set w=ξ−1w=\xi-1 and y=η−1y=\eta-1, and let ZIZ_I be the monomial scheme of (3) in these coordinates, supported at (1,1)(1,1). Every element of VSV_S is regular near (1,1)(1,1), even when some exponents are negative, so restriction to ZIZ_I is defined.

Lemma 2.3. Polynomials in the span of uavbu^av^b, (a,b)∈I(a,b)\in I, interpolate arbitrary values on SS if and only if the restriction map VS→H0(ZI,OZI)V_S\to H^0(Z_I,\mathcal{O}_{Z_I}) is injective. Equivalently, interpolation on SS holds if and only if the zero polynomial is the only Laurent polynomial G∈VSG\in V_S satisfying

∂a+bG∂ηa∂ξb∣(ξ,η)=(1,1)=0for every (a,b)∈I.\left.\frac{\partial^{a+b}G}{\partial\eta^a\partial\xi^b}\right|_{(\xi,\eta)=(1,1)}=0\qquad\text{for every }(a,b)\in I.

Proof. Use the binomial polynomials (ua)(vb)\binom{u}{a}\binom{v}{b}, (a,b)∈I(a,b)\in I, in place of the monomials uavbu^av^b. This is a triangular change of basis: each polynomial has leading term uavb/(a!b!)u^av^b/(a!b!), and all its other monomials are indexed by II because II is a Young diagram. The evaluation matrix at points of SS in this basis has entries (ja)(kb)\binom{j}{a}\binom{k}{b} for (j,k)∈S(j,k)\in S and (a,b)∈I(a,b)\in I, including when jj or kk is negative. These are exactly the coefficients of yawby^aw^b in ηjξk=(1+y)j(1+w)k\eta^j\xi^k=(1+y)^j(1+w)^k. Thus the restriction matrix in the monomial basis of the local algebra of ZIZ_I is the transpose of the evaluation matrix at points of SS. Consequently, evaluation is surjective if and only if restriction is injective.

For ordinary fat points, this duality between jets at a torus point and interpolation on lattice points appears in Dumnicki [5 Proposition 13], González–Karu [10 Section 2], Castravet [2 Lemmas 8.2–8.4], and He [13]. Lemma 2.3 gives the same argument for any Young diagram.

Restriction in holomorphic charts. Let XX be a smooth irreducible complex algebraic surface, with local holomorphic coordinates (ξ,η)(\xi,\eta) taking the value (1,1)(1,1) at a chosen point. Put w=log⁡ξw=\log\xi and y=log⁡ηy=\log\eta, choosing branches that vanish at (1,1)(1,1). Each generator (η−1)a(ξ−1)b(\eta-1)^a(\xi-1)^b is equal to yawby^a w^b multiplied by a holomorphic unit, so the monomial ideal of ZIZ_I is unchanged in the analytic local ring. In the normalized basis yawb/(a!b!)y^a w^b/(a!b!), restriction of the germs ηjξk=ekw+jy\eta^j\xi^k=e^{kw+jy} has the matrix

B0=(∂a+bekw+jy∂ya∂wb∣(w,y)=(0,0))(a,b)∈I, (j,k)∈S=(jakb)(a,b)∈I, (j,k)∈S.(6)B_0=\left(\left.\frac{\partial^{a+b}e^{kw+jy}}{\partial y^a\partial w^b}\right|_{(w,y)=(0,0)}\right)_{(a,b)\in I,\,(j,k)\in S} =(j^a k^b)_{(a,b)\in I,\,(j,k)\in S}. \tag*{(6)}

The matrix B0B_0 is the transpose of the polynomial evaluation matrix on SS. The same calculation applies to sections of a holomorphic line bundle on XX expressed in a local frame. Suppose bases indexed by SS have local representatives converging to ekw+jye^{kw+jy}, together with the derivatives indexed by the set II. Their restriction matrices then converge to B0B_0. If B0B_0 has full column rank, one of its ∣S∣×∣S∣|S|\times|S| minors is nonzero and remains nonzero under sufficiently small perturbations. The nearby restriction maps are therefore injective. In § 4, we apply this observation to bases constructed from theta functions on elliptic curves degenerating to nodal curves.

Weighted monomial ideals. Let p,q,Kp,q,K be positive integers. Put

JKp,q(w,y)=(wbya:pb+qa≥K),IKp,q={(a,b)∈Z≥02:pb+qa<K}.(7)\mathcal{J}^{p,q}_K(w,y)=(w^b y^a:pb+qa\ge K),\qquad I^{p,q}_K=\{(a,b)\in\mathbb{Z}_{\ge0}^2:pb+qa<K\}. \tag*{(7)}

The monomials indexed by IKp,qI^{p,q}_K form a basis of the quotient algebra C[w,y]/JKp,q\mathbb{C}[w,y]/\mathcal{J}^{p,q}_K. The points in column tt of IKp,qI^{p,q}_K have integer second coordinates satisfying 0≤b<(K−qt)/p0\le b<(K-qt)/p, so the column has height

At=max⁡{0,⌈K−qtp⌉}.(8)A_t=\max\left\{0,\left\lceil\frac{K-qt}{p}\right\rceil\right\}. \tag*{(8)}

For (p,q)=(1,r)(p,q)=(1,r) and K=rmK=rm, we recover the ideal of the collision of fat points in Lemma 2.2:

Jrm1,r(w,y)=(wr,y)m.(9)\mathcal{J}^{1,r}_{rm}(w,y)=(w^r,y)^m. \tag*{(9)}

The triangle Sh(α)S_h(\alpha). Let hh be a positive integer and α\alpha a positive rational number. Write Sh(α)S_h(\alpha) for the set of lattice points in the triangle with vertices (h,0)(h,0), (0,αh)(0,\alpha h), and (0,(α+9)h)(0,(\alpha+9)h), with the upper sloping edge omitted except for the vertex (h,0)(h,0):

Sh(α)={(h,0)}∪{(h−e,k):1≤e≤h, k∈Z, αe≤k<(α+9)e}.(10)S_h(\alpha)=\{(h,0)\}\cup\{(h-e,k):1\le e\le h,\ k\in\mathbb{Z},\ \alpha e\le k<(\alpha+9)e\}. \tag*{(10)}

For 1≤e≤h1\le e\le h, the column j=h−ej=h-e contains exactly 9e9e points: the half-open interval [αe,(α+9)e)[\alpha e,(\alpha+9)e) has integer length 9e9e and hence contains 9e9e integers. Including the vertex (h,0)(h,0), we obtain

∣Sh(α)∣=1+9h(h+1)2=(3h+22).(11)|S_h(\alpha)|=1+\frac{9h(h+1)}{2}=\binom{3h+2}{2}. \tag*{(11)}

Proposition 2.4. Let p,q,h,Kp,q,h,K be positive integers. Set α=Kph−9\alpha=\frac{K}{ph}-9. Suppose q>9pq>9p and K≥3hpqK\ge3h\sqrt{pq}.

Then α>0\alpha>0, and the restriction matrix (6) for I=IKp,qI=I^{p,q}_K and S=Sh(α)S=S_h(\alpha) has rank ∣Sh(α)∣|S_h(\alpha)|.

Proof. Put σ=K/(ph)\sigma= K/(ph), so that α=σ−9\alpha= \sigma- 9. The hypotheses give

σ≥3q/p>9,σ29≥qp.(12)\sigma\ge3\sqrt{q/p} > 9,\qquad\frac{\sigma^2}{9} \ge\frac{q}{p}. \tag*{(12)}

Put S=Sh(α)S = S_h(\alpha) and Nk=#{j:(j,k)∈S}N_k = \#\{j : (j,k) \in S\}. List the nonzero row lengths NkN_k of SS in decreasing order to form a Young diagram. The column tt of this diagram has length #{k:Nk≥t+1}\#\{k : N_k \ge t+1\}. Thus this diagram is contained in IKp,qI_K^{p,q} precisely when

#{k:Nk≥t}≤At−1(t≥1),(13)\#\{k : N_k \ge t\} \le A_{t-1}\qquad(t \ge1), \tag*{(13)}

where At−1A_{t-1} is the height of the (t−1)(t-1)-st column of IKp,qI_K^{p,q} given by (8). Under this condition, Lemma 1.1 gives interpolation of arbitrary values on SS by polynomials in the span of uavbu^a v^b, (a,b)∈IKp,q(a,b) \in I_K^{p,q}. By (6), the restriction matrix B0B_0 with I=IKp,qI = I_K^{p,q} therefore has full column rank.

It remains to verify (13). For 0<k<σh0 < k < \sigma h, the horizontal slice of the triangle Sh(α)S_h(\alpha) is

[max⁡{0,h−k/α}, h−k/σ),[\max\{0,h-k/\alpha\},\ h-k/\sigma),

whose width is

min⁡{9kασ,h−kσ}.\min\left\{\frac{9k}{\alpha\sigma},h-\frac{k}{\sigma}\right\}.

The graph of the width w(k)w(k) has a peak at (αh,9h/σ)(\alpha h,9h/\sigma); see Figure 2 (PDF p. 8).

The slice width as a function of height

Figure 2 (PDF p. 8). The slice width as a function of height.

For t≥2t \ge2, a slice containing at least tt lattice points has width strictly greater than t−1t-1, since its right endpoint is excluded. Thus every height with Nk≥tN_k \ge t lies in the open interval

ασ9(t−1)<k<σ(h−t+1).\frac{\alpha\sigma}{9}(t-1) < k < \sigma(h-t+1).

This interval is illustrated in Figure 2 (PDF p. 8). When nonempty, it has length

σh−σ29(t−1)≤K−q(t−1)p,\sigma h-\frac{\sigma^2}{9}(t-1) \le\frac{K-q(t-1)}{p},

by (12). An open interval of positive length LL contains at most ⌈L⌉\lceil L\rceil integers, so there are at most At−1A_{t-1} such heights by (8). If the interval is empty, the bound is automatic. This proves (13) for every column of positive index. For t=1t=1, all occupied heights, including the exceptional height zero, belong to [0,σh)=[0,K/p)[0,\sigma h)=[0,K/p), which contains ⌈K/p⌉=A0\lceil K/p\rceil=A_0 integers. This completes the proof. □

The argument allows equality in the second inequality of (12). Thus the proposition includes the case K=3hpqK=3h\sqrt{pq} whenever this number is an integer.

Example 1 (Sixteen points). Take (p,q)=(1,16)(p,q)=(1,16), h=4h=4, and K=48=3hpqK=48=3h\sqrt{pq}. Then α=3\alpha=3. As shown in Figure 3, S4(3)S_4(3) has 91 points, while I481,16I_{48}^{1,16} has 96 points. Proposition 2.4 says that the resulting 96×9196\times91 matrix has rank 91. After the transfer to the plane in § 5, this rules out a curve of degree 12 passing through 16 general points with multiplicity at least three. This is the equality case 12=31612=3\sqrt{16} in Theorem A. Example 3 gives the corresponding theta series.

Lattice points $S_4(3)$ and monomials $I_{48}^{1,16}$

Figure 3. The 91 lattice points of S4(3)S_4(3) and the 96 monomials indexed by I481,16I_{48}^{1,16}.

Example 2 (Ten points). Take (p,q)=(1,10)(p,q)=(1,10), h=3h=3, and K=30K=30. Here 3hpq=910<303h\sqrt{pq}=9\sqrt{10}<30, and α=1\alpha=1. Figure 4 shows the 55 points of S3(1)S_3(1) and the 60 monomials indexed by I301,10I_{30}^{1,10}. Proposition 2.4 gives a 60×5560\times55 matrix of rank 55. Since J301,10=(w10,y)3J_{30}^{1,10}=(w^{10},y)^3, this is the interpolation calculation for ten points of multiplicity three. Example 4 explains how it rules out plane curves of degree 9 through 10 general triple points. Example 5 extends these conditions to arbitrary multiplicity at one point.

Lattice points $S_3(1)$ and monomials $I_{30}^{1,10}$

Figure 4. The 55 lattice points of S3(1)S_3(1) and the 60 monomials indexed by I301,10I_{30}^{1,10} in Example 2.

Interpolation on the normal ruled surface

Let C⊂P2C \subset\mathbb{P}^{2} be a smooth plane cubic, with normal bundle M=NC/P2=OC(3)M = N_{C/\mathbb{P}^{2}} = \mathcal{O}_{C}(3) of degree nine. Let Tot⁡(M)\operatorname{Tot}(M) be its total space. Its projective completion is a ruled surface

π:Σˉ=PC(OC⊕M)⟶C.\pi: \bar{\Sigma} = \mathbb{P}_{C}(\mathcal{O}_{C} \oplus M) \longrightarrow C.

We use the convention that projective bundles parametrize lines rather than quotients. The summands OC\mathcal{O}_{C} and MM of OC⊕M\mathcal{O}_{C} \oplus M define the zero section C0C_{0} and the infinity section C∞C_{\infty} of Σˉ\bar{\Sigma}, respectively, so Σˉ∖C∞=Tot⁡(M)\bar{\Sigma} \setminus C_{\infty} = \operatorname{Tot}(M). The projective bundle formulas give

O(C0)=O(C∞)⊗π∗M,C02=9,C∞2=−9,C0⋅C∞=0.(14)\mathcal{O}(C_{0}) = \mathcal{O}(C_{\infty}) \otimes\pi^{*}M,\qquad C_{0}^{2} = 9,\qquad C_{\infty}^{2} = -9,\qquad C_{0} \cdot C_{\infty} = 0. \tag*{(14)}

See [12, II, Proposition 7.11; V, Propositions 2.3 and 2.9].

Theorem B. Let pp, qq, hh, KK be positive integers with q>9pq > 9p and K≥3hpqK \ge3h\sqrt{pq}. There exist a smooth plane cubic CC, a point x∈Tot⁡(M)x \in\operatorname{Tot}(M), and local holomorphic coordinates (w,y)(w,y) centered at xx such that

H0(Σˉ,O(hC0)⊗JKp,q(w,y))=0.(15)H^{0}\left(\bar{\Sigma}, \mathcal{O}(hC_{0}) \otimes\mathcal{J}_{K}^{p,q}(w,y)\right) = 0. \tag*{(15)}

Here JKp,q(w,y)\mathcal{J}_{K}^{p,q}(w,y) denotes the ideal sheaf that extends the local ideal by the unit ideal away from xx.

In the next sections, we will show that the specialization p=1p = 1, q=rq = r, K=rmK = rm gives Theorem A (Nagata Conjecture) and that the general case gives Theorem C of § 6 about the weighted blow-up of P2\mathbb{P}^{2} with weights (p,q)(p,q) at one point for very general local parameters.

Strategy of the proof. Let vv denote the tautological section of π∗M\pi^{*}M on Tot⁡(M)\operatorname{Tot}(M), which becomes a vertical fiber coordinate in a local frame of MM on CC. On Tot⁡(M)\operatorname{Tot}(M), we have O(hC0)≅π∗Mh\mathcal{O}(hC_{0}) \cong\pi^{*}M^{h} by (14). We have

H0(Tot⁡(M),π∗Mh)=H0(C,π∗π∗Mh)≅H0(C,Mh⊗π∗O)≅⨁j=0∞H0(C,Mh−j).H^{0}(\operatorname{Tot}(M),\pi^{*}M^{h}) = H^{0}(C,\pi_{*}\pi^{*}M^{h}) \cong H^{0}(C,M^{h}\otimes\pi_{*}\mathcal{O}) \cong\bigoplus_{j=0}^{\infty} H^{0}(C,M^{h-j}).

More precisely, every global section of π∗Mh\pi^{*}M^{h} on Tot⁡(M)\operatorname{Tot}(M) can be written uniquely as ∑j=0∞(π∗gj)vj\sum_{j=0}^{\infty}(\pi^{*}g_{j})v^{j}, where gj∈H0(C,Mh−j)g_{j} \in H^{0}(C,M^{h-j}). On Σˉ\bar{\Sigma}, we have O(hC0)≅(π∗Mh)(hC∞)\mathcal{O}(hC_{0}) \cong(\pi^{*}M^{h})(hC_{\infty}) by (14). Thus every global section of O(hC0)\mathcal{O}(hC_{0}) on Σˉ\bar{\Sigma} restricts to Tot⁡(M)\operatorname{Tot}(M) as a unique sum

F=∑j=0h(π∗gj)vj,gj∈H0(C,Mh−j).(16)F = \sum_{j=0}^{h}(\pi^{*}g_{j})v^{j},\qquad g_{j} \in H^{0}(C,M^{h-j}). \tag*{(16)}

The summation only goes up to hh because the order of the poles along C∞C_{\infty} is bounded from above by hh. The Riemann–Roch theorem gives h0(C,Mh−j)=9(h−j)h^{0}(C,M^{h-j}) = 9(h-j) for j<hj < h, while h0(C,OC)=1h^{0}(C,\mathcal{O}_{C}) = 1 [12 IV, Theorem 1.3]. Hence

h0(Σˉ,O(hC0))=1+9h(h+1)2=(3h+22).h^{0}(\bar{\Sigma},\mathcal{O}(hC_{0})) = 1 + \frac{9h(h+1)}{2} = \binom{3h+2}{2}.

This is the cardinality of the set Sh(α)S_{h}(\alpha) by (11). For a carefully chosen family of cubic curves degenerating to a nodal cubic, we will construct a point x∈Tot⁡(M)x \in\operatorname{Tot}(M), local holomorphic coordinates (w,y)(w,y) centered at xx, and a basis of H0(Σ‾,O(hC0))H^0(\overline{\Sigma},O(hC_0)). In the notation of (16), the basis elements will be of the form (π∗gk)vj(\pi^*g_k)v^j with gk∈H0(C,Mh−j)g_k\in H^0(C,M^{h-j}) indexed by points (j,k)∈Sh(α)(j,k)\in S_h(\alpha). The local expressions of the basis elements at the point xx will converge to ekw+jye^{kw+jy} as the cubic degenerates, with every partial derivative converging to the corresponding derivative of this exponential. The restriction matrices will converge to the matrix B0B_0 in (6), and Proposition 2.4 will give (15).

The GAGA theorems allow us to construct line bundles and compute global sections in the holomorphic category [23 §12, Theorems 1–3]. For 0<τ<10<\tau<1, consider the Tate curve [24 V, §1]

Cτ=C∗/τZ≃C/(2πiZ+(log⁡τ)Z).C_\tau=\mathbb{C}^*/\tau^{\mathbb{Z}}\simeq\mathbb{C}/(2\pi i\mathbb{Z}+(\log\tau)\mathbb{Z}).

The additive and multiplicative quotients are isomorphic by the exponential map. We denote the quotient map C∗→Cτ\mathbb{C}^*\to C_\tau by z↦[z]z\mapsto[z]. The annulus τ≤∣z∣≤1\tau\leq\lvert z\rvert\leq1 is a fundamental domain in C∗\mathbb{C}^*, with its outer boundary identified with its inner boundary by the dilation z↦τzz\mapsto\tau z.

For d∈Zd\in\mathbb{Z} and γ∈C∗\gamma\in\mathbb{C}^*, let Bd,γB_{d,\gamma} be the line bundle on CτC_\tau obtained from the trivial bundle C∗×C\mathbb{C}^*\times\mathbb{C} on C∗\mathbb{C}^* by the Z\mathbb{Z}-action generated by (z,t)↦(τz,γz−dt)(z,t)\mapsto(\tau z,\gamma z^{-d}t). In the covering frame, a holomorphic section of Bd,γB_{d,\gamma} lifts uniquely to a holomorphic function f:C∗→Cf:\mathbb{C}^*\to\mathbb{C} satisfying

f(τz)=γz−df(z).f(\tau z)=\gamma z^{-d}f(z).

Functions of this form are called *multiplicative theta functions of order dd. Conversely, every such function descends to a section. Multiplication of the covering frames gives

Bd,γ⊗Bd′,γ′≃Bd+d′,γγ′.B_{d,\gamma}\otimes B_{d',\gamma'}\simeq B_{d+d',\gamma\gamma'}.

The multiplicative theta function Θτ(z)\Theta_\tau(z) is defined as the infinite product

Θτ(z)=∏s=0∞(1−τsz)∏s=1∞(1−τs/z),(17)\Theta_\tau(z)=\prod_{s=0}^{\infty}(1-\tau^s z)\prod_{s=1}^{\infty}(1-\tau^s/z), \tag*{(17)}

which converges normally on compact annuli, has simple zeros exactly at τZ\tau^{\mathbb{Z}}, and satisfies

Θτ(τz)=−z−1Θτ(z),\Theta_\tau(\tau z)=-z^{-1}\Theta_\tau(z),

as described in [22 §4.1.2]. Thus Θτ(−z/γ)\Theta_\tau(-z/\gamma) lifts a section of B1,γB_{1,\gamma} with divisor [−γ]∈Cτ[-\gamma]\in C_\tau. In particular, deg⁡B1,γ=1\deg B_{1,\gamma}=1, and the tensor product rule gives deg⁡Bd,γ=d\deg B_{d,\gamma}=d for every integer dd.

Lemma 3.1. If d>0d>0, then H0(Cτ,Bd,γ)H^0(C_\tau,B_{d,\gamma}) has dimension dd. Write the equivariant lift of a section as a Laurent series f(z)=∑k∈Zckzkf(z)=\sum_{k\in\mathbb{Z}}c_kz^k. Its coefficients satisfy the recurrence

ck+d=γ−1τkck(18)c_{k+d}=\gamma^{-1}\tau^k c_k \tag*{(18)}

for every k∈Zk\in\mathbb{Z}. A basis is given by the sections whose equivariant lifts are the Laurent theta series

ϑkd,γ(z)=∑s∈Zγ−sτsk+ds(s−1)2zk+ds,(19)\vartheta_k^{d,\gamma}(z)=\sum_{s\in\mathbb{Z}}\gamma^{-s}\tau^{sk+\frac{ds(s-1)}{2}}z^{k+ds}, \tag*{(19)}

where we choose one kk in each residue class modulo $d.

Proof. Comparing coefficients in the Laurent series for f(τz)=γz−df(z)f(\tau z)=\gamma z^{-d}f(z) gives the recurrence (18). Thus one coefficient in each residue class modulo dd determines all the others. These dd coefficients can be chosen arbitrarily. Indeed, on a compact annulus, the terms of each series (19) are bounded by c1exp⁡(−c2s2+c3∣s∣)c_1\exp(-c_2s^2+c_3\lvert s\rvert) for constants c1,c2>0c_1,c_2>0 and c3c_3, since d>0d>0 and log⁡τ<0\log\tau<0. This bound is summable over s∈Zs\in\mathbb{Z}: for large ∣s∣\lvert s\rvert, it is at most c1exp⁡(−c2s2/2)c_1\exp(-c_2s^2/2). The sum is holomorphic [25 Chapter 2, Theorem 5.2], and reindexing the series gives f(τz)=γz−df(z)f(\tau z)=\gamma z^{-d}f(z). Thus f(z)f(z) descends to a global section of Bd,γB_{d,\gamma}. This proves the basis claim.

As τ→0\tau\to0, the Tate curve CτC_\tau degenerates to a nodal curve whose normalization is P1\mathbb{P}^1 with 00 and ∞\infty identified [11 §5.2, Proposition 5.7 and Exercise 47]. To motivate the subsequent choices, we recall that the nodal degeneration and its vanishing cycle can be seen in the plumbing chart

X=z,Y=τ/z,∣X∣,∣Y∣<ε.X=z,\qquad Y=\tau/z,\qquad\lvert X\rvert,\lvert Y\rvert<\varepsilon.

Here we fix ε\varepsilon such that 0<ε<10<\varepsilon<1 and 0<τ<ε20<\tau<\varepsilon^2. These inequalities guarantee that the plumbing chart is contained in the fundamental annulus. The latter is diffeomorphic to the cylinder

z=er+iθ,log⁡τ≤r≤0,θ∈R/2πZ.z=e^{r+i\theta},\qquad\log\tau\le r\le0,\qquad\theta\in\mathbb{R}/2\pi\mathbb{Z}.

The angular circle γτ(θ)=[τeiθ]\gamma_\tau(\theta)=[\sqrt{\tau}e^{i\theta}] in CτC_\tau has coordinates (X,Y)=(τeiθ,τe−iθ)(X,Y)=(\sqrt{\tau}e^{i\theta},\sqrt{\tau}e^{-i\theta}) and shrinks into the node (0,0)(0,0) as τ→0\tau\to0. It is the vanishing cycle in Figure 5.

The vanishing cycle in the cylinder, plumbing chart, and nodal fiber

Figure 5. The vanishing cycle γτ\gamma_\tau.

A fixed small ww-disk centered at the origin gives the moving chart z=τewz=\sqrt{\tau}e^w of CτC_\tau centered at z0=τz_0=\sqrt{\tau} for all sufficiently small τ\tau. This point approaches the node as τ→0\tau\to0. We now normalize the theta basis of Lemma 3.1 in the moving chart.

Lemma 3.2. Let dd be a positive integer and let U∈R∖ZU\in\mathbb{R}\setminus\mathbb{Z}. The bundle Bd,τU+d/2B_{d,\tau^{U+d/2}} has a basis, indexed by the dd integers U<k<U+dU<k<U+d, whose equivariant lifts satisfy

ϑ^k,τ(τew)=∑s∈Zτs(k−U)+ds(s−1)2e(k+ds)w→τ→0ekw.(20)\widehat{\vartheta}_{k,\tau}(\sqrt{\tau}e^w)=\sum_{s\in\mathbb{Z}}\tau^{s(k-U)+\frac{ds(s-1)}{2}}e^{(k+ds)w}\xrightarrow{\tau\to0}e^{kw}. \tag*{(20)}

The convergence is uniform on compact subsets of C\mathbb{C}, with every fixed derivative.

Proof. The interval (U,U+d)(U,U+d) contains one integer in each residue class modulo dd. In Lemma 3.1, take γ=τU+d/2\gamma=\tau^{U+d/2} and normalize the theta basis by setting

ϑ^k,τ(z)=τ−k/2ϑkd,γ(z).\widehat{\vartheta}_{k,\tau}(z)=\tau^{-k/2}\vartheta_k^{d,\gamma}(z).

Substituting z=τewz=\sqrt{\tau}e^w gives the normalized theta series (20).

The term with s=0s=0 is ekwe^{kw}. For s≥1s \ge1, the powers of τ\tau in the terms ss and −s-s are

s(k−U)+ds(s−1)2,s(U+d−k)+ds(s−1)2,s(k-U)+\frac{ds(s-1)}{2}, \qquad s(U+d-k)+\frac{ds(s-1)}{2},

respectively. Both are positive. On the disc ∣w∣≤R|w| \le R, the sum of the remaining terms is therefore bounded by

e∣k∣R∑s≥1[(edRτk−U)s+(edRτU+d−k)s]⟶τ→00.e^{|k|R}\sum_{s\ge1}\left[\left(e^{dR}\tau^{k-U}\right)^s+\left(e^{dR}\tau^{U+d-k}\right)^s\right]\longrightarrow_{\tau\to0}0.

These are geometric series once τ\tau is small. To control derivatives, write gτ(w)=ϑ^k,τ(τew)−ekwg_\tau(w)=\widehat{\vartheta}_{k,\tau}(\sqrt{\tau}e^w)-e^{kw}. For R,ρ>0R,\rho>0, apply the same bound on ∣w∣≤R+ρ|w|\le R+\rho. Cauchy’s estimate on a circle of radius ρ\rho about each point with ∣w∣≤R|w|\le R gives, for every ℓ≥0\ell\ge0,

sup⁡∣w∣≤R∣∂ℓgτ∂wℓ(w)∣≤ℓ!ρℓsup⁡∣ζ∣≤R+ρ∣gτ(ζ)∣⟶τ→00.(21)\sup_{|w|\le R}\left|\frac{\partial^\ell g_\tau}{\partial w^\ell}(w)\right| \le\frac{\ell!}{\rho^\ell}\sup_{|\zeta|\le R+\rho}|g_\tau(\zeta)| \longrightarrow_{\tau\to0}0. \tag*{(21)}

See [25 Chapter 2, Corollary 4.3 and Theorem 5.3].

Proof of Theorem B. Put α=K/(ph)−9>0\alpha=K/(ph)-9>0, as in Proposition 2.4. We are looking for a line bundle MτM_\tau on CτC_\tau of degree 99 so that normalized global sections of MτeM_\tau^e, a line bundle of degree 9e9e, have asymptotics ekwe^{kw} for kk in the j=h−ej=h-e column of the triangle Sh(α)S_h(\alpha), which requires αe≤k<(α+9)e\alpha e\le k<(\alpha+9)e by (10). By Lemma 3.2, the line bundle Bd,τU+d/2B_{d,\tau}^{U+d/2} has normalized theta functions tending to ekwe^{kw} for the integers U<k<U+dU<k<U+d. Thus we need to take

Mτ=B9,τα+9/2−δ,M_\tau=B_{9,\tau}^{\alpha+9/2-\delta},

where the small correction −δ-\delta is there to handle the half-open endpoints. Concretely, write α=A/D\alpha=A/D in lowest terms and put δ=12Dh\delta=\frac{1}{2Dh}. For 1≤e≤h1\le e\le h, we have Mτe=B9e,τ9e/2+e(α−δ)M_\tau^e=B_{9e,\tau}^{9e/2+e(\alpha-\delta)}. Lemma 3.2 applies with U=e(α−δ)U=e(\alpha-\delta) and degree 9e9e. Since αe∈D−1Z\alpha e\in D^{-1}\mathbb{Z} and 0<eδ<1/D0<e\delta<1/D, we have

(e(α−δ),e(α−δ)+9e)∩Z=[αe,(α+9)e)∩Z.(22)\left(e(\alpha-\delta),e(\alpha-\delta)+9e\right)\cap\mathbb{Z}=[\alpha e,(\alpha+9)e)\cap\mathbb{Z}. \tag*{(22)}

In particular, the endpoints on the left are nonintegral. By (10), the normalized theta functions of MτeM_\tau^e therefore tend to ekwe^{kw} for exactly the integers kk occurring in column j=h−ej=h-e of Sh(α)S_h(\alpha).

We work in the fixed covering frame of MτM_\tau and its tensor powers. The chart (z,v)=(τew,ey)(z,v)=(\sqrt{\tau}e^w,e^y) embeds a fixed polydisk ∣w∣,∣y∣<R<π|w|,|y|<R<\pi into Tot⁡Mτ\operatorname{Tot}M_\tau once ∣log⁡τ∣>2R|\log\tau|>2R. Indeed, if two points (w,y)(w,y) and (w′,y′)(w',y') have the same image, then w′−w=slog⁡τ+2πitw'-w=s\log\tau+2\pi it for integers s,ts,t. The bounds on real and imaginary parts force s=t=0s=t=0. The map y↦eyy\mapsto e^y is injective on this disk as well.

Let Σ‾τ=PCτ(O⊕Mτ)\overline{\Sigma}_\tau=\mathbb{P}_{C_\tau}(\mathcal{O}\oplus M_\tau). For each 1≤e≤h1\le e\le h, multiply the normalized theta basis of H0(Cτ,Mτe)H^0(C_\tau,M_\tau^e) by vh−ev^{h-e}. Together with vhv^h, these sections form a basis of H0(Σ‾τ,O(hC0))H^0(\overline{\Sigma}_\tau,\mathcal{O}(hC_0)) by (16). The basis is indexed by Sh(α)S_h(\alpha): the sections coming from MτeM_\tau^e correspond to (j,k)(j,k) with j=h−ej=h-e and αe≤k<(α+9)e\alpha e\le k<(\alpha+9)e, and vhv^h corresponds to (h,0)(h,0).

In the chart (z,v)=(τew,ey)(z,v)=(\sqrt{\tau}e^w,e^y) of Tot⁡(Mτ)\operatorname{Tot}(M_\tau), using the covering frame of MτM_\tau and its tensor powers, the section indexed by (j,k)(j,k) converges locally to ekw+jye^{kw+jy}. By Lemma 3.2 and (21), this convergence holds uniformly on compact subsets, together with every derivative in ww. The dependence on yy is entirely through the factor ejye^{jy}, so differentiating aa times in yy simply multiplies the local expression by jaj^a. Thus the mixed derivative ∂a+b/(∂ya∂wb)\partial^{a+b}/(\partial y^a\partial w^b), evaluated at (w,y)=(0,0)(w,y)=(0,0), converges to jakbj^ak^b.

The evaluation matrix therefore converges entrywise to (6), with basis sections indexed by Sh(α)S_h(\alpha) and derivatives indexed by IKp,qI_K^{p,q}. By Proposition 2.4, the limiting matrix has a nonzero minor of size ∣Sh(α)∣|S_h(\alpha)|. This minor remains nonzero for all sufficiently small positive τ\tau, proving (15).

The line bundles MτM_{\tau} are normal bundles of plane cubics. Indeed, the degree-three line bundle Lτ=B3,τ3/2+(α−δ)/3L_{\tau}=B_{3,\tau^{3/2+(\alpha-\delta)/3}} satisfies Lτ3=MτL_{\tau}^{3}=M_{\tau} and embeds CτC_{\tau} as a smooth plane cubic, with normal bundle Lτ3=MτL_{\tau}^{3}=M_{\tau} [12 IV, Example 3.3.3]; see also [26 Tags 0H2V and 0B3P].

Example 3 (Theta series for sixteen points). We return to Example 1 and Figure 3. Here (p,q)=(1,16)(p,q)=(1,16), h=4h=4, and K=48K=48, so α=3\alpha=3, δ=1/8\delta=1/8, and Mτ=B9,τ59/8M_{\tau}=B_{9,\tau^{59/8}}. We describe explicitly the basis theta function associated with each point of S4(3)S_{4}(3). For 1≤e≤41\le e\le4, the points in column j=4−ej=4-e are (4−e,k)(4-e,k) for 3e≤k<12e3e\le k<12e. The corresponding normalized theta functions, multiplied by the fiber factor v4−ev^{4-e}, have local expressions

∑t∈Zτt(k−23e/8)+9e t(t−1)2e(k+9et)w+(4−e)y.\sum_{t\in\mathbb{Z}}\tau^{t(k-23e/8)+\frac{9e\,t(t-1)}{2}}e^{(k+9et)w+(4-e)y}.

The term with t=0t=0 is ekw+(4−e)ye^{kw+(4-e)y}, whose exponents record the lattice point (4−e,k)(4-e,k). Every other term has a positive power of τ\tau. By Lemma 3.2, the sum of these remaining terms tends to zero uniformly on compact subsets, together with all derivatives. For example, the point (3,3)(3,3) corresponds to e=1e=1 and k=3k=3. Displaying the terms with t=0,1,−1t=0,1,-1, we obtain

e3w+3y+τ1/8e12w+3y+τ71/8e−6w+3y+⋯⟶e3w+3y.e^{3w+3y}+\tau^{1/8}e^{12w+3y}+\tau^{71/8}e^{-6w+3y}+\cdots\longrightarrow e^{3w+3y}.

Proof of the Nagata Conjecture

We first transfer Theorem B from the ruled surface to the plane. We fix a smooth cubic for which Theorem B holds and then degenerate the plane to its normal cone.

Proposition 4.1. Fix positive integers p,q,h,Kp,q,h,K. Let C⊂P2C\subset\mathbb{P}^{2} be a smooth cubic with normal bundle MM, and let Σ‾=PC(OC⊕M)\overline{\Sigma}=\mathbb{P}_{C}(\mathcal{O}_{C}\oplus M). Suppose

H0(Σ‾,O(hC0)⊗JKp,q(w,y))=0.H^{0}\left(\overline{\Sigma},\mathcal{O}(hC_{0})\otimes\mathcal{J}_{K}^{p,q}(w,y)\right)=0.

for local holomorphic coordinates at a point of Tot⁡(M)\operatorname{Tot}(M). Then there are regular local parameters (u,v)(u,v) at a point of P2\mathbb{P}^{2} for which

H0(P2,O(3h)⊗JKp,q(u,v))=0.(23)H^{0}\left(\mathbb{P}^{2},\mathcal{O}(3h)\otimes\mathcal{J}_{K}^{p,q}(u,v)\right)=0. \tag*{(23)}

Proof. We use a standard deformation to the normal cone [8 §5.1]; see also [12 II, Theorem 8.24] and [26 Tag 0FBG]. See the construction in Figure 6. We blow up C×{0}C\times\{0\} in P2×A1\mathbb{P}^{2}\times\mathbb{A}^{1}. Write Y\mathcal{Y} for the resulting threefold, ss for the parameter on A1\mathbb{A}^{1}, ρ:Y→P2\rho:\mathcal{Y}\to\mathbb{P}^{2} for the projection, and E\mathcal{E} for the exceptional divisor. The central fiber of Y\mathcal{Y} is Q∪EQ\cup\mathcal{E}, where

Deformation to the normal cone of the cubic

Figure 6. Deformation to the normal cone of the cubic.

Q≃P2,E≃Σ‾,Q∩E=C∞.Q\simeq\mathbb{P}^{2},\qquad\mathcal{E}\simeq\overline{\Sigma},\qquad Q\cap\mathcal{E}=C_{\infty}.

The weighted ideal has finite colength in the holomorphic local ring of Tot⁡(M)\operatorname{Tot}(M). Choose NN such that it contains mN+1\mathfrak{m}^{N+1}, where m\mathfrak{m} is the maximal ideal of its support. Replace (w,y)(w,y) by algebraic regular parameters (u,v)(u,v) with the same NN-jet. Their monomials agree modulo mN+1\mathfrak{m}^{N+1}, so they define the same weighted ideal in the holomorphic local ring of Tot⁡(M)\operatorname{Tot}(M).

The morphism Y∖Q→A1\mathcal{Y}\setminus Q\to\mathbb{A}^{1} is flat and has smooth fibers. Therefore, it is smooth. After an étale change of the parameter curve, extend the point of Tot⁡(M)\operatorname{Tot}(M) to a section of Y∖Q→A1\mathcal{Y}\setminus Q\to\mathbb{A}^{1} [26 Tag 05TG]. Lift u,vu,v to regular functions near the section and subtract their restrictions to it to make them vanish along the section. Their relative differentials are linearly independent at the original point and hence remain linearly independent along the section after shrinking. They are therefore relative local parameters along the section. The ideal (ubva:pb+qa≥K)(u^{b}v^{a} : pb + qa \geq K) defines a finite flat scheme ZZ supported on this section: its quotient has the fixed basis ubvau^{b}v^{a}, (a,b)∈IKp,q(a,b) \in I_{K}^{p,q}. Its ideal sheaf is flat as well, by the exact sequence 0→IZ→OY→OZ→00 \to I_Z \to\mathcal{O}_Y \to\mathcal{O}_Z \to0.

Put A=ρ∗O(3h)(−hE)\mathcal{A} = \rho^*\mathcal{O}(3h)(-h\mathcal{E}). Since E∣Q=C\mathcal{E}|_Q = C and E+Q\mathcal{E} + Q is the divisor of ss, we obtain

A∣Q=OP2,A∣E=OΣ‾(hC∞)⊗π∗Mh=OΣ‾(hC0).(24)\mathcal{A}|_Q = \mathcal{O}_{\mathbb{P}^2}, \qquad\mathcal{A}|_{\mathcal{E}} = \mathcal{O}_{\overline{\Sigma}}(hC_\infty) \otimes\pi^*M^h = \mathcal{O}_{\overline{\Sigma}}(hC_0). \tag*{(24)}

Both restrictions A∣Q\mathcal{A}|_Q and A∣E\mathcal{A}|_{\mathcal{E}} are trivial on C∞C_\infty. A global section of A\mathcal{A} on Q∪EQ \cup\mathcal{E} is a pair of sections agreeing along C∞C_\infty. Its restriction to QQ is a constant, uniquely determined by the restriction of its E\mathcal{E}-part to C∞C_\infty. Since Z0Z_0 is disjoint from QQ, it follows that

H0(Y0,A∣Y0⊗IZ0)≃H0(Σ‾,O(hC0)⊗IZ0)=0.H^0(Y_0,\mathcal{A}|_{Y_0} \otimes I_{Z_0}) \simeq H^0(\overline{\Sigma},\mathcal{O}(hC_0) \otimes I_{Z_0}) = 0.

Upper semicontinuity [12 III, Theorem 12.8] gives the same vanishing on nearby fibers. There the surface is P2\mathbb{P}^2, and the vertical twist O(−hE)\mathcal{O}(-h\mathcal{E}) restricts trivially. This proves (23).

The use of a vertical twist is related to the degeneration method of Ciliberto–Miranda [4 §2], who blow up a line in the central plane. Here the cubic gives an elliptic ruled surface.

Proof of Theorem A. First, let d=3hd = 3h and suppose 9h2≤rm29h^2 \leq rm^2, with r≥10r \geq10. Apply Theorem B and Proposition 4.1 with

p=1,q=r,K=rm≥3hr.p = 1,\qquad q = r,\qquad K = rm \geq3h\sqrt{r}.

They give local parameters on P2\mathbb{P}^2 for which

H0(P2,O(3h)⊗(ur,v)m)=0,H^0\left(\mathbb{P}^2,\mathcal{O}(3h) \otimes(u^r,v)^m\right) = 0,

using (9). Lemma 2.2 deforms this scheme into rr distinct multiplicity-mm fat points. Injectivity of the evaluation matrix persists, so no degree-3h3h form vanishes to order at least mm at rr general points.

For arbitrary positive integers d,md,m with d≤mrd \leq m\sqrt{r}, apply this result with h=dh = d and multiplicity 3m3m. If a form of degree dd vanished to order at least mm at every point, its cube would be a form of degree 3d3d of multiplicity at least 3m3m, which was just ruled out.

Example 4 (Ten and sixteen points). Take r=10r = 10, m=3m = 3, and d=9d = 9, so h=3h = 3, K=30K = 30, and α=1\alpha= 1. The columns of S3(1)S_3(1) are

j0123k3,…,292,…,191,…,90\begin{array}{c|cccc} j & 0 & 1 & 2 & 3 \\ \hline k & 3,\ldots,29 & 2,\ldots,19 & 1,\ldots,9 & 0 \end{array}

They contain 55 points, matching the dimension of the space of forms of degree 9. The staircase 1,1030\frac{1,10}{30} has column lengths 30, 20, 10, so its length is 60, the number of conditions imposed by ten triple points. It follows that no curve of degree 9 passes through ten general triple points.

Example 1 and Figure 3 give the case r=16r = 16, m=3m = 3, d=12d = 12: here K=rm=48K = rm = 48 and h=4h = 4. The argument excludes curves of degree 12 through sixteen general triple points.

Monomial valuations and weighted blow-ups

Throughout this section, pp and qq are coprime positive integers with q>9pq > 9p. Fix a point x∈P2x \in\mathbb{P}^2 and regular local parameters (u,v)(u,v) at xx. The corresponding monomial valuation is

ν(∑a,b≥0cabubva)=min⁡cab≠0(pb+qa).(25)\nu\left(\sum_{a,b\geq0} c_{ab}u^b v^a\right)=\min_{c_{ab}\ne0}(pb+qa). \tag*{(25)}

For a section of OP2(d)\mathcal{O}_{\mathbb{P}^2}(d), use any local frame at xx. Changing the frame multiplies the local equation by a unit and does not change its valuation. Put

μ^(ν)=sup⁡0≠F∈H0(P2,O(d))d≥1ν(F)d.(26)\widehat{\mu}(\nu)=\sup_{\substack{0\ne F\in H^0(\mathbb{P}^2,\mathcal{O}(d))\\d\geq1}}\frac{\nu(F)}{d}. \tag*{(26)}

Theorem C. For a very general choice of local parameters at the fixed point xx,

ν(F)<dpqfor every d≥1 and 0≠F∈H0(P2,O(d)).(27)\nu(F)<d\sqrt{pq}\qquad\text{for every }d\geq1\text{ and }0\ne F\in H^0(\mathbb{P}^2,\mathcal{O}(d)). \tag*{(27)}

Nevertheless,

μ^(ν)=pq.(28)\widehat{\mu}(\nu)=\sqrt{pq}. \tag*{(28)}

Thus the supremum in (26) is not attained, including when pqpq is a square.

If one normalizes the valuation to ν/p\nu/p and sets t=q/pt=q/p, the equality (28) becomes μ^(ν/p)=t\widehat{\mu}(\nu/p)=\sqrt{t}. This proves the rational-weight case with t>9t>9 of the valuative Nagata conjecture of Dumnicki–Harbourne–Küronya–Roé–Szemberg [6 Conjecture 4.3]. Their stronger conjecture has the threshold t≥8+1/36t\geq8+1/36 [6 Conjecture 2.4]. For recent equivalent formulations in the broader setting of plane valuations, see [9 Conjecture C and Corollary 3.14]. The relation with Nagata’s conjecture through collisions of fat points already appears in [6 Proposition 4.4].

It is important to emphasize that the local parameters need to be very general. For example, in affine linear coordinates the line v=0v=0 has valuation q>pqq>\sqrt{pq}. To specify a finite-dimensional parameter space, let mx\mathfrak{m}_x be the maximal ideal at xx and put J=⌊q/p⌋J=\lfloor q/p\rfloor. The pairs (u,v)∈(mx/mxJ+1)2(u,v)\in(\mathfrak{m}_x/\mathfrak{m}_x^{J+1})^2 with independent linear terms form an irreducible open subset, denoted JJ(x)\mathcal{J}_J(x). This finite jet determines the valuation in every degree. Indeed, changing the parameters modulo mxJ+1\mathfrak{m}_x^{J+1} adds terms of valuation at least p(J+1)>qp(J+1)>q. The change of parameters therefore induces the identity on the associated graded ring of the weighted filtration. In particular, every valuation ideal is unchanged. We use “very general” in this fixed finite-dimensional parameter space; compare [6 Remark 2.3].

Proof of Theorem C. For each h≥1h \ge1, put Kh=⌊3hpq⌋K_h=\left\lfloor3h\sqrt{pq}\right\rfloor. Theorem B and Proposition 4.1 give local parameters on P2\mathbb{P}^2 for which the restriction of H0(O(3h))H^0(\mathcal{O}(3h)) to O/JKhp,q\mathcal{O}/\mathcal{J}_{K_h}^{p,q} is injective. A projective automorphism moves the support of this finite scheme to the fixed point xx.

For fixed d,Kd,K, failure of injectivity is a closed condition on J(x)\mathcal{J}(x). Indeed, choose affine coordinates at xx and polynomial representatives of the parameter jets. The coefficients of the inverse formal change of coordinates, to any fixed order, are regular functions of these coefficients and the inverse Jacobian determinant. Expanding the degree-dd forms and retaining the terms indexed by IKp,qI_K^{p,q} gives a matrix of regular functions. Its maximal minors define the noninjectivity locus. The valuation ideals are independent of the chosen representatives.

For (d,K)=(3h,Kh)(d,K)=(3h,K_h), the local parameters just constructed show that this closed locus is proper. Choose a jet outside the union of these loci over all h≥1h \ge1. If a nonzero degree-dd form had ν(F)≥dpq\nu(F)\ge d\sqrt{pq}, then

ν(F3)=3ν(F)≥3dpq,deg⁡(F3)=3d.\nu(F^3)=3\nu(F)\ge3d\sqrt{pq}, \qquad\deg(F^3)=3d.

Since the valuation is integral, ν(F3)≥Kd\nu(F^3)\ge K_d, contradicting injectivity in degree 3d3d. This proves (27).

For the reverse asymptotic inequality, the length of the weighted scheme is

length⁡(O/JKp,q)=∑a≥0Aa=K22pq+O(K),(29)\operatorname{length}(\mathcal{O}/\mathcal{J}_K^{p,q})=\sum_{a\ge0} A_a=\frac{K^2}{2pq}+O(K), \tag*{(29)}

where Aa=max⁡{0,⌈K−qap⌉}A_a=\max\left\{0,\left\lceil\frac{K-qa}{p}\right\rceil\right\} by (8). The estimate follows by summing (K−qa)/p(K-qa)/p for 0≤a<K/q0\le a<K/q; replacing each term by its ceiling changes the sum by O(K)O(K). For 0<c<pq0<c<\sqrt{pq} and K=⌈cd⌉K=\lceil cd\rceil, the length (29) is less than h0(P2,O(d))=(d+22)h^0(\mathbb{P}^2,\mathcal{O}(d))=\binom{d+2}{2} for large dd. Hence some nonzero degree-dd form has valuation at least KK for every choice of parameters. Thus μ^(ν)≥c\widehat{\mu}(\nu)\ge c for every c<pqc<\sqrt{pq}, proving the equality claimed in the theorem. □

Example 5. For the weights (p,q)=(1,10)(p,q)=(1,10) and any m≥1m\ge1,

J10m1,10=(u10,v)m,length⁡(O/J10m1,10)=5m(m+1).\mathcal{J}_{10m}^{1,10}=(u^{10},v)^m,\qquad\operatorname{length}(\mathcal{O}/\mathcal{J}_{10m}^{1,10})=5m(m+1).

Writing F=∑i≥0fi(u)viF=\sum_{i\ge0}f_i(u)v^i, we can express these conditions as ord⁡ufi≥10(m−i)\operatorname{ord}_u f_i\ge10(m-i) for 0≤i<m0\le i<m. Theorem C gives d>m10d>m\sqrt{10} for every nonzero degree-dd form satisfying these conditions for very general local parameters. For m=3m=3, this is the ideal in Example 2: degree 9 is excluded, whereas in degree 10, the dimension of the space of global forms is 66, while there are only 60 linear conditions. For m=5m=5, degree 15 is excluded, whereas in degree 16 the dimension of the space of global forms is 153, while there are only 150 linear conditions. Thus the least possible degrees in these two cases are 10 and 16, respectively.

Example 6. Take (p,q)=(4,49)(p,q)=(4,49), so that q/p=(7/2)2>9q/p=(7/2)^2>9 and pq=14\sqrt{pq}=14. The ideal

J1964,49=(u49,u37v,u25v2,u13v3,v4)\mathcal{J}_{196}^{4,49}=(u^{49},u^{37}v,u^{25}v^2,u^{13}v^3,v^4)

has colength 49+37+25+13=12449+37+25+13=124. For very general parameters, Theorem C excludes a nonzero form of degree at most 14 in this ideal. Degree-fifteen forms, however, have dimension 136>124136>124. Hence the least degree satisfying these vanishing conditions is exactly fifteen.

In particular, no curve of degree 14 has a local equation u49−v4u^{49}-v^4 plus terms of higher (4,49)(4,49)-weighted degree in these prescribed very general parameters. The model cusp u49=v4u^{49}=v^4 has normalization u=t4u=t^4, v=t49v=t^{49}. Its delta invariant is the number of gaps in the semigroup ⟨4,49⟩\langle4,49\rangle, namely 12+24+36=7212+24+36=72. This is smaller than the arithmetic genus (14−1)(14−2)/2=78(14-1)(14-2)/2=78 of a degree-fourteen plane curve. Thus the genus bound alone does not explain the exclusion.

The weighted blow-up. Let π:Y→P2\pi:Y\to\mathbb{P}^{2} be the normalization of the blow-up of the ideal sheaf (uq,vp)(u^{q},v^{p}) (extended by the unit ideal away from xx). This is the (p,q)(p,q)-weighted blow-up of P2\mathbb{P}^{2} with respect to the local parameters (u,v)(u,v). It is a projective surface with cyclic quotient singularities and one prime exceptional divisor EE. Write HH for the pullback of the line class. We have

H2=1,H⋅E=0,E2=−1pq.(30)H^{2}=1,\qquad H\cdot E=0,\qquad E^{2}=-\frac{1}{pq}. \tag*{(30)}

See, for example, [1 Theorem 4.3]. Every nonexceptional prime divisor of YY is the strict transform of a plane curve F=0F=0 of degree dd, with class dH−ν(F)EdH-\nu(F)E. Put

D=H−pq E.D=H-\sqrt{pq}\,E.

Corollary 5.1. For the very general parameters in Theorem C,

Nef⁡(Y)=R≥0H+R≥0D,\operatorname{Nef}(Y)=\mathbb{R}_{\geq0}H+\mathbb{R}_{\geq0}D,
Eff⁡‾(Y)=R≥0E+R≥0D.(31)\overline{\operatorname{Eff}}(Y)=\mathbb{R}_{\geq0}E+\mathbb{R}_{\geq0}D. \tag*{(31)}

The class DD is strictly nef and has square zero. No nonzero effective R\mathbb{R}-divisor has a class on its ray. The Cox ring of YY is not finitely generated.

Proof. Theorem C and (30) give

D2=0,D⋅E=1pq>0,D⋅C~=d−ν(F)pq>0.D^{2}=0,\qquad D\cdot E=\frac{1}{\sqrt{pq}}>0,\qquad D\cdot\widetilde{C}=d-\frac{\nu(F)}{\sqrt{pq}}>0.

Thus DD has positive intersection with every prime curve. In particular, no nonzero effective R\mathbb{R}-divisor can have a class on its ray. A class xH−yExH-yE is nef precisely when y≥0y\geq0 and x≥y/pqx\geq y/\sqrt{pq}. This proves the first formula. Every effective divisor is a sum of EE and strict transforms with ν(F)/d<pq\nu(F)/d<\sqrt{pq}. The dimension count in the proof of Theorem C gives effective classes whose ratios approach pq\sqrt{pq}, proving the second formula.

The divisor class group is generated by HH and EE. If the Cox ring were finitely generated, the classes of finitely many homogeneous generators would generate the closed effective cone. Each extremal ray would then contain a nonzero effective class, contradicting the assertion about DD.

References

  1. [1]E. Artal Bartolo, J. Martín-Morales, and J. Ortigas-Galindo, Intersection theory on abelian-quotient V-surfaces and Q-resolutions, J. Singul. 8 (2014), 11–30. doi:10.5427/jsing.2014.8b.DOI
  2. [2]A.-M. Castravet, Mori dream spaces and blow-ups, in Algebraic Geometry: Salt Lake City 2015, Proceedings of Symposia in Pure Mathematics 97.1, American Mathematical Society, Providence, RI, 2018, 143–167. doi:10.1090/pspum/097.1/01671.DOI
  3. [3]C. Ciliberto, B. Harbourne, R. Miranda, and J. Roé, Variations on Nagata’s conjecture, in A Celebration of Algebraic Geometry, B. Hassett, J. McKernan, J. Starr, and R. Vakil (eds.), Clay Mathematics Proceedings 18, American Mathematical Society, Providence, RI, 2013, 185–203. Publisher’s open-access volume.
  4. [4]C. Ciliberto and R. Miranda, Degenerations of planar linear systems, J. Reine Angew. Math. 501 (1998), 191–220. doi:10.1515/crll.1998.077.DOI
  5. [5]M. Dumnicki, Cutting diagram method for systems of plane curves with base points, Ann. Polon. Math. 90 (2007), no. 2, 131–143. doi:10.4064/ap90-2-3.DOI
  6. [6]M. Dumnicki, B. Harbourne, A. Küronya, J. Roé, and T. Szemberg, Very general monomial valuations of ℙ² and a Nagata type conjecture, Comm. Anal. Geom. 25 (2017), no. 1, 125–161. doi:10.4310/CAG.2017.v25.n1.a4.DOI
  7. [7]L. Evain, Une minoration du degré de courbes planes à singularités imposées, Bull. Soc. Math. France 126 (1998), no. 4, 525–543. doi:10.24033/bsmf.2335.DOI
  8. [8]W. Fulton, Intersection Theory, second edition, Ergebnisse der Mathematik und ihrer Grenzgebiete (3) 2, Springer-Verlag, Berlin, 1998. doi:10.1007/978-1-4612-1700-8.DOI
  9. [9]C. Galindo, F. Monserrat, C.-J. Moreno-Ávila, and J.-J. Moyano-Fernández, On the valuative Nagata conjecture, Res. Math. Sci. 12 (2025), article 18, 24 pp. doi:10.1007/s40687-025-00500-2.DOI
  10. [10]J. L. González and K. Karu, Some non-finitely generated Cox rings, Compos. Math. 152 (2016), no. 5, 984–996. doi:10.1112/S0010437X15007745.DOI
  11. [11]R. Hain, Lectures on moduli spaces of elliptic curves, in Transformation Groups and Moduli Spaces of Curves, L. Ji and S.-T. Yau (eds.), Advanced Lectures in Mathematics 16, International Press, Somerville, MA, and Higher Education Press, Beijing, 2011, 95–166. Author’s version: arXiv:0812.1803v3.arxiv.org/abs/0812.1803
  12. [12]R. Hartshorne, Algebraic Geometry, Graduate Texts in Mathematics 52, Springer-Verlag, New York–Heidelberg, 1977. doi:10.1007/978-1-4757-3849-0.DOI
  13. [13]Z. He, Blow-ups of toric surfaces and the Mori dream space property, Exp. Math. 30 (2021), no. 3, 386–404. doi:10.1080/10586458.2018.1547322.
  14. [14]E. Miller and B. Sturmfels, Combinatorial Commutative Algebra, Graduate Texts in Mathematics 227, Springer, New York, 2005. doi:10.1007/b138602.DOI
  15. [15]M. Nagata, On the 14-th problem of Hilbert, Amer. J. Math. 81 (1959), no. 3, 766–772. doi:10.2307/2372927.DOI
  16. [16]M. Nagata, Lectures on the Fourteenth Problem of Hilbert, Tata Institute of Fundamental Research Lectures on Mathematics 31, Tata Institute of Fundamental Research, Bombay, 1965. Notes by M. Pavaman Murthy. Publisher’s open-access text.
  17. [17]OpenAI, Nagata’s conjecture for plane curves, OpenAI Math Release preprint, September 23, 2026. Released manuscript.hub.valency.io/works/W_zbgnc7ph
  18. [18]OpenAI, Maximal Sehadri constants on arbitrary polarized surfaces, OpenAI Math Release preprint, September 23, 2026. Released manuscript.hub.valency.io/works/W_jmdujwyp
  19. [19]OpenAI, Maximal multipoint Sehadri constants in higher dimensions, OpenAI Math Release preprint, October 5, 2026. Released manuscript.hub.valency.io/works/W_asx3sjmn
  20. [20]OpenAI, Maximal multipoint Sehadri constants in positive characteristic, OpenAI Math Release preprint, October 5, 2026. Released manuscript.hub.valency.io/works/W_nyrv942k
  21. [21]OpenAI, openai/math, repository and release documentation, 2026. Release repository.
  22. [22]H. Rosengren, Elliptic hypergeometric functions, in Lectures on Orthogonal Polynomials and Special Functions, H. S. Cohl and M. E. H. Ismail (eds.), London Mathematical Society Lecture Note Series 464, Cambridge University Press, Cambridge, 2020, 213–279. doi:10.1017/9781108908993.005.DOI
  23. [23]J.-P. Serre, Géométrie algébrique et géométrie analytique, Ann. Inst. Fourier 6 (1956), 1–42. doi:10.5802/aif.59.DOI
  24. [24]J. H. Silverman, Advanced Topics in the Arithmetic of Elliptic Curves, Graduate Texts in Mathematics 151, Springer-Verlag, New York, 1994. doi:10.1007/978-1-4612-0851-8.DOI
  25. [25]E. M. Stein and R. Shakarchi, Complex Analysis, Princeton Lectures in Analysis II, Princeton University Press, Princeton, NJ, 2003. Publisher’s page.
  26. [26]The Stacks Project Authors, The Stacks Project, 2026. Online reference.
  27. [27]J. Tevelev, Log MMP constraints on curves with cuspidal singularities, preprint, 2026. arXiv:2608.25031.arxiv.org/abs/2608.25031

Paper details

vlnc:W_53qnbawb
v1 · latestHistory (1)

published · Fresh — added to the Hub within the last 30 days

added ·

Usage

views · 1

downloads · 0

A view counts once per browser per day, a download each time the PDF is requested.

CC BY 4.0

Original source

  • Mathematics

ChatGPT Astra · View statement →

Looking for related papers…
Contents