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Nagata's conjecture for plane curves

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Abstract

We prove that a nonzero effective plane curve of degree dd at r≥10r\ge10 very general complex points has total multiplicity strictly less than drd\sqrt r. The inequality holds simultaneously for all curves, including reducible and nonreduced curves, and establishes Nagata's conjecture in its strict, nonhomogeneous form.

Introduction

Prescribing multiple points of a plane curve is an interpolation problem: how small can its degree be when the positions and the required orders of vanishing are given? Nagata’s conjecture predicts the answer at the square-root scale for sufficiently many very general points. Nagata introduced the problem in his work on Hilbert’s fourteenth problem and proved the square cases r≥16r \ge16 [12, 13]. We prove the strict inequality for every r≥10r \ge10, allowing unequal multiplicities.

We first work over C\mathbb{C}. Let

Ur={(p1,…,pr)∈(PC2)r:pi≠pj for i≠j}.U_r = \left\{(p_1,\ldots,p_r) \in\left(\mathbb{P}^2_{\mathbb{C}}\right)^r : p_i \ne p_j \text{ for } i \ne j\right\}.

A nonzero effective plane curve is the zero divisor of a nonzero homogeneous form of degree d≥1d \ge1. Its multiplicity at a point is the order of that form in the regular local ring. Components may repeat. The phrase very general in the following theorem means the complement of one countable union of proper closed subsets, chosen simultaneously for all degrees and multiplicity vectors.

The scale can already be seen when all prescribed multiplicities equal mm. A degree-dd form has (d+22)\binom{d+2}{2} coefficients, and order at least mm at rr points imposes at most r(m+12)r\binom{m+1}{2} linear conditions. Their leading terms balance at d=mrd = m\sqrt{r}. A count of conditions supplies curves asymptotically above this scale; proving their absence below it requires control of the dependencies among the conditions, for every mm. The strict endpoint also matters: at nine points a nonzero cubic always exists, so the asserted strict inequality cannot start at r=9r = 9.

Theorem 1.1. For every integer r≥10r \ge10, there is a countable union ErE_r of proper Zariski-closed subsets of UrU_r, with nonempty complement, such that the following holds for every tuple (p1,…,pr)∉Er(p_1,\ldots,p_r) \notin E_r. If CC is a nonzero effective plane curve of degree d≥1d \ge1 and m1,…,mr∈Z≥0m_1,\ldots,m_r \in\mathbb{Z}_{\ge0} satisfy mult⁡piC≥mi\operatorname{mult}_{p_i} C \ge m_i, then

dr>∑i=1rmi.d\sqrt{r} > \sum_{i=1}^{r} m_i.

On the blowup of the plane at such a tuple, the theorem gives a real divisor class of self-intersection zero that intersects every curve positively. It also determines the multipoint Seshadri constant: the largest tt for which the pullback of a line minus tt times the sum of the exceptional curves has nonnegative intersection with every curve. Its value is 1/r1/\sqrt{r}, which is irrational when rr is nonsquare. Section 6 proves these consequences and extends the theorem to every uncountable algebraically closed field of characteristic zero.

Prior work and the interpolation approach

The geometry of plane linear systems connects this problem with the cones of effective and nef divisor classes on blowups. Ciliberto–Harbourne–Miranda–Roé [4] develop these connections and compare several forms and extensions of Nagata’s conjecture. For homogeneous multiplicities, Roé [15] obtained the uniform estimate d>m(r−1−π/8)d > m(\sqrt{r-1}-\pi/8) for r≥10r \ge10 by specializing to configurations with infinitely near points. Harbourne [11] sharpened rational lower bounds and proved further cases in restricted multiplicity ranges. For ten very general points, degeneration methods give d/m≥117/37d/m \ge117/37 for every nonempty homogeneous system: Eckl’s Seshadri estimate and Ciliberto–Dumitrescu–Miranda–Roé’s analysis of plane systems give this bound in their respective formulations [9, 3]. Such bounds explain the importance of controlling arbitrarily large multiplicities at each fixed nonsquare rr.

Dumnicki–Harbourne–Küronya–Roé–Szemberg [8] study an analogue for very general monomial valuations, while Nivoche [14] relates the conjecture to transcendental interpolation in Cn\mathbb{C}^{n}. These perspectives emphasize that the obstruction is not merely the number of imposed conditions, but how vanishing conditions interact with the geometry of the ambient surface. More recently, Ciliberto–Miranda–Roé [6 Theorem 1] constructed irrational square-zero nef rays on the blowups at every r≥10r \ge10 very general points. Those constructions do not determine the equal-weight multipoint Seshadri constant. Nagata’s conjecture singles out the class with equal exceptional coefficients, whose nefness gives that constant’s exact value.

The proof below uses two established approaches to this interaction. Ciliberto–Miranda [5] develop degenerations of plane linear systems, and Evain [10] studies their infinitesimal limits when fat points, meaning points equipped with specified orders of vanishing, approach a divisor. Dumnicki [7] encodes interpolation by finite diagrams of monomial exponents and their evaluation matrices. In particular, the proof of his Proposition 13 converts a one-point derivative matrix into polynomial evaluation on the exponent diagram. Our final rank problem has the same evaluation interpretation, with a different set of allowed polynomial degrees supplied by a collinear collision.

The elliptic stage uses the classical multiplicative theta product and its residue-class Laurent bases; the conventions used here are recorded in Rosengren [16] (arXiv version, Section 1.2 and Exercise 1.6.5). We prove the needed product identities, basis formulas and convergence estimates in the normalization required by the argument.

Proof strategy

Closed incidence loci turn a failure at very general points into a system of curves existing at every configuration. A product over cyclic permutations makes the multiplicities equal; write dd and mm for the resulting degree and common multiplicity. Moving the points toward a smooth curve gives a nonzero polynomial on its normal line bundle, with order at least mm at arbitrary normal displacements. For square rr, its two highest coefficients already exclude d/m≤rd/m \le\sqrt{r}, including equality (Section 2).

For nonsquare rr, we use a cubic and set nine normal displacements to zero. Dividing out the forced coefficient zeros and changing the fiber coordinate give a finite-dimensional space of polynomial sections whose first m+1m+1 coefficient bundles have equal degree (Section 3). On each fixed elliptic curve, the remaining q=r−9q=r-9 points collide along a horizontal coordinate line. After b<mb < m fiber derivatives, a section must then have base order at least q(m−b)q(m-b); thus a particular finite jet map has a nonzero kernel. A separate degeneration gives explicit normalized theta bases whose expressions in logarithmic base and fiber coordinates (x,y)(x,y) tend to eKx+jye^{Kx+jy}. Here jj is the fiber degree and KK a Laurent exponent. Their mixed derivatives give the limiting matrix

(Kℓjb),0≤b<m,0≤ℓ<q(m−b),(K^\ell j^b), \qquad0 \le b < m,\quad0 \le\ell< q(m-b),

with columns indexed by exponent pairs (j,K)(j,K) (Section 4). Only these numerical matrices are compared across curves; the argument does not choose a simultaneous family of kernel vectors.

To exclude the kernel, a total count of exponent pairs is not enough. We group them into horizontal rows of fixed KK, with jj varying. Interpolation one row at a time gives full column rank if no row has more than mm points and at most q(m−t+1)q(m-t+1) rows have at least tt points. The exponent pairs lie in a polygon whose slice-width profile supplies exactly these bounds. Since d/md/m is rational and rr is nonsquare, the strict gap d/m<rd/m < \sqrt{r} permits a contraction of that polygon; taking a common power of the original curve absorbs the integer endpoint error in the row count. Full rank persists for small positive degeneration parameter, contradicting the kernel on each fixed curve (Section 5).

From plane curves to normal polynomials

We reduce a violation at very general points to an equal-multiplicity system existing at every configuration. Moving its points toward a smooth plane curve then gives a polynomial on the normal bundle. This polynomial will exclude the square cases and supply the input for the cubic construction in Section 3.

The order of a section is the order of its scalar expression in a local frame. A frame change multiplies this expression by a unit, preserving the order. In local coordinates, order at least mm means that every Taylor coefficient of total degree less than mm vanishes. Thus algebraic and holomorphic orders agree, and holomorphic coordinate changes preserve them.

A universal equal-multiplicity system

For positive integers dd, mm, write Ur(d,m)\mathsf U_r(d,m) for the property

For every (p1,…,pr)∈Ur(p_1,\ldots,p_r) \in U_r there is a nonzero form

S∈H0(P2,OP2(d))such thatmult⁡pi(S)≥m(1≤i≤r).(1)S \in H^0(\mathbb{P}^2,\mathcal{O}_{\mathbb{P}^2}(d)) \quad\text{such that} \quad\operatorname{mult}_{p_i}(S) \ge m \quad(1 \le i \le r). \tag*{(1)}

Here and below the multiplicity of a form is the multiplicity of its zero divisor.

Lemma 2.1 (Reduction to universal systems). For each r≥10r \ge10 there is a countable union ErE_r of proper Zariski-closed subsets of UrU_r, all defined over Q\mathbb{Q}, with Ur∖Er≠∅U_r \setminus E_r \ne\varnothing, having the following property. If a tuple outside ErE_r supports a degree-d0d_0 form, d0≥1d_0 \ge1, with multiplicities at least m1,…,mr∈Z≥0m_1,\ldots,m_r \in\mathbb{Z}_{\ge0} and

d0r≤∑i=1rmi,d_0\sqrt{r} \le\sum_{i=1}^{r} m_i,

then Ur(d,m)\mathsf U_r(d,m) holds for some positive integers d,md,m with d/m≤rd/m \le\sqrt{r}. If Ur(d,m)\mathsf U_r(d,m) holds, then Ur(Nd,Nm)\mathsf U_r(Nd,Nm) holds for every positive integer NN. Consequently, to prove Theorem 1.1 for a fixed rr, it suffices to rule out every Ur(d,m)\mathsf U_r(d,m) with d/m≤rd/m \le\sqrt{r}.

Proof. For a positive integer ee and n=(n1,…,nr)∈Z≥0r\mathbf{n}=(n_1,\ldots,n_r)\in\mathbb{Z}_{\geq0}^r, let Ae,n⊆UrA_{e,\mathbf{n}}\subseteq U_r consist of the tuples admitting a nonzero degree-ee form with multiplicity at least nin_i at the iith point. In standard affine charts, the required Taylor coefficients give a matrix with (e+22)\binom{e+2}{2} columns, one for each form coefficient. Its entries are polynomials with integer coefficients in the point coordinates. A nonzero form exists exactly when the matrix has less than full column rank. Thus Ae,nA_{e,\mathbf{n}} is cut out by its full-column-size minors; if there are fewer rows than columns, the condition is automatic. Invariance of order makes these rank conditions agree on overlaps. Consequently Ae,nA_{e,\mathbf{n}} is Zariski closed and defined over Q\mathbb{Q}.

Let ErE_r be the union of all proper Ae,nA_{e,\mathbf{n}}. This is a countable union. On the dense chart where all points are affine, each proper Ae,nA_{e,\mathbf{n}} has a defining minor that is a nonzero polynomial over Q\mathbb{Q}. Choose 2r2r complex numbers algebraically independent over Q\mathbb{Q} as affine coordinates of the marked points. Such numbers can be chosen successively, since the algebraic closure of a countable field is countable. None of these minors vanishes at the resulting tuple, which also avoids the diagonals. Hence it lies in Ur∖ErU_r\setminus E_r.

Now suppose that a violation as in the statement occurs outside ErE_r. Then Ad0,m=UrA_{d_0,\mathbf{m}}=U_r. We use the cyclic-product reduction of Nagata [13]. Permuting the ordered points gives the same assertion for each cyclic shift of m\mathbf{m}. At any fixed tuple, choose a nonzero form for each of the rr cyclic shifts and take their product. This product is nonzero, and orders add because the product of the initial Taylor terms is nonzero. Each original multiplicity occurs once at each point. Hence the product has degree and common lower multiplicity

d=rd0,m=∑i=1rmi.d=rd_0,\qquad m=\sum_{i=1}^{r}m_i.

The assumed violation makes m>0m>0, and

dm=rd0∑imi≤r.\frac{d}{m}=\frac{rd_0}{\sum_i m_i}\leq\sqrt{r}.

The construction applies at every tuple, proving Ur(d,m)\mathsf U_r(d,m); taking NNth powers proves the common-multiple assertion. Thus excluding these universal systems excludes every violation outside the same ErE_r, for all degrees and multiplicity vectors. □\square

Specialization to a normal bundle

Let B⊆P2B\subseteq\mathbb{P}^2 be a smooth irreducible plane curve of degree k≥1k\geq1, and fix a nonzero homogeneous equation GBG_B for it. Put

L=OB(1),M=Lk.L=\mathcal{O}_B(1),\qquad M=L^k.

The equation identifies the normal bundle of BB in P2\mathbb{P}^2 with MM, as in the formula for an effective Cartier divisor [17 Tag 0B3P]. In a local frame ee for OP2(1)\mathcal{O}_{\mathbb{P}^2}(1), the local equation t=GB/ekt=G_B/e^k identifies a normal vector with its derivative under tt. For w∈Maw\in M_a, the expression fj(a)wjf_j(a)w^j is an element of LadL_a^d when fjf_j is a section of Ld−kjL^{d-kj}. Thus the polynomial in the next proposition is intrinsically a section of the pullback of LdL^d to Tot⁡(M)\operatorname{Tot}(M).

Proposition 2.2 (A necessary normal polynomial). Suppose that Ur(d,m)\mathsf U_r(d,m) holds. For every choice of distinct points a1,…,ar∈Ba_1,\ldots,a_r\in B and arbitrary vectors ci∈Maic_i\in M_{a_i}, there is a nonzero polynomial

F(w)=∑j=0⌊d/k⌋fjwj,fj∈H0(B,Ld−kj),F(w)=\sum_{j=0}^{\lfloor d/k\rfloor}f_jw^j,\qquad f_j\in H^0(B,L^{d-kj}),

having multiplicity at least mm at each (ai,ci)∈Tot⁡(M)(a_i,c_i) \in\operatorname{Tot}(M). Its coefficients may be taken to be algebraic sections.

Proof. We move the marked points in the plane, rescale the normal coordinate, and retain the first nonzero term of a family of plane forms.

Choose a plane affine chart and its standard frame near each aia_i. The differential of the local equation tit_i is nonzero by smoothness, so choose an affine tangent vector ViV_i with dti(Vi)=cid t_i(V_i)=c_i in that frame. The affine-linear motions

pi(s)=ai+sVip_i(s)=a_i+sV_i

are rational in ss, stay distinct for sufficiently small ss, and satisfy

lim⁡s→0ti(pi(s))s=ci\lim_{s\to0}\frac{t_i(p_i(s))}{s}=c_i

in the chosen frames. The vectors cic_i are arbitrary complex normal vectors; no compatibility among them is required.

Multiplicity at least mm at all pi(s)p_i(s) gives a homogeneous linear system over C(s)\mathbb{C}(s) in the degree-dd form coefficients. It has a nonzero solution: otherwise some full-column-size minor would be a nonzero rational function, giving full column rank at general complex values of ss and contradicting Ur(d,m)\mathsf U_r(d,m).

Clear denominators in a nonzero rational solution, and divide its polynomial coefficients by their maximal common power of ss. This gives a finite polynomial family of homogeneous degree-dd forms

S(s)=∑α≥0sαSα,S0≠0,S(s)=\sum_{\alpha\geq0}s^\alpha S_\alpha,\qquad S_0\ne0,

satisfying the required multiplicities for general ss. For each nonzero SαS_\alpha, factor out its largest power of GBG_B:

Sα=GBjαRα,0≤jα≤⌊d/k⌋.S_\alpha=G_B^{j_\alpha}R_\alpha,\qquad0\leq j_\alpha\leq\lfloor d/k\rfloor.

Then RαR_\alpha has degree d−kjαd-kj_\alpha and Rα∣B≠0R_\alpha|_B\ne0, since the homogeneous ideal of BB is generated by GBG_B.

Set

u=min⁡Sα≠0(α+jα),F(w)=∑α+jα=u(Rα∣B)wjα.u=\min_{S_\alpha\ne0}(\alpha+j_\alpha),\qquad F(w)=\sum_{\alpha+j_\alpha=u}(R_\alpha|_B)w^{j_\alpha}.

The sum is nonempty, and its terms have distinct exponents jαj_\alpha because α+jα=u\alpha+j_\alpha=u. Thus FF is nonzero, with algebraic coefficients of the types in (2.2).

It remains to identify this polynomial as the normal limit and pass the multiplicities to it.

Near a marked point choose a frame ee for OP2(1)\mathcal{O}_{\mathbb{P}^2}(1), put t=GB/ekt=G_B/e^k, and extend a local coordinate on BB to a holomorphic coordinate ζ\zeta off BB so that (ζ,t)(\zeta,t) are surface coordinates. Write rα(ζ,t)r_\alpha(\zeta,t) for the scalar expression of RαR_\alpha in the frame ed−kjαe^{d-kj_\alpha}. Substituting t=swt=sw in the local expression of S(s)S(s) and dividing by sus^u gives

Φ(s,ζ,w)=∑Sα≠0sα+jα−uwjαrα(ζ,sw).\Phi(s,\zeta,w)=\sum_{S_\alpha\ne0}s^{\alpha+j_\alpha-u}w^{j_\alpha}r_\alpha(\zeta,sw).

Every exponent of ss is nonnegative, so Φ\Phi extends holomorphically to s=0s=0 with value FF. Terms with α+jα>u\alpha+j_\alpha>u vanish there; in the remaining terms only rα(ζ,0)r_\alpha(\zeta,0) contributes. The limit respects the normal-bundle and value-bundle frames. Indeed, if e′=a(ζ,t)ee'=a(\zeta,t)e, then t′=a(ζ,t)−ktt'=a(\zeta,t)^{-k}t and the scalar expression of the section is multiplied by a(ζ,t)−da(\zeta,t)^{-d}. After t=swt=sw, the transitions at s=0s=0 are

w′=a(ζ,0)−kw,F′=a(ζ,0)−dF.w'=a(\zeta,0)^{-k}w,\qquad F'=a(\zeta,0)^{-d}F.

These are the transitions of MM and the pullback of LdL^d. Changing the extension of ζ\zeta off BB reduces at s=0s=0 to its coordinate change on BB, since the other terms contain t=swt=sw. Thus the local rescaling realizes the intrinsic polynomial FF above.

Finally fix an index ii and use such coordinates near aia_i. The functions

ζi(s)=ζ(pi(s)),wi(s)=t(pi(s))s\zeta_i(s)=\zeta(p_i(s)),\qquad w_i(s)=\frac{t(p_i(s))}{s}

extend holomorphically to s=0s=0, with values representing aia_i and cic_i. Translate the divided family to the lifted moving point:

Ψi(s,ξ,ω)=Φ(s,ζi(s)+ξ,wi(s)+ω).\Psi_i(s,\xi,\omega)=\Phi\bigl(s,\zeta_i(s)+\xi,w_i(s)+\omega\bigr).

For each general nonzero ss, the substitution t=swt=sw is a local biholomorphism of the surface, and multiplication by s−us^{-u} is multiplication by a nonzero scalar. The multiplicity assumption on S(s)S(s) therefore implies

∂ξa∂ωbΨi(s,0,0)=0(a,b≥0, a+b<m).\partial_\xi^a\partial_\omega^b\Psi_i(s,0,0)=0\qquad(a,b\geq0,\ a+b<m).

Each expression on the left is holomorphic at s=0s=0 and vanishes for general nonzero ss, hence also at zero. These are exactly the order-mm conditions for FF at (ai,ci)(a_i,c_i).

The square case

We use two basic facts about smooth projective curves. A nonzero section of a line bundle has an effective zero divisor whose degree is the degree of the bundle. In particular, a degree-zero line bundle has a nonzero section only if it is trivial. Also, for a smooth complex projective curve of positive genus, Pic⁡0(B)\operatorname{Pic}^0(B) is a complex torus; its subgroup of elements of any fixed finite order is finite, so its torsion subgroup is countable [17 Tag 0C1Z].

Proposition 2.3 (Strict inequality for square rr). Let r=k2r=k^2 with k≥4k\geq4. There are no positive integers d,md,m such that d≤kmd\leq km and Ur(d,m)\mathsf U_r(d,m) holds.

Proof. Suppose that d≤kmd\leq km and Ur(d,m)\mathsf U_r(d,m) holds. We choose the marked points to exclude normal polynomials of fiber degree below mm, and the displacements to exclude fiber degree mm. Take a smooth degree-kk plane curve BB, for example a Fermat curve, and retain L=OB(1)L=\mathcal{O}_B(1) and M=LkM=L^k. Its genus is (k−1)(k−2)/2>0(k-1)(k-2)/2>0, and deg⁡M=k2=r\deg M=k^2=r. Choose distinct points a1,…,ara_1,\ldots,a_r so that, with P=∑iaiP=\sum_i a_i, the degree-zero bundle

A=M(−P)A=M(-P)

is nontorsion. Such a choice exists: fix r−1r-1 distinct points and vary the last one. The map a↦OB(a)a\mapsto\mathcal{O}_B(a) is injective on a positive-genus curve, since a linear equivalence between two distinct single points would give a nonconstant meromorphic function with one simple pole, hence a degree-one map to P1\mathbb{P}^1, making the curve rational. Thus varying the last point gives uncountably many distinct bundles AA, while the torsion bundles are countable; the finitely many prohibited coincidences may also be avoided.

The restriction sequence

0⟶OP2→GBOP2(k)⟶OB(k)⟶00 \longrightarrow\mathcal{O}_{\mathbb{P}^2} \xrightarrow{G_B} \mathcal{O}_{\mathbb{P}^2}(k) \longrightarrow\mathcal{O}_B(k) \longrightarrow0

and H1(P2,OP2)=0H^1(\mathbb{P}^2,\mathcal{O}_{\mathbb{P}^2})=0 [17 Tag 01XT] give

h0(B,M)=(k+22)−1=k2+3k2<k2=r.h^0(B,M)=\binom{k+2}{2}-1=\frac{k^2+3k}{2}<k^2=r.

Hence one can choose c=(ci)i∈⨁iMaic=(c_i)_i\in\bigoplus_i M_{a_i} outside the image of the evaluation map

H0(B,M)⟶⨁i=1rMai.H^0(B,M)\longrightarrow\bigoplus_{i=1}^{r}M_{a_i}.

Apply Proposition 2.2 with these choices. Let jj be the largest exponent with fj≠0f_j\ne0. Then j≤⌊d/k⌋≤mj\le\lfloor d/k\rfloor\le m. If j<mj<m, take jj derivatives with respect to a local fiber coordinate. Since jj is the largest exponent, the result is j!fjj!f_j, independent of the fiber coordinate. Differentiation lowers order by at most jj, so fjf_j has base vanishing order at least m−jm-j at each aia_i. Its bundle has degree

deg⁡Ld−kj=k(d−kj)≤k2(m−j)=r(m−j).\deg L^{d-kj}=k(d-kj)\le k^2(m-j)=r(m-j).

Strict inequality is incompatible with these required zeros. Equality forces d=kmd=km, and removing the zeros then gives a nonzero section of

Lk(m−j)(−(m−j)P)=Am−j.L^{k(m-j)}(-(m-j)P)=A^{m-j}.

This is a nontrivial degree-zero bundle, because AA is nontorsion and m−j>0m-j>0, so it too has no nonzero section. Thus j<mj<m is impossible.

It follows that j=mj=m and d=kmd=km. In this case fmf_m is a nonzero constant. At each marked fiber the restriction of FF is a degree-mm polynomial, with leading coefficient fmf_m, having a zero of order at least mm at cic_i. In any compatible frame it therefore equals

F∣Mai(w)=fm(w−ci)m.F|_{M_{a_i}}(w)=f_m(w-c_i)^m.

Comparing the coefficient of wm−1w^{m-1} gives

(fm−1(ai))i=−mfm(ci)i.(f_{m-1}(a_i))_i=-mf_m(c_i)_i.

But fm−1∈H0(B,M)f_{m-1}\in H^0(B,M), and multiplication by the nonzero scalar −mfm-mf_m preserves the image of the evaluation map. This contradicts the choice of cc and finishes the proof.

Together with Lemma 2.1, the proposition proves Theorem 1.1 for square rr, including the strict inequality and unequal multiplicities.

Nine zero displacements on a cubic

For the remaining argument we will apply Proposition 2.2 with k=3k=3 and with zero normal displacements at nine distinct points of a smooth plane cubic. Write P=a1+⋯+a9P=a_1+\cdots+a_9. Extend the coefficient list by fj=0f_j=0 for j>⌊d/3⌋j>\lfloor d/3\rfloor. At each (ai,0)(a_i,0), expansion in the fiber variable shows that multiplicity at least mm implies

fj∈H0(B,Ld−3j(−(m−j)P))(0≤j<m).f_j\in H^0\left(B,L^{d-3j}(-(m-j)P)\right)\qquad(0\le j<m).

Indeed, in a local base coordinate ζ\zeta centered at aia_i, the coefficient of ζawj\zeta^a w^j must vanish whenever a+j<ma+j<m. Thus fjf_j has base order at least m−jm-j at every point of PP. The coefficient bundles in (2.3) all have degree 3(d−3m)3(d-3m), independent of jj. These conditions hold regardless of the additional points and normal displacements chosen in the proposition.

Lemma 2.4 (Excluding degree at most 3m3m). If r≥10r \ge10 and Ur(d,m)\mathsf U_r(d,m) holds for positive integers d,md,m, then d>3md>3m.

Proof. Suppose first that d<3md<3m. Choose a smooth plane cubic and nine distinct points with zero normal displacements, as above, completing them to rr distinct base points with arbitrary further displacements. Every exponent occurring in (2.2) is less than mm. For each such exponent, (2.3) prescribes at least 9(m−j)9(m-j) zeros, whereas

deg⁡Ld−3j=3(d−3j)<9(m−j).\deg L^{d-3j}=3(d-3j)<9(m-j).

Thus every coefficient is zero, contradicting the nonzero polynomial provided by Proposition 2.2. Now suppose that d=3md=3m. A smooth plane cubic has genus one. Choose the nine points so that A=L3(−P)A=L^3(-P) is nontorsion, by the same argument used in the square case. Complete them to rr distinct base points, choosing a nonzero vector c10∈Ma10c_{10}\in M_{a_{10}}; this is possible because r≥10r\ge10. Apply Proposition 2.2 with these choices and zero displacements at the first nine points. For every j<mj<m, the bundle in (2.3) is Am−jA^{m-j}, a nontrivial degree-zero bundle. Hence these coefficients vanish, and the nonzero normal polynomial must be F(w)=fmwmF(w)=f_mw^m for a nonzero constant fmf_m. This is nonzero at (a10,c10)(a_{10},c_{10}), so it cannot have multiplicity at least m≥1m\ge1 there. This is again a contradiction. □

Polynomial sections on an elliptic curve

Nine zero normal displacements impose zeros on the coefficients of a normal polynomial. Dividing out these zeros puts its first m+1m+1 coefficients in bundles of the same positive degree. We first make this change intrinsically on any smooth cubic. We then choose cubics and marked points for which theta functions give explicit bases of the resulting spaces, ready for the collision and limit in Section 4.

In this section and Section 4, H0H^0 denotes holomorphic sections. The algebraic sections supplied by Proposition 2.2 belong to these spaces, so excluding holomorphic solutions will also exclude the necessary normal polynomials.

Removing the nine prescribed coefficient zeros

For this construction, let d,md,m be any positive integers with d>3md>3m. Let BB be a smooth plane cubic, let L=OB(1)L=\mathcal{O}_B(1) and M=L3M=L^3, and choose nine distinct points with divisor P=a1+⋯+a9P=a_1+\cdots+a_9. Write σP\sigma_P for the canonical section of OB(P)\mathcal{O}_B(P) with zero divisor PP, and put

A=M⊗OB(−P),T=Ld−3m,u0=⌊d/3⌋.A=M\otimes\mathcal{O}_B(-P),\qquad T=L^{d-3m},\qquad u_0=\lfloor d/3\rfloor.

Thus deg⁡A=0\deg A=0 and deg⁡T=3(d−3m)>0\deg T=3(d-3m)>0. Multiplication by σP\sigma_P defines a bundle map A→MA\to M, written

w=σPv,w=\sigma_Pv,

which is invertible over B∖PB\setminus P. Define coefficient spaces inside H0(B,T⊗Am−j)H^0(B,T\otimes A^{m-j}) by

Vj={H0(B,T⊗Am−j),0≤j≤m,σPj−mH0(B,Ld−3j),m<j≤u0.(2)V_j= \begin{cases} H^0(B,T\otimes A^{m-j}), & 0\le j\le m,\\ \sigma_P^{j-m}H^0(B,L^{d-3j}), & m<j\le u_0. \end{cases} \tag*{(2)}

Negative powers denote dual powers. The target in the second line is correct because

Ld−3j⊗OB((j−m)P)=T⊗Am−j.L^{d-3j} \otimes\mathcal{O}_B((j-m)P) = T \otimes A^{m-j}.

Multiplication by σPj−m\sigma_P^{j-m} is injective, as can be checked on B∖PB \setminus P. Let WW be the space of polynomial sections on Tot⁡(A)\operatorname{Tot}(A)

F~(v)=∑j=0u0gjvj,gj∈Vj,\widetilde{F}(v) = \sum_{j=0}^{u_0} g_j v^j,\qquad g_j \in V_j,

valued in the pullback of T⊗Am=Ld(−mP)T \otimes A^m = L^d(-mP). It is a finite-dimensional space: its coefficient blocks are spaces of sections on the compact curve BB, and distinct powers of the fiber coordinate make their sum direct.

The nine zero displacements are now built into WW. The remaining points impose ordinary multiplicities at scalar fiber coordinate 11, as follows.

Proposition 3.1. Suppose r≥10r \ge10, d>3md > 3m, and Ur(d,m)\mathsf U_r(d,m) holds. Choose BB, PP, AA and WW as above, and fix a holomorphic frame of AA on a coordinate disk in B∖PB \setminus P. For every choice of q=r−9q = r - 9 distinct points b1,…,bqb_1,\ldots,b_q in this disk, there is a nonzero F~∈W\widetilde{F} \in W of multiplicity at least mm at each point (bα,1)(b_\alpha,1) of Tot⁡(A)\operatorname{Tot}(A), where 11 is the scalar coordinate in the chosen frame.

Proof. Apply Proposition 2.2 at the distinct points a1,…,a9,b1,…,bqa_1,\ldots,a_9,b_1,\ldots,b_q. Take zero normal displacements at the aia_i. At bαb_\alpha, take the image under multiplication by σP\sigma_P of the vector with scalar coordinate 11 in the chosen frame of AA. The normal-polynomial proposition allows these arbitrary normal vectors, so it supplies a nonzero

F(w)=∑j=0u0fjwj,fj∈H0(B,Ld−3j),F(w) = \sum_{j=0}^{u_0} f_j w^j,\qquad f_j \in H^0(B,L^{d-3j}),

with the required multiplicities.

By (2.3), fjf_j vanishes along (m−j)P(m-j)P for j<mj < m. Consequently the expression

F~(v)=σP−mF(σPv)=∑j=0u0fjσPj−mvj\widetilde{F}(v) = \sigma_P^{-m}F(\sigma_Pv) = \sum_{j=0}^{u_0} f_j\sigma_P^{j-m}v^j

extends across PP. The prescribed zeros cancel its negative powers of σP\sigma_P, and its coefficients have exactly the forms in (2). It therefore belongs to WW and is nonzero, since the fiber substitution is invertible on B∖PB \setminus P.

Near each bαb_\alpha, w=σPvw = \sigma_Pv is a nonsingular change of surface coordinates. The value-bundle map given by multiplication by σP−m\sigma_P^{-m} is also invertible there; in local frames it is multiplication by a holomorphic unit. These two operations preserve ordinary order of vanishing and take the displaced point to (bα,1)(b_\alpha,1). □

We next realize these coefficient spaces on explicit elliptic curves. Their bases will retain the bundle multipliers, not merely their degrees; those multipliers determine the Laurent exponents in the limit.

Theta functions and plane cubics

For 0<τ<10 < \tau< 1, let

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

This is a connected compact complex torus of dimension one. For n∈Zn \in\mathbb{Z} and γ∈C∗\gamma\in\mathbb{C}^*, define D(n,γ)D(n,\gamma) as the holomorphic line bundle obtained from C∗×C\mathbb{C}^* \times\mathbb{C} by the action generated by

(z,t)⟼(τz,γz−nt).(z,t) \longmapsto(\tau z,\gamma z^{-n}t).

In its covering-space frame, sections are holomorphic functions with

f(τz)=γz−nf(z),f(\tau z) = \gamma z^{-n}f(z),

and ordinary multiplication gives the tensor identifications

D(n,γ)⊗D(n′,γ′)=D(n+n′,γγ′).D(n,\gamma) \otimes D(n',\gamma') = D(n+n',\gamma\gamma').

Define

Θτ(z)=∏p=0∞(1−τpz)∏p=1∞(1−τp/z).\Theta_\tau(z) = \prod_{p=0}^{\infty}(1-\tau^p z)\prod_{p=1}^{\infty}(1-\tau^p/z).

We write Θ\Theta when τ\tau is fixed. On every compact annulus, the sums of the absolute deviations of the factors from 11 are bounded by geometric series. The products therefore converge locally uniformly on C∗\mathbb{C}^*, and reindexing gives

Θ(τz)=−z−1Θ(z).\Theta(\tau z) = -z^{-1}\Theta(z).

Its zeros are precisely the points of τZ\tau^{\mathbb{Z}}, all simple: exactly one factor vanishes at each, while the remaining product is nonzero. Thus Θ(z/a)\Theta(z/a) is a section of D(1,−a)D(1,-a) with divisor the single point represented by a∈C∗a \in\mathbb{C}^*. Products of nn such sections, with the parameters having product (−1)nγ(-1)^n\gamma, show that D(n,γ)D(n,\gamma) has degree nn for n>0n > 0. Tensor products and duals give the formula for every integer nn; in degree zero, use D(0,γ)=D(1,γ)⊗D(1,1)−1D(0,\gamma) = D(1,\gamma) \otimes D(1,1)^{-1}.

The multiplicative theta convention and residue-class bases are classical; see Rosengren [16], arXiv version, Section 1.2 and Exercise 1.6.5. We include the proof to fix all multipliers and normalizations.

Lemma 3.2. For n>0n > 0 and γ∈C∗\gamma\in\mathbb{C}^*, the space H0(Xτ,D(n,γ))H^0(X_\tau,D(n,\gamma)) has dimension nn. The Laurent coefficients of a section f(z)=∑K∈ZcKzKf(z) = \sum_{K \in\mathbb{Z}} c_K z^K satisfy

cK+n=γ−1τKcK,c_{K+n} = \gamma^{-1}\tau^K c_K,
cK+np=cKγ−pτpK+np(p−1)/2(p∈Z).(3)c_{K+np} = c_K\gamma^{-p}\tau^{pK+np(p-1)/2}\qquad(p \in\mathbb{Z}). \tag*{(3)}

One coefficient in each residue class modulo nn may be prescribed arbitrarily. Taking one nonzero starting coefficient at a time gives a basis supported in the individual residue classes.

Proof. A holomorphic function on C∗\mathbb{C}^* has a Laurent expansion convergent on compact annuli. Comparing coefficients in its functional equation gives τKcK=γcK+n\tau^K c_K = \gamma c_{K+n}; iteration in either direction proves (3).

Conversely, prescribe one coefficient per residue class and extend by the recurrence. For a fixed starting exponent KK, the terms on any compact annulus are bounded by

Cexp⁡(−cp2+C′∣p∣),c>0,C\exp(-cp^2+C'|p|),\qquad c>0,

because n>0n > 0 and log⁡τ<0\log\tau< 0. The resulting Laurent series converges normally and satisfies the functional equation. There are exactly nn free coefficients, and uniqueness of Laurent expansions proves the basis assertion. ∎

Lemma 3.3. For every γ∈C∗\gamma\in\mathbb{C}^{*}, the complete space of sections of D(3,γ)D(3,\gamma) embeds XτX_{\tau} into P2\mathbb{P}^{2} as a smooth irreducible plane cubic, with OP2(1)\mathcal{O}_{\mathbb{P}^{2}}(1) pulling back to D(3,γ)D(3,\gamma).

Proof. Let QQ be an effective divisor of degree t∈{1,2}t \in\{1,2\}. A product of tt theta factors, using lifts of its points with their multiplicities, is a section with divisor exactly QQ. Division by this product identifies sections of D(3,γ)D(3,\gamma) vanishing along QQ with sections of some D(3−t,γ′)D(3-t,\gamma'). Their dimension is 3−t3-t by Lemma 3.2.

For t=1t=1, this proves that the three-dimensional section space has no base points. For two distinct points it shows that the associated map separates them. For Q=2pQ=2p, the dimension drop from sections vanishing at pp to those vanishing twice supplies a section of order exactly one at pp. Its ratio with a section nonzero there has nonzero derivative. The map is therefore an injective holomorphic immersion, and compactness makes it an embedding.

By Chow’s Theorem [2], the closed analytic image is algebraic. It is smooth and irreducible because it is an embedded connected compact Riemann surface. Its hyperplane bundle pulls back to D(3,γ)D(3,\gamma), of degree three, so the image is a plane cubic.

Choosing the cubic and marked points

We now fix a nonsquare integer r≥10r \ge10 and a hypothetical universal system Ur(d,m)\mathsf U_r(d,m) with d/m≤rd/m \le\sqrt{r}. The rationality of d/md/m and Lemma 2.4 give 3<d/m<r3 < d/m < \sqrt{r}. Set

q=r−9,ρ=3(d/m−3),ρ∗=3(r−3),q=r-9,\qquad\rho=3(d/m-3),\qquad\rho_{*}=3(\sqrt{r}-3),
0<ρ<ρ∗,2ρ∗+ρ∗29=q.(4)0<\rho<\rho_{*},\qquad2\rho_{*}+\frac{\rho_{*}^{2}}{9}=q. \tag*{(4)}

Put

h=3(d−3m)=mρ>0,u0=⌊d/3⌋≥m.h=3(d-3m)=m\rho>0,\qquad u_{0}=\lfloor d/3\rfloor\ge m.

Set x0=1/2x_{0}=1/2 and choose a rational number Δ\Delta such that

0<Δ<x0,ρ+Δρ9<ρ∗.(5)0<\Delta<x_{0},\qquad\rho+\frac{\Delta\rho}{9}<\rho_{*}. \tag*{(5)}

The strict slope gap leaves an interval of such choices. Rationality of Δ\Delta will keep the Laurent exponent intervals away from integral endpoints.

Choose nine distinct real numbers xix_i with

0<xi<x0,∑i=19(x0−xi)=Δ,(6)0<x_i<x_{0},\qquad\sum_{i=1}^{9}(x_{0}-x_i)=\Delta, \tag*{(6)}
η=∑i=19xi+ρ∗3,zi=τxi (1≤i≤9),z0=τx0.\eta=\frac{\sum_{i=1}^{9}x_i+\rho_{*}}{3},\qquad z_i=\tau^{x_i}\ (1\le i\le9),\qquad z_0=\tau^{x_0}.

For example, take xi=x0−iΔ/45x_i=x_0-i\Delta/45. The quantities ρ\rho, Δ\Delta, xix_i, η\eta can be kept unchanged under a common multiple of (d,m)(d,m), whereas hh, u0u_0 and the coefficient spaces depend on the actual pair. We keep this pair fixed while taking the collision on each curve and the subsequent limit in τ\tau.

For each 0<τ<10<\tau<1, use Lemma 3.3 to identify XτX_{\tau} with a plane cubic BB, with the holomorphic identification

L=OB(1)=D(3,τη),M=L3.L=\mathcal{O}_{B}(1)=D(3,\tau^{\eta}),\qquad M=L^{3}.

Let aia_i be the point represented by ziz_i and put P=a1+⋯+a9P=a_1+\cdots+a_9. These points and the point represented by z0z_0 are distinct: their exponents lie in (0,1)(0,1), and two lifts represent the same point only if their exponents differ by an integer.

In the covering-space frame, the section

Π(z)=∏i=19Θ(z/zi)\Pi(z)=\prod_{i=1}^{9}\Theta(z/z_i)

has divisor PP and gives an identification

OB(P)=D(9,−τ∑ixi)\mathcal{O}_B(P)=D\left(9,-\tau^{\sum_i x_i}\right)

under which the canonical section σP\sigma_P is represented by Π(z)\Pi(z). Thus the bundles already used in the construction are

A=M⊗OB(−P),T=Ld−3m.A=M\otimes\mathcal{O}_B(-P),\qquad T=L^{d-3m}.

Since 3η=∑ixi+ρ∗3\eta=\sum_i x_i+\rho_*, we have

A=D(0,−τρ∗),deg⁡T=h,T⊗Am=Ld⊗OB(−mP).A=D(0,-\tau^{\rho_*}),\qquad\deg T=h,\qquad T\otimes A^m=L^d\otimes\mathcal{O}_B(-mP).

These identifications use the covering-space frames and their tensor products. We retain the displayed powers of τ\tau as written, without replacing the multiplier presentations by isomorphic ones.

A cubic equation identifies the normal bundle of BB with M=L3M=L^3. Its differential at each point surjects onto the normal fiber, so every scalar specified in the chosen covering-space frame is an allowed normal displacement in Proposition 2.2. Rescaling the cubic equation does not restrict those choices. All constructions are made for each fixed τ\tau; their algebraic dependence on τ\tau is not required.

Denote the resulting polynomial space by Wτ\mathcal{W}_\tau. By Lemma 3.2, its first m+1m+1 coefficient blocks have degree and dimension hh. For j>mj>m, the dimension is 3(d−3j)3(d-3j) when d−3j>0d-3j>0, and is one when d−3j=0d-3j=0. In the last case the source is H0(B,OB)=CH^0(B,\mathcal{O}_B)=\mathbb{C}, since BB is compact and connected.

Near the point represented by (z,v)=(z0,1)(z,v)=(z_0,1), use coordinates

z=z0ex,v=ey.z=z_0e^x,\qquad v=e^y.

Choose the xx-disk small enough to map injectively to BB and avoid PP, and the yy-disk small enough that eye^y is injective. In the fixed covering-space frame of T⊗AmT\otimes A^m, the scalar expression is

F~(x,y)=∑j=0u0gj(z0ex)ejy.\widetilde{F}(x,y)=\sum_{j=0}^{u_0}g_j(z_0e^x)e^{jy}.

Here gj(z)g_j(z) denotes the holomorphic function in its covering-space frame; all summands take values in the same bundle.

For every fixed τ∈(0,1)\tau\in(0,1) and every qq distinct positions ξ1,…,ξq\xi_1,\ldots,\xi_q sufficiently near zero, apply Proposition 3.1 in this disk and the fixed frame of AA. It gives a nonzero F~∈Wτ\widetilde{F}\in\mathcal{W}_\tau of multiplicity at least mm at each (x,y)=(ξα,0)(x,y)=(\xi_\alpha,0), since v=1v=1 corresponds to y=0y=0. The existence is pointwise in τ\tau and in the tuple of positions; the collision will use no simultaneous choice of sections.

Colliding points and degenerating sections

We turn the multiplicities at the remaining qq points into derivative conditions at one point of Tot⁡(A)\operatorname{Tot}(A). Universal existence will force these conditions to have a nonzero solution in Wτ\mathcal{W}_\tau. We then choose bases whose derivative matrices have an explicit limit as τ→0+\tau\to0^+. Section 5 will prove full column rank when the common multiplicity is sufficiently large at a fixed ratio d/md/m.

All choices from Section 3, including dd, mm, qq, hh, u0u_0 and ρ\rho, ρ∗\rho_*, Δ\Delta, xix_i, x0x_0, η\eta, remain fixed. The collision takes place with τ\tau fixed, before the matrix limit in τ\tau.

Collision on a fixed surface

The collision below belongs to the broader study of limits of fat-point conditions; compare Evain [10], Sections 2 and 6. We prove the particular local constraint directly.

For each fixed τ\tau, use the coordinates and the frame in (3.7). If F∈WτF \in\mathcal{W}_{\tau} has coefficients gjg_j, write its scalar expression in this chart as

HF(x,y)=∑j=0u0gj(z0ex)ejy.H_F(x,y)=\sum_{j=0}^{u_0}g_j(z_0e^x)e^{jy}.

Define the finite index set

I={(ℓ,b)∈Z≥02:0≤b<m,0≤ℓ<q(m−b)}.\mathcal{I}=\{(\ell,b)\in\mathbb{Z}_{\geq0}^{2}:0\leq b<m,\quad0\leq\ell<q(m-b)\}.

and the linear map Jτ:Wτ⟶CIJ_{\tau}:\mathcal{W}_{\tau}\longrightarrow\mathbb{C}^{\mathcal{I}} whose coordinates are

(JτF)ℓ,b=∂xℓ∂ybHF(x,y)∣(0,0),0≤b<m,0≤ℓ<q(m−b).(7)(J_{\tau}F)_{\ell,b}=\left.\partial_x^{\ell}\partial_y^bH_F(x,y)\right|_{(0,0)},\qquad0\leq b<m,\quad0\leq\ell<q(m-b). \tag*{(7)}

The value bundle is expressed in one fixed local frame when these derivatives are taken.

Lemma 4.1 (Collision of the further points). If Ur(d,m)\mathsf U_r(d,m) holds, then ker⁡Jτ≠{0}\ker J_{\tau}\ne\{0\} for every fixed τ∈(0,1)\tau\in(0,1).

Proof. Fix τ\tau. Choose a sequence of ordered tuples (ξ1,ν,…,ξq,ν)(\xi_{1,\nu},\ldots,\xi_{q,\nu}) of distinct points in the xx-coordinate disk, all tending to zero. By Proposition 3.1, there is a nonzero Fν∈WτF_{\nu}\in\mathcal{W}_{\tau} with multiplicity at least mm at every (ξa,ν,0)(\xi_{a,\nu},0).

Fix a basis of the finite-dimensional space Wτ\mathcal{W}_{\tau} and normalize the coefficient vector of each FνF_{\nu} to have Euclidean norm one. A subsequence converges to a unit vector, defining a nonzero F0∈WτF_0\in\mathcal{W}_{\tau}: the coefficient blocks in (2) form a direct sum. As the basis and chart are fixed, coefficient convergence gives locally uniform convergence of HFνH_{F_{\nu}} and all of its derivatives.

For 0≤b<m0\leq b<m, set

hb,ν(x)=∂ybHFν(x,0),hb,0(x)=∂ybHF0(x,0).h_{b,\nu}(x)=\partial_y^bH_{F_{\nu}}(x,0),\qquad h_{b,0}(x)=\partial_y^bH_{F_0}(x,0).

Multiplicity at least mm at (ξa,ν,0)(\xi_{a,\nu},0) implies

ord⁡ξa,νhb,ν≥m−b(1≤a≤q).\operatorname{ord}_{\xi_{a,\nu}}h_{b,\nu}\geq m-b\qquad(1\leq a\leq q).

If hb,0h_{b,0} is identically zero, all of its required jets already vanish. Otherwise choose a small closed disk centered at zero, contained in the coordinate disk, on which hb,0h_{b,0} has no zeros except possibly at zero and has none on the boundary. For all sufficiently large ν\nu, every ξa,ν\xi_{a,\nu} is inside this disk, and uniform convergence on its boundary implies that hb,νh_{b,\nu} and hb,0h_{b,0} have the same number of zeros there, counted with multiplicity. The argument principle, or Rouché’s Theorem, therefore gives

ord⁡0hb,0≥q(m−b).\operatorname{ord}_0h_{b,0}\geq q(m-b).

This holds for every b<mb<m, and is exactly JτF0=0J_{\tau}F_0=0.

The rows in (7) describe a local ideal. If the distinct centers are (ξa,0)(\xi_a,0) and Q(x)=∏a=1q(x−ξa)Q(x)=\prod_{a=1}^{q}(x-\xi_a), write a local holomorphic function as ∑b≥0hb(x)yb\sum_{b\geq0}h_b(x)y^b. The multiplicity conditions require Qm−bQ^{m-b} to divide hbh_b for b<mb<m. When the centers collide, the corresponding limiting conditions are divisibility by xq(m−b)x^{q(m-b)}, or membership in (xq,y)m(x^q,y)^m. Their number is

∣I∣=∑b=0m−1q(m−b)=qm(m+1)2.|\mathcal{I}|=\sum_{b=0}^{m-1}q(m-b)=\frac{qm(m+1)}{2}.

Lemma 4.1 establishes these conditions for a nonzero limit. It remains to compute the matrix of JτJ_\tau in bases suited to τ→0+\tau\to0^+.

A common chart and normalized theta sections

Although the tori vary, one polydisk in (x,y)(x,y) is a valid chart for all sufficiently small positive τ\tau. Fix RR with 0<R<π/20<R<\pi/2, and let

δP=min⁡1≤i≤9{x0−xi,1−(x0−xi)}>0.\delta_P=\min_{1\leq i\leq9}\{x_0-x_i,1-(x_0-x_i)\}>0.

For small enough τ\tau, require ∣log⁡τ∣>2R|\log\tau|>2R and δP∣log⁡τ∣>R\delta_P|\log\tau|>R. If z0exz_0e^x and z0ex′z_0e^{x'}, with ∣x∣,∣x′∣<R|x|,|x'|<R, represent the same point of XτX_\tau, then

x′−x=alog⁡τ+2πib(a,b∈Z).x'-x=a\log\tau+2\pi ib\qquad(a,b\in\mathbb{Z}).

The bounds on the real and imaginary parts force a=b=0a=b=0. Thus this disk maps injectively to XτX_\tau. If a point of the disk represented a point of PP, its real coordinate would satisfy

Re⁡x=(xi−x0+a)log⁡τfor some i and a∈Z,\operatorname{Re}x=(x_i-x_0+a)\log\tau\qquad\text{for some }i\text{ and }a\in\mathbb{Z},

whose absolute value is at least δP∣log⁡τ∣>R\delta_P|\log\tau|>R. Hence the disk avoids PP. The covering-space frame trivializes AA there, and v=eyv=e^y is injective for ∣y∣<R|y|<R. Thus (3.7) gives the common polydisk ∣x∣,∣y∣<R|x|,|y|<R around the marked point on Tot⁡(A)\operatorname{Tot}(A). We continue to use the covering-space frames of Section 3.

Lemma 4.2 (Normalized theta sections). Fix an integer n>0n>0, a real number σ\sigma, and a complex number ϵ\epsilon with ∣ϵ∣=1|\epsilon|=1. Put U=σ−x0nU=\sigma-x_0n and assume U∉ZU\notin\mathbb{Z}. For each integer KK with U<K<U+nU<K<U+n, there is a section sK,τs_{K,\tau} of D(n,ϵτσ)D(n,\epsilon\tau^\sigma) obtained from the Laurent recurrence (3.3) by setting the coefficient of zKz^K equal to τ−x0K\tau^{-x_0K} and all other residue classes modulo nn equal to zero. These nn sections form a basis. In the local covering-space frame their expressions are

sK,τ(z0ex)=∑p∈Zϵ−pτp(K−U)+np(p−1)/2e(K+np)x⟶eKx.(8)s_{K,\tau}(z_0e^x)=\sum_{p\in\mathbb{Z}}\epsilon^{-p}\tau^{p(K-U)+np(p-1)/2}e^{(K+np)x}\longrightarrow e^{Kx}. \tag*{(8)}

The convergence is uniform on each compact subset of the complex xx-plane, and the same is true after any fixed number of xx-derivatives. Moreover,

Π(z0ex)⟶1\Pi(z_0e^x)\longrightarrow1

with the same uniform holomorphic and derivative convergence.

Proof. Because U∉ZU\notin\mathbb{Z}, the interval (U,U+n)(U,U+n) contains nn integers, one in each residue class modulo nn. The chosen starting coefficients therefore give a basis by Lemma 3.2. The recurrence yields

cK+np=τ−x0Kϵ−pτ−σp+pK+np(p−1)/2.c_{K+np}=\tau^{-x_0K}\epsilon^{-p}\tau^{-\sigma p+pK+np(p-1)/2}.

Substitution of z=z0ex=τx0exz=z_0e^x=\tau^{x_0}e^x gives the series in (8).

Write a=K−U∈(0,n)a=K-U\in(0,n) and δ=min⁡{a,n−a}>0\delta=\min\{a,n-a\}>0. For each integer t≥1t\ge1, the exponent of τ\tau in the term with p=tp=t is

ta+nt(t−1)2.ta+\frac{nt(t-1)}{2}.

and in the term with p=−tp=-t it is

t(n−a)+nt(t−1)2.t(n-a)+\frac{nt(t-1)}{2}.

Both are at least δt\delta t. Their quadratic growth gives normal convergence on compact xx-disks for each fixed τ\tau, permitting termwise differentiation. On ∣x∣≤R′|x|\le R', the contribution of all terms with p≠0p\ne0 to the derivative of order c≥0c\ge0 has absolute value at most

2e∣K∣R′∑t≥1(∣K∣+nt)c(enR′τδ)t.2e^{|K|R'}\sum_{t\ge1} (|K|+nt)^c\left(e^{nR'}\tau^\delta\right)^t.

For sufficiently small τ\tau, the quantity in parentheses is at most 1/21/2. The sum is then bounded by a constant, depending only on R′R', cc, nn, KK, times τδ\tau^\delta, and tends to zero. The p=0p=0 term is eKxe^{Kx}. This proves the asserted convergence of the sections and all fixed derivatives on any compact disk.

For the product, put ai=x0−xi∈(0,1)a_i=x_0-x_i\in(0,1). The factors of Θ(τaiex)\Theta(\tau^{a_i}e^x) differ from 1 by terms whose total absolute value on ∣x∣≤R′|x|\le R' is at most

eR′(∑p=0∞τp+ai+∑p=1∞τp−ai)=eR′1−τ(τai+τ1−ai).e^{R'}\left(\sum_{p=0}^{\infty}\tau^{p+a_i}+\sum_{p=1}^{\infty}\tau^{p-a_i}\right) =\frac{e^{R'}}{1-\tau}\left(\tau^{a_i}+\tau^{1-a_i}\right).

Summing over the nine indices gives a quantity SR′(τ)S_{R'}(\tau) tending to zero. The elementary product bound

∣∏ν(1+uν)−1∣≤exp⁡(∑ν∣uν∣)−1\left|\prod_\nu(1+u_\nu)-1\right|\le\exp\left(\sum_\nu|u_\nu|\right)-1

holds for an absolutely summable family by passage from finite products. It bounds ∣Π(z0ex)−1∣|\Pi(z_0e^x)-1| uniformly by exp⁡(SR′(τ))−1\exp(S_{R'}(\tau))-1. The product converges normally on compact disks for each τ\tau, so its expressions are holomorphic. Applying the uniform bound on a slightly larger disk and then using Cauchy’s derivative estimates proves convergence of every fixed derivative on the original disk. □

Bases for the polynomial spaces

We now apply Lemma (8) to the actual coefficient spaces of Wτ\mathcal{W}_\tau. For 0≤j≤m0\le j\le m, their bundle is

T⊗Am−j=D(h,(−1)m−jτ(d−3m)η+(m−j)ρ∗).T\otimes A^{m-j}=D\left(h,(-1)^{m-j}\tau^{(d-3m)\eta+(m-j)\rho_*}\right).

Since η−3x0=(ρ∗−Δ)/3\eta-3x_0=(\rho_*-\Delta)/3, its interval parameter is

Uj=h9(ρ∗−Δ)+(m−j)ρ∗.U_j=\frac{h}{9}(\rho_*-\Delta)+(m-j)\rho_*.

For m<j≤u0m<j\le u_0 with d−3j>0d-3j>0, the space in (2) is the image of the sections of

Ld−3j=D(nj,τ(d−3j)η),nj=3(d−3j)=h−9(j−m)>0,L^{d-3j}=D\left(n_j,\tau^{(d-3j)\eta}\right),\qquad n_j=3(d-3j)=h-9(j-m)>0,

under multiplication by Πj−m\Pi^{j-m}. The interval parameter for this source bundle is

Uj=nj9(ρ∗−Δ).U_j=\frac{n_j}{9}(\rho_*-\Delta).

These parameters are irrational. Indeed, after substituting ρ∗=3(r−3)\rho_* = 3(\sqrt{r} - 3), the coefficient of r\sqrt{r} in either expression is the positive integer d−3jd - 3j, and the remaining terms are rational because Δ∈Q\Delta\in\mathbb{Q}. In particular,

Uj∉Z(0≤j≤u0, d−3j>0).(9)U_j \notin\mathbb{Z} \qquad(0 \le j \le u_0,\ d - 3j > 0). \tag*{(9)}

The finite exponent set is

S=⋃j=0m{(j,K):K∈Z, Uj<K<Uj+h}\mathcal{S} = \bigcup_{j=0}^{m} \{(j,K): K \in\mathbb{Z},\ U_j < K < U_j + h\}
∪⋃m<j≤u0d−3j>0{(j,K):K∈Z, Uj<K<Uj+nj}\cup\bigcup_{\substack{m<j\le u_0\\d-3j>0}} \{(j,K): K \in\mathbb{Z},\ U_j < K < U_j + n_j\}
∪{(j,0):m<j≤u0, d−3j=0},nj=h−9(j−m).(10)\cup\{(j,0): m<j\le u_0,\ d-3j=0\}, \qquad n_j = h - 9(j-m). \tag*{(10)}

All indices jj in this definition are integers. The last set is empty unless 33 divides dd, and otherwise consists of the single pair (d/3,0)(d/3,0). Because d>3md > 3m, that pair has j>mj > m.

For a pair (j,K)(j,K) in the first union, choose the normalized section from Lemma 4.2 in H0(B,T⊗Am−j)H^0(B,T\otimes A^{m-j}) as the coefficient of vjv^j. For a pair in the second union, choose the normalized section in H0(B,Ld−3j)H^0(B,L^{d-3j}), multiply it by Πj−m\Pi^{j-m}, and use the result as the coefficient of vjv^j. For the last union, use Πj−m\Pi^{j-m} as the coefficient of vjv^j: the source space is H0(B,L0)=CH^0(B,L^0)=\mathbb{C}, with basis the constant section 11. Denote the resulting fiber polynomials by Ej,K,τE_{j,K,\tau}.

Each choice gives a basis of its coefficient block. For j>mj > m, multiplication by Πj−m\Pi^{j-m} is injective, since Π\Pi is nonzero on B∖PB\setminus P, and its image is the block by definition. The different powers vjv^j form a direct sum. Hence

{Ej,K,τ:(j,K)∈S}\{E_{j,K,\tau}:(j,K)\in\mathcal{S}\}

is a basis of WτW_\tau for every τ∈(0,1)\tau\in(0,1). There are no duplicate pairs, and the index set is independent of τ\tau.

The block dimensions also give the useful identity

∣S∣=dim⁡Wτ=(d+22)−9(m+12).|\mathcal{S}| = \dim W_\tau= \binom{d+2}{2} - 9\binom{m+1}{2}.

To see this, sum the dimensions 3(d−3j)3(d-3j) of H0(B,Ld−3j)H^0(B,L^{d-3j}) for d−3j>0d-3j>0 and add one when 33 divides dd. The result is (d+22)\binom{d+2}{2}. For j<mj<m, the coefficient condition in (2.3) reduces the block dimension by 9(m−j)9(m-j); their sum is 9(m+12)9\binom{m+1}{2}.

In the common local chart, the scalar expressions of this basis satisfy

HEj,K,τ(x,y)⟶eKx+jy((j,K)∈S)H_{E_{j,K,\tau}}(x,y) \longrightarrow e^{Kx+jy} \qquad((j,K)\in\mathcal{S})

locally uniformly, together with all fixed mixed derivatives. For the first union this is (4.2) times ejye^{jy}. For the second union, the additional factor Π(z0ex)j−m\Pi(z_0e^x)^{j-m} tends to 11 with all derivatives by Lemma 4.2; the exponent j−mj-m is fixed. The same product assertion proves the claim for the degree-zero case with K=0K=0. As S\mathcal{S} is finite, all of these convergences can be taken on one fixed smaller polydisk and for the same sufficiently small values of τ\tau.

The limiting jet matrix

Evaluation of monomials in exponent pairs is a useful way to express interpolation rank. Dumnicki [7 proof of Proposition 13] uses this principle to relate a one-point multiplicity matrix to polynomial evaluation on a diagram. Here the normalized theta sections produce the exponent pairs directly, with the derivative indices prescribed by the preceding collision.

Proposition 4.3. Choose fixed orderings of I\mathcal{I} and S\mathcal{S}, and represent JτJ_\tau in the basis Ej,K,τE_{j,K,\tau} by the matrix BτB_\tau. These matrices have one fixed size and converge entrywise as τ→0+\tau\to0^{+} to the matrix

B0=(Kℓjb)(ℓ,b)∈I(j,K)∈S.(11)B_0 = \left(K^\ell j^b\right)_{\substack{(\ell,b)\in\mathcal{I}\\(j,K)\in\mathcal{S}}}. \tag*{(11)}

If B0B_0 has full column rank, then JτJ_\tau is injective for all sufficiently small positive τ\tau.

Proof. The basis construction gives ∣S∣|\mathcal{S}| columns for every τ\tau, and the row set is the fixed set I\mathcal{I}. The mixed-derivative convergence just established gives

(Bτ)(ℓ,b),(j,K)=∂xℓ∂ybHEj,K,τ(x,y)∣(0,0)⟶Kℓjb.(B_\tau)_{(\ell,b),(j,K)}=\left.\partial_x^\ell\partial_y^b H_{E_{j,K,\tau}}(x,y)\right|_{(0,0)} \longrightarrow K^\ell j^b.

Zeroth derivatives contribute the factor 11, also when K=0K=0 or j=0j=0. This is (11). If B0B_0 has full column rank, some minor of size ∣S∣|\mathcal{S}| has nonzero determinant. The corresponding determinant of BτB_\tau converges to it and is therefore nonzero for all sufficiently small positive τ\tau. Thus BτB_\tau has full column rank, and its linear map JτJ_\tau is injective.

The factors τ−x0K\tau^{-x_0K} may tend to zero or infinity, but for each τ>0\tau>0 they give invertible basis changes and preserve rank. Lemma 4.1 supplies a nonzero kernel separately for each fixed τ\tau; Proposition 4.3 compares numerical matrices in the explicit bases. Thus no continuous choice of kernel vectors, or algebraic family of plane embeddings across τ=0\tau=0, is required. To contradict Lemma 4.1, it remains to prove full column rank of the corresponding limiting matrix for a sufficiently large common multiple of (d,m)(d,m).

Interpolation on the exponent set

We prove that the limiting matrix (11) has full column rank when the common multiplicity is sufficiently large at a fixed ratio d/md/m. The final assembly will achieve that size by taking a common power. The matrix columns are indexed by the finite exponent set S\mathcal{S} of (10), and its rows are the restrictions to S\mathcal{S} of the monomials

KℓJb,0≤b<m,0≤ℓ<q(m−b).K^\ell J^b,\qquad0\leq b<m,\qquad0\leq\ell<q(m-b).

where evaluation at (j,K)(j,K) substitutes J=jJ=j. Thus full column rank means that their span interpolates every function on S\mathcal{S}. We first give a sufficient condition in terms of the distribution of horizontal row sizes. We then prove that condition by enclosing S\mathcal{S} in a polygon and counting its horizontal slices. All parameters remain fixed as in Section 3; in particular, q=r−9q=r-9 and h=mρ>0h=m\rho>0.

Interpolation by horizontal rows

The interpolation procedure treats larger rows first and multiplies each correction by factors vanishing on all previously treated rows. The number of earlier rows controls the degree in KK, while the current row size controls the degree in JJ. Their joint constraint explains why a bound on the largest row, or on the total number of points, would not suffice.

Lemma 5.1 (Interpolation by horizontal rows). Let q,mq,m be positive integers and S⊂C2S \subset\mathbb{C}^{2} a finite set, with coordinates (j,K)(j,K). For each represented height KK, let NKN_K be its row size. Suppose

NK≤m,#{K:NK≥t}≤q(m−t+1)(1≤t≤m, t∈Z).N_K \le m,\qquad\#\{K:N_K\ge t\}\le q(m-t+1)\qquad(1\le t\le m,\ t\in\mathbb{Z}).

Then every function S→CS\to\mathbb{C} is the restriction of a polynomial in

Pq,m=span⁡C{KℓJb:0≤b<m,0≤ℓ<q(m−b)}⊂C[J,K].\mathcal{P}_{q,m}=\operatorname{span}_{\mathbb{C}}\{K^{\ell}J^b:0\le b<m,\quad0\le\ell<q(m-b)\}\subset\mathbb{C}[J,K].

Here evaluation at (j,K)(j,K) substitutes J=jJ=j.

Proof. The empty set is immediate. Otherwise order the distinct heights as K1,…,KsK_1,\ldots,K_s so that their sizes N1,…,NsN_1,\ldots,N_s are nonincreasing. The first ii rows have size at least NiN_i, even when sizes are tied, and hence

i≤#{K:NK≥Ni}≤q(m−Ni+1).i\le\#\{K:N_K\ge N_i\}\le q(m-N_i+1).

Starting with the zero polynomial, match the prescribed values one row at a time. For row ii, put

Qi(K)=∏a=1i−1(K−Ka),Q_i(K)=\prod_{a=1}^{i-1}(K-K_a),

where the empty product is one. Since Qi(Ki)≠0Q_i(K_i)\ne0 and the NiN_i first coordinates on this row are distinct, univariate interpolation gives a polynomial pi(J)p_i(J) of degree at most Ni−1N_i-1 such that Qi(Ki)pi(j)Q_i(K_i)p_i(j) is the correction required at every point of row ii. Adding Qi(K)pi(J)Q_i(K)p_i(J) matches that row and preserves all previous rows.

Every monomial of this correction has b≤Ni−1<mb\le N_i-1<m and

ℓ≤i−1<q(m−Ni+1)≤q(m−b),\ell\le i-1<q(m-N_i+1)\le q(m-b),

by (5.1). Thus each correction belongs to Pq,m\mathcal{P}_{q,m}, and their sum interpolates the prescribed values. □

For the exponent set SS, it remains to prove the two row bounds in this lemma. We will obtain them by enclosing SS in a polygon and using its horizontal slice lengths to count the rows.

An enclosing polygon

Write a=ρ∗=3(r−3)>0a=\rho_* =3(\sqrt{r}-3)>0, and set

U0=h9(a−Δ)+ma,X=jm,Y=K−U0m.U_0=\frac{h}{9}(a-\Delta)+ma,\qquad X=\frac{j}{m},\qquad Y=\frac{K-U_0}{m}.

Thus U0U_0 is the lower endpoint of the exponent interval for j=0j=0. For 0<λ≤10<\lambda\le1, and with t+=max⁡{t,0}t_+=\max\{t,0\}, define

Dλ={(X,Y)∈R2:X≥0,−aX≤Y≤−aX+λa−9(X−λ)+}.(12)D_\lambda=\{(X,Y)\in\mathbb{R}^{2}:X\ge0,\quad-aX\le Y\le-aX+\lambda a-9(X-\lambda)_+\}. \tag*{(12)}

By (5), we have ρ+Δρ/9<a\rho+\Delta\rho/9<a. Choose 0<λ<10<\lambda<1 sufficiently close to 11 that

ρ+Δρ9<λa−9(1−λ).\rho+\frac{\Delta\rho}{9}<\lambda a-9(1-\lambda).

This choice depends only on rr, the ratio d/md/m, and Δ\Delta. We will show that this inequality places SS inside mDλ+(0,U0)mD_\lambda+(0,U_0). The horizontal widths of this scaled, translated polygon will be at most mλ<mm\lambda<m, and the heights supporting a slice of length at least ss will form an interval of length q(mλ−s)q(m\lambda-s) for [eq].

Lemma 5.2. Every pair (j,K)∈S(j,K) \in S satisfies

0≤X≤1+ρ/9,0 \le X \le1 + \rho/9,
−aX+Δ(X−1)+≤Y≤−aX+ρ+(Δ−9)(X−1)+.(13)-aX + \Delta(X-1)_{+} \le Y \le-aX + \rho+ (\Delta-9)(X-1)_{+}. \tag*{(13)}

The region in (13) is contained in Dλ\mathcal{D}_{\lambda}. Consequently, S⊆mDλ+(0,U0)S \subseteq m\mathcal{D}_{\lambda} + (0,U_{0}).

Proof. The index bound j≤⌊d/3⌋j \le\lfloor d/3 \rfloor gives X≤d/(3m)=1+ρ/9X \le d/(3m) = 1 + \rho/9. For j≤mj \le m, the exponent interval is

U0−aj<K<U0−aj+h,U_{0} - aj < K < U_{0} - aj + h,

which gives the first branches of the two bounds. For j>mj > m with d−3j>0d - 3j > 0, its length is n=h−9(j−m)n = h - 9(j-m) and its lower endpoint is n(a−Δ)/9n(a-\Delta)/9. The identities

n9(a−Δ)−U0=−aj+Δ(j−m),n=h−9(j−m)\frac{n}{9}(a-\Delta) - U_{0} = -aj + \Delta(j-m), \qquad n = h - 9(j-m)

give the second branches after division by mm.

If a degree-zero block occurs, its sole exponent is (j,K)=(d/3,0)(j,K) = (d/3,0), where j=m+h/9j = m + h/9. Hence

X=1+ρ/9,Y=−a−ρ9(a−Δ).X = 1 + \rho/9, \qquad Y = -a - \frac{\rho}{9}(a-\Delta).

Both bounds in (13) equal this value, so the endpoint is included.

For containment, the lower bound is at least −aX-aX. If X≤1X \le1, then (5.3) gives

λa−9(X−λ)+≥λa−9(1−λ)>ρ.\lambda a - 9(X-\lambda)_{+} \ge\lambda a - 9(1-\lambda) > \rho.

If 1≤X≤1+ρ/91 \le X \le1 + \rho/9, subtracting the common term −aX−9(X−1)-aX - 9(X-1) from the upper bounds reduces their comparison to

ρ+Δ(X−1)≤ρ+Δρ/9<λa−9(1−λ),\rho+ \Delta(X-1) \le\rho+ \Delta\rho/9 < \lambda a - 9(1-\lambda),

by (5.3). Thus the entire region, including its endpoint, lies in Dλ\mathcal{D}_{\lambda}.

Horizontal slices and integer rows

The length of a bounded interval is the difference of its endpoints; a singleton has length zero. When a required length is zero, we still require the slice to be nonempty.

Lemma 5.3 (Horizontal slice profile). We have Dλ=λD1\mathcal{D}_{\lambda} = \lambda\mathcal{D}_{1}. The nonempty horizontal slices of D1\mathcal{D}_{1} have lengths

w(Y)={1−Y/a,0≤Y≤a,1+Y/(a(1+a/9)),−a(1+a/9)≤Y≤0.w(Y) = \begin{cases} 1-Y/a, & 0 \le Y \le a, \\ 1+Y/\bigl(a(1+a/9)\bigr), & -a(1+a/9) \le Y \le0. \end{cases}

Their maximum length is one. For 0≤s≤mλ0 \le s \le m\lambda, the heights of nonempty slices of mDλ+(0,U0)m\mathcal{D}_{\lambda} + (0,U_{0}) of length at least ss form the closed interval

[U0−a(1+a/9)(mλ−s), U0+a(mλ−s)],[U_{0} - a(1+a/9)(m\lambda-s),\ U_{0} + a(m\lambda-s)],

whose length is q(mλ−s)q(m\lambda-s)*.

Proof. Scaling both coordinates by λ\lambda in (12) gives Dλ=λD1D_\lambda=\lambda D_1. The lower boundary of D1D_1 is Y=−aXY=-aX and its upper boundary is

Y={a(1−X),0≤X≤1,(a+9)(1−X),X≥1.Y=\begin{cases} a(1-X), & 0\le X\le1,\\ (a+9)(1-X), & X\ge1. \end{cases}

Thus its vertices are

(0,0),(0,a),(1,0),(1+a/9,−a(1+a/9)).(0,0),\quad(0,a),\quad(1,0),\quad(1+a/9,-a(1+a/9)).

The slices are

0≤X≤1−Y/a,0≤Y≤a,0\le X\le1-Y/a,\qquad0\le Y\le a,
−Y/a≤X≤1−Y/(a+9),−a(1+a/9)≤Y≤0,-Y/a\le X\le1-Y/(a+9),\qquad-a(1+a/9)\le Y\le0,

and are empty at all other heights. Their lengths are the stated functions, since 1+Y/a−Y/(a+9)=1+Y/(a(1+a/9))1+Y/a-Y/(a+9)=1+Y/(a(1+a/9)). Both attain their maximum one at Y=0Y=0.

Scale by mλm\lambda and translate vertically by U0U_0. Solving these two linear inequalities for length at least ss gives the claimed closed interval. Its length is

(2a+a2/9)(mλ−s)=q(mλ−s),(2a+a^2/9)(m\lambda-s)=q(m\lambda-s),

because a=3(r−3)a=3(\sqrt{r}-3) implies 2a+a2/9=r−9=q2a+a^2/9=r-9=q. At s=mλs=m\lambda the interval is the single height U0U_0; at s=0s=0 it is the full vertical range of the polygon.

For each integer KK, let

NK=#{j∈Z:(j,K)∈S}.N_K=\#\{j\in\mathbb{Z}:(j,K)\in S\}.

Only finitely many of these row sizes are nonzero. The slice profile in Figure 1 bounds both each row size and the number of rows of any given minimum size. The passage from lengths to integer counts adds at most one endpoint. We will absorb it with the size condition

Slice widths and their superlevel interval for $D_1$

Figure 1. Slice widths and their superlevel interval for D1D_1, drawn schematically with a=ρ∗a=\rho_\ast and 0<s<10<s<1. In panel (a), the marked slice at Y−=−a(1+a/9)(1−s)Y_-=-a(1+a/9)(1-s) has length ss. In panel (b), slices of length at least ss occur exactly at heights from Y−Y_- to Y+=a(1−s)Y_+=a(1-s), an interval of length q(1−s)q(1-s). Scaling by mλm\lambda and translating by (0,U0)(0,U_0) gives the polygon and height intervals used to bound the integer rows.

q(1−λ)m≥1.q(1-\lambda)m\ge1.

Lemma 5.4 (Integer row counts). If q(1−λ)m≥1q(1-\lambda)m \ge1, then the exponent set satisfies

NK≤m(K∈Z),N_K \le m \qquad(K \in\mathbb{Z}),
#{K∈Z:NK≥t}≤q(m−t+1)(1≤t≤m, t∈Z).(14)\#\{K \in\mathbb{Z}: N_K \ge t\} \le q(m-t+1) \qquad(1 \le t \le m,\ t \in\mathbb{Z}). \tag*{(14)}

Proof. By Lemmas 5.2 and 5.3, the integer positions in a represented row lie in an interval of length at most mλ<mm\lambda< m. Their span is at least NK−1N_K-1, so integrality gives NK≤mN_K \le m, also for a singleton row.

A row with NK≥tN_K \ge t requires a nonempty slice of length at least t−1t-1. If t−1>mλt-1 > m\lambda, there are no such rows. Otherwise their integer heights lie in a closed interval of length q(mλ−t+1)q(m\lambda-t+1). An interval of length L≥0L \ge0 contains at most ⌊L⌋+1≤L+1\lfloor L\rfloor+1 \le L+1 integers. Therefore

#{K∈Z:NK≥t}≤q(mλ−t+1)+1=q(m−t+1)−q(1−λ)m+1≤q(m−t+1)\#\{K \in\mathbb{Z}: N_K \ge t\} \le q(m\lambda-t+1)+1 = q(m-t+1)-q(1-\lambda)m+1 \le q(m-t+1)

by (5.5). The extra one accounts for integral endpoints, including when the height interval is a singleton.

Full rank and the strict inequality

Proposition 5.5. If q(1−λ)m≥1q(1-\lambda)m \ge1, then the limiting matrix B0B_0 of (4.5) has full column rank. Consequently, JτJ_\tau is injective for all sufficiently small positive τ\tau.

Proof. Apply Lemma 5.1 to S=SS=\mathcal S, using Lemma 5.4. The row vectors of B0B_0 are the restrictions to SS of the monomials spanning Pq,m\mathcal{P}_{q,m}. They therefore span CS\mathbb{C}^{S}, so B0B_0 has rank #S\#S. Proposition 4.3 then gives the injectivity of JτJ_\tau for sufficiently small τ\tau.

Completion of the proof of Theorem 1.1. By Lemma 2.1, it suffices to exclude every universal system Ur(d,m)\mathsf U_r(d,m) with d/m≤rd/m \le\sqrt{r}. Proposition 2.3 does so when rr is a square, including equality.

For nonsquare rr, the rational ratio d/md/m is strictly below r\sqrt{r}, and Lemma 2.4 forces d/m>3d/m > 3. Choose Δ\Delta as in (3.5) and λ\lambda as in (5.3). By Lemma 2.1, replace (d,m)(d,m) by a common positive integral multiple large enough to satisfy (5.5). The ratio d/md/m, and hence the choices of ρ\rho, Δ\Delta, and λ\lambda, do not change. Apply all the preceding constructions to this one chosen pair. Then Proposition 3.1 and Lemma 4.1 give a nonzero kernel of JτJ_\tau for every fixed τ∈(0,1)\tau\in(0,1). Proposition 5.5 gives an injective JτJ_\tau for all sufficiently small positive τ\tau, a contradiction. The collision has been taken on each fixed curve before the matrix limit; no simultaneous choice of kernel vectors is needed.

There are therefore no universal systems of the required slope. Lemma 2.1 supplies the single countable union ErE_r and the strict inequality outside it, simultaneously for every positive degree and every nonnegative integral multiplicity vector. That reduction concerns all nonzero homogeneous forms, so the conclusion includes reducible and nonreduced effective curves.

Fields and multipoint positivity

The analytic proof was carried out over C\mathbb{C}. Its conclusion extends by algebraic incidence conditions, without embedding another field into C\mathbb{C}. The implication from complex Nagata to the corresponding statement over uncountable algebraically closed characteristic-zero fields is also discussed by Bansal–Majumder [1]. We give the incidence argument with the simultaneous quantifiers needed here.

Corollary 6.1. Let kk be an uncountable algebraically closed field of characteristic zero, and let r≥10r \ge10. There is a countable union of proper Zariski-closed subsets of the space of distinct ordered rr-tuples in Pk2\mathbb{P}^{2}_{k}, with nonempty complement, outside which the conclusion of Theorem 1.1 holds with the same degree and multiplicity conventions.

Proof. Let Ad,mA_{d,\mathbf{m}} be the Q\mathbb{Q}-defined incidence locus constructed in the proof of Lemma 2.1: its points are the tuples admitting a nonzero degree-dd form with multiplicities at least m\mathbf{m}. On affine charts it is defined by the full-column-size minors of the Taylor-coefficient matrix. The same rational minors define its base change over any characteristic-zero field.

Whenever dr≤∑imid\sqrt{r} \le\sum_i m_i, Theorem 1.1 shows that this locus is proper over C\mathbb{C}. It is therefore proper over Q\mathbb{Q} and remains proper over kk: a nonzero defining minor on a rational affine chart stays nonzero after field extension. Exclude these loci for all the countably many violating pairs (d,m)(d,\mathbf{m}). Each tuple remaining satisfies every asserted inequality. The complement is nonempty: choose 2r2r affine coordinates in kk algebraically independent over Q\mathbb{Q}. They avoid all these proper rationally defined loci and all coincidences. Such coordinates exist by uncountability, since the algebraic closure in kk of a field generated over Q\mathbb{Q} by finitely many elements is countable. □

Let XX be the blowup of the plane at a tuple covered by Theorem 1.1 or Corollary 6.1. Write HH for the pullback of a line and E1,…,ErE_1,\ldots,E_r for the exceptional curves. A real divisor class is nef if its intersection with every irreducible curve is nonnegative, and strictly nef if every such intersection is positive. The multipoint Seshadri constant of the line bundle OP2(1)\mathcal{O}_{\mathbb{P}^{2}}(1) at the tuple is

ε(O(1);p1,…,pr)=sup⁡{t≥0:H−t∑iEi is nef}.\varepsilon(\mathcal{O}(1);p_1,\ldots,p_r)=\sup\{t\ge0:H-t\sum_i E_i\text{ is nef}\}.

Corollary 6.2. The class Nr=rH−∑iEiN_r=\sqrt{r}H-\sum_i E_i is strictly nef and satisfies Nr2=0N_r^2=0. In particular,

ε(O(1);p1,…,pr)=1r.\varepsilon(\mathcal{O}(1);p_1,\ldots,p_r)=\frac{1}{\sqrt{r}}.

Proof. Every irreducible curve on XX is either an exceptional curve or the strict transform of an irreducible plane curve. The first kind has intersection 11 with NrN_r. For the second kind, the intersection is dr−∑imult⁡piC>0d\sqrt{r}-\sum_i\operatorname{mult}_{p_i}C>0. Thus NrN_r is strictly nef. The intersection identities H2=1H^2=1, H⋅Ei=0H\cdot E_i=0, and Ei⋅Ej=−δijE_i\cdot E_j=-\delta_{ij} give Nr2=0N_r^2=0.

The class H−r−1/2∑iEiH-r^{-1/2}\sum_i E_i is nef, so the Seshadri constant is at least r−1/2r^{-1/2}. For the opposite bound, fix a positive integer nn and put en=⌈r(n+1)⌉e_n=\lceil\sqrt{r}(n+1)\rceil. There are at most r(n+12)r\binom{n+1}{2} linear conditions on degree-ene_n forms for multiplicity at least nn at all the points, whereas

(en+22)>r(n+12).\binom{e_n+2}{2}>r\binom{n+1}{2}.

Thus a nonzero such form exists. If H−t∑iEiH-t\sum_i E_i is nef with t≥0t\ge0, intersecting its class with the strict transform of this form’s divisor DD gives

0≤en−t∑imult⁡piD≤en−trn.0\le e_n-t\sum_i\operatorname{mult}_{p_i}D\le e_n-trn.

Hence t≤en/(rn)t\le e_n/(rn), which tends to 1/r1/\sqrt{r} as n→∞n\to\infty. This proves the upper bound using only the count of multiplicity conditions. □

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