Introduction

For a smooth projective variety XX, canonical nonvanishing asks whether pseudo-effectivity of KXK_X guarantees a pluricanonical form: a nonzero section of mKXmK_X for some integer m>0m > 0. Pseudo-effectivity says that the numerical class is a limit of effective divisor classes. The question concerns the canonical line bundle itself, rather than an approximation to its numerical class. Over C\mathbb{C}, pseudo-effectivity of KXK_X is equivalent to XX not being covered by rational curves [5], Corollary 0.3. Nonvanishing thus asks for a pluricanonical form on every smooth projective variety outside the uniruled class.

Nonvanishing is weaker than abundance. For a nef canonical divisor, abundance asks for semiampleness: some positive multiple is generated by its global sections and therefore defines a morphism. Obtaining the first section is a separate difficulty. We prove the following nonvanishing theorem in dimension four.

Theorem 1.1. Let XX be a smooth connected projective complex fourfold. If KXK_X is pseudo-effective, then H0(X,mKX)≠0H^0(X,mK_X) \ne0 for some positive integer mm.

The theorem imposes no condition on numerical dimension, irregularity, or holomorphic Euler characteristic. Its conclusion is qualitative; it gives no uniform bound on the integer mm.

The threefold results explain both the history of the problem and the lower-dimensional inputs used here. Miyaoka proved nonvanishing for minimal threefolds [34] and then abundance in numerical dimension one [35], pp. 203–204. Kawamata’s work on pluricanonical systems and his abundance theorem for minimal threefolds established the broader canonical case [22, 23]. Keel–Matsuki–McKernan proved log abundance for threefolds, with the correction included here [25, 26]. Boundary arguments also require sections to agree where components meet: Fujino’s semi-log-canonical threefold abundance theorem supplies generation on the whole reduced floor, including its conductor identifications [10], Corollary 4.10. These are established lower-dimensional theorems used before the new fourfold argument.

Several important fourfold cases were already known. Fujino proved semiampleness for canonical fourfolds with nef canonical divisor and positive irregularity. He distinguished nonvanishing for non-uniruled fourfolds of irregularity zero from the remaining abundance question in Kodaira dimension zero [11], Corollary 4.7 and Problems 4.10–4.11. Lazić–Peternell proved nonvanishing for Q\mathbb{Q}-factorial terminal projective minimal varieties with canonical numerical dimension one and nonzero holomorphic Euler characteristic [30], Theorem 6.7. Ambro’s canonical bundle formula gives a complementary reduction: the lower-dimensional minimal model program and abundance settle a nef klt adjoint whose nef reduction has lower-dimensional image [1], Theorem 4.3. The nef reduction contracts the curves of degree zero through very general points; the dimension of its image is the nef dimension. This curve-theoretic dimension is distinct from numerical dimension, which is defined by nonzero intersection powers of the nef divisor.

The smooth theorem also has a log canonical consequence. Hashizume proved that smooth canonical nonvanishing in dimension nn implies nonvanishing for log canonical pairs with real boundaries, as well as log minimal models, in dimensions at most nn [20], Theorem 1.4. For rational data we replace the resulting effective real representative by a rational one, preserving its support and working on the original variety.

Corollary 1.2. Let (X,Δ)(X,\Delta) be a connected normal projective log canonical complex pair of dimension at most four. Suppose that Δ≥0\Delta\ge0 is rational and D=KX+ΔD = K_X + \Delta is Q\mathbb{Q}-Cartier and nef. For every positive integer rr such that rDrD is Cartier, there is a positive integer mm with H0(X,OX(mrD))≠0H^0(X,\mathcal{O}_X(mrD)) \ne0.

The corollary does not require XX to be Q\mathbb{Q}-factorial, and mm may depend on the pair and the prescribed index. Log abundance asks for semiample-ness of the nef adjoint KX+ΔK_X+\Delta. The passage from the first section to that conclusion uses the supported-boundary lifting and abundance-after-nonvanishing theorems in the separate companion Lifting sections from the reduced support of an adjoint [39], Theorems 1.1–1.2. Together with the corollary, they give fourfold log abundance; that consequence does not enter the proof below.

A recent comparison is Liu–Xu’s preprint on good minimal models for log canonical pairs of dimension at most five with nonnegative invariant Iitaka dimension and numerical dimension at most one [31], Theorem 5.1. Its hypotheses already include nonvanishing and restrict numerical dimension. The present smooth theorem obtains the first section without either restriction.

Geometry of a possible counterexample

Suppose nonvanishing fails. Existence of minimal models in dimension four allows us to fix a terminal minimal model YY, retaining the pluricanonical section spaces. The termination input used here is the ordinary-pair case of Chen–Tsakanikas [7], Theorem 1.1; it supplies a minimal model, without asserting semiample-ness. Write K=KYK=K_Y. The divisor KK is nef and not big. The preceding reductions give q(Y)=h1(Y,OY)=0q(Y)=h^1(Y,\mathcal{O}_Y)=0 and full nef dimension.

On a fixed very general locus, every curve has positive KK-degree and every proper positive-dimensional subvariety is of general type. A fixed Cartier index makes the positive curve degrees uniformly bounded away from zero.

Choose ample polarizations approaching the nef ray of KK, scaled so that their volumes remain small while their degrees on curves through that locus tend to infinity. A section with unusually high vanishing at a moving point would force a persistent component in the base locus of the corresponding jet systems. Differentiation with respect to the moving point controls the multiplicity along that component. This uses the parameter-differentiation method of Ein–Küchle–Lazarsfeld [9], Proposition 2.3. We apply it to the whole space of sections satisfying the jet conditions, so the estimate controls ordinary powers of the ideal of the component. Intersection theory bounds its degree and canonical intersection. General type then produces a curve of bounded degree, contradicting the chosen scaling. The resulting upper bound applies to every section in every allowed Cartier degree. The independent moving-center estimates and the finite-cover lemma used in this argument and its two-factor extension are [38], Lemmas 7.1–7.5. We apply them to the fourfold geometry and prove the required curve and correspondence obstructions here.

A second use of this argument concerns sections over two copies of YY. Fix an integer ℓ>0\ell>0 making S0=ℓKS_0=\ell K Cartier and consider

Z=P(OY×Y(S0,1)⊕OY×Y(S0,2))⟶Y×Y.Z=\mathbb{P}\left(\mathcal{O}_{Y\times Y}(S_{0,1})\oplus\mathcal{O}_{Y\times Y}(S_{0,2})\right)\longrightarrow Y\times Y.

A subscript indicates pullback from the corresponding factor. The two summands give two distinguished sections of this projective bundle. The symmetric-power formula records the distributions of a fixed tensor exponent between the two factors: its summands are O(aS0,1+bS0,2)\mathcal{O}(aS_{0,1}+bS_{0,2}), for nonnegative integers a,ba,b with a+ba+b fixed. A polarization on ZZ combines the two base polarizations and a multiple of its tautological bundle. We show that it generates many jets at a very general point away from the two distinguished sections. Its Seshadri constant, the infimum of degree divided by multiplicity over curves through the point, measures this local positivity.

Moving base components in ZZ have several possible images and fibers. One case requires an additional argument. Restrict to a slice where one base coordinate is fixed. A multisection different from the two distinguished sections meets them in divisors whose difference represents a multiple of KK. This is a signed representative: its coefficients may be positive or negative. We must prove that the logarithmic adjoint on a resolution of its full support is big. This is where minimal metrics and ordinary cohomological injectivity enter the geometry.

The companion Minimal metrics and interior injectivity for nef adjoints [37] supplies two analytic inputs. Every minimal semipositive metric on the pullback of a nef projective klt adjoint has zero Lelong numbers. In addition, an injectivity theorem on ordinary H1H^1 compares an interior rational boundary with an endpoint boundary when the two endpoint bundles carry such metrics. The exact hypotheses are recorded in Section 4. These statements concern actual rational line bundles; numerical equivalence would not suffice.

The cohomological method draws on the harmonic-form approach of Enoki, as extended by Fujino to singular metrics, and on Matsumura’s treatment of metrics with transcendental singularities [15], Theorem 1.2, Lemmas 3.1–3.2, and Section 3, Claim 1 [32], Theorems 1.3 and 5.9, Sections 5.2–5.3. Fujino’s complete metrics on an analytic complement and his comparison with coherent cohomology with multiplier ideals give a model for the setup. Matsumura supplies uniform estimates for primitives of exact forms.

Applied to two nearby nef klt adjoints, the cohomological injection makes restriction to a whole reduced non-klt boundary surjective. Lower-dimensional abundance and gluing across the conductor supply a section on that boundary. Once this section has been lifted, Gongyo–Matsumura’s fourfold criterion converts nonvanishing and the zero-Lelong metric into semiampleness [17], Corollary 5.3. This order matters: the criterion is applied after the first section has been obtained. The signed-representative argument then excludes the offending multisection. The remaining analysis also excludes dominant finite correspondences, using a fixed branch complement and the positive canonical degree of curves.

From jets to a rank contradiction

We now have opposing estimates. Sections on one copy of YY can vanish only to a small order, while the projective bundle over Y×YY \times Y has enough jets to give a large evaluation rank. We fix the polarization, a smooth resolution and a flag of general hyperplane sections ending in a curve, together with one finite system of jets. The scalar estimate also supplies a fixed movable curve on the blowup of a point. Its intersection with effective divisors will bound orders of sections after reduction. We spread all these finite data and reduce modulo sufficiently large primes.

Ordinary jets produce an evaluation matrix whose generic rank is large. On the diagonal, the canonical Frobenius filtration expresses its possible values through truncated powers of the cotangent bundle. A single flag estimate bounds the sum of the dimensions of these spaces, forcing a much smaller rank there. A nonzero maximal determinant must therefore vanish to high order at a suitable diagonal point. Its two actual determinant line bundles, one from each factor, have classes controlled by the fixed movable curve. This bounds the order of every section of either factor on the reduction itself. The resulting small determinant order is incompatible with the order forced by the rank drop.

The filtration has a substantial history. For curves, the diagonal filtration appears in Raynaud’s work [40, Remarques 4.1.2(2)]; Joshi–Ramanam–Xia–Yu formulate it using the Cartier connection [21, Section 5.3]. Sun and Kitadai–Sumihiro give the higher-dimensional filtration and its local description by truncated monomials [41, Theorem 3.7] [27, Corollary 3.5]. Mustaţă–Schwede’s comparison of ordinary and Frobenius powers provides the local jet conversion [36, proof of Proposition 2.12, Equation eq:2.8], and Langer’s estimate controls the Frobenius instability error [28, Corollary 2.5]. The argument combines these tools with the two-factor geometry and the common flag estimate. Section 7 specifies the numerical separation between the resulting ranks and orders and verifies the inputs of the common theorem.

The complete finite-data Frobenius comparison is proved independently in [38]. It is also applicable to the all-dimensional abundance argument. Its hypotheses are the stated geometric data and numerical inequalities. No all-dimensional abundance conclusion or logarithmic Iitaka subadditivity is used in the fourfold preparation of these data.

Reading order. Section 2 fixes the terminal model and its curve-degree obstruction. Section 3 develops the moving-center tools and proves the scalar order bound. Section 4 states the analytic inputs, and Section 5 proves logarithmic general type for signed supports. Section 6 excludes the product’s moving centers and obtains the two-slot jets. Section 7 verifies the finite data for the common Frobenius theorem, completing smooth nonvanishing. Section 8 gives the original-variety and prescribed-index consequence.

Conventions. Varieties are over C\mathbb{C} except when the finite-data comparison is reduced to positive characteristic. A subvariety is of general type when a smooth projective resolution is of general type. Rational line bundles and their sections are interpreted after clearing specified denominators. An inequality in nef order means that its difference is nef. A very general locus is the complement of a countable union of proper closed subsets. The symbols rr for a prescribed Cartier index, rtr_t for a scaling integer, q(Y)q(Y) for irregularity, and qq for a projective-bundle weight have distinct uses.

A fixed minimal model of full nef dimension

Assume that smooth canonical nonvanishing fails in dimension four. We first choose a terminal minimal model on which every curve through a very general point has a fixed positive lower bound for its canonical degree. We then show that every proper positive-dimensional subvariety through such a point is of general type. These two properties will control the moving centers of the later jet argument. The model remains fixed while its ample perturbations vary.

Proposition 2.1. If Theorem 1.1 fails, there is a projective Q\mathbb{Q}-factorial terminal fourfold YY, with K=KYK=K_Y, such that

(i) KK is nef, κ(Y,K)=−∞\kappa(Y,K)=-\infty, and K4=0K^4=0;

(ii) q(Y)=0q(Y)=0 and the nef dimension of KK is four;

(iii) for some integer ι>0\iota>0, ιK\iota K is Cartier and

K⋅C≥1ι(1)K\cdot C\geq\frac{1}{\iota} \tag*{(1)}

for every integral curve CC through a point of a fixed very general locus in YY.

Proof. Start with a smooth counterexample HH. Run the canonical minimal model program. Existence of the necessary flips follows from [3]. Termination in the pseudo-effective fourfold case is [7], applied with zero nef data to the ordinary pair with zero boundary. Divisorial contractions lower the Picard number, so together these statements give termination of the program. Pseudo-effectivity is preserved and excludes a Mori fiber space as its endpoint. We obtain a projective Q\mathbb{Q}-factorial terminal minimal model YY. Canonical section spaces in sufficiently divisible degrees are birationally invariant here. On a common resolution the differences from the respective pulled-back canonical divisors are effective exceptional divisors, and pushing their sheaves forward does not add sections. Thus κ(Y,K)=−∞\kappa(Y,K)=-\infty. In particular KK is not big; as it is nef, this says K4=0K^4=0.

Terminal singularities are rational. Hence q(Y)q(Y) agrees with the irregularity of a resolution. If it were positive, [11] would make KK semiample, a contradiction. Likewise, if the nef dimension were at most three, [1], with the established log minimal model program and log abundance in those dimensions, would make KK semiample. This includes nef dimension zero. Thus the nef dimension is four.

The curve property of nef reduction [2] says in this case that K⋅C>0K \mathbin{\cdot} C>0 for every integral curve through a very general point. Choose ι\iota with ιK\iota K Cartier. Its degree on an integral complete curve is an integer, so positivity gives (1). This uses only the curve property of nef reduction, not an Iitaka fibration on YY.

Proposition 2.2. For YY as in Proposition 2.1, every proper positive-dimensional subvariety through a point of a suitable fixed very general locus is of general type.

Proof. We first work with one family of subvarieties, and at the end make the very general locus independent of the family. Hilbert schemes give countably many finite-type parameter spaces for integral subvarieties of YY. Stratification, resolution of the universal families, and generic smoothness give countably many smooth families

b:V⟶B,e:V⟶Y,b:\mathcal{V}\longrightarrow B,\qquad e:\mathcal{V}\longrightarrow Y,

whose fibers are smooth projective resolutions of their images and whose fiber maps are birational onto those images. To obtain this description, resolve the total universal family on an integral parameter stratum, shrink until its fibers are smooth and the fiber maps birational, and repeat on the complement by noetherian induction. Non-dominant evaluation families can be discarded by excluding their image closures in YY.

Consider a dominant family with fibers of dimension dd, where 0<d<40<d<4. We may slice the parameter space to dimension 4−d4-d so that ee becomes generically finite and remains dominant. Indeed, the parameters incident to a general point of YY have a component of dimension dim⁡B−(4−d)\dim B-(4-d) on the locus where the fiber maps are generically embeddings. General ample cuts in a compactification of BB meet this locus in finitely many points. We take the cuts very generally, so a very general point of the slice has the generic value of every plurigenus of the original family. There are only countably many such conditions.

On the resulting smooth total space, ramification and terminality give

KV∼Qe∗K+EV,EV≥0.K_{\mathcal{V}}\sim_{\mathbb{Q}} e^*K+E_{\mathcal{V}},\qquad E_{\mathcal{V}}\geq0.

For completeness, the rational lift of ee to a resolution of YY is defined at codimension-one points by properness. The usual ramification formula there, followed by the effective discrepancies of the terminal target, proves this divisor inequality. Its restriction to a very general fiber is

KV∼QeV∗K+EV,EV≥0.(2)K_V\sim_{\mathbb{Q}} e_V^*K+E_V,\qquad E_V\geq0. \tag*{(2)}

In particular KVK_V is pseudo-effective.

The dimension of VV is at most three. The minimal model program and abundance in these dimensions give a good terminal minimal model Vmin⁡V_{\min}. Suppose that VV is not of general type. The semiample canonical divisor of Vmin⁡V_{\min} defines a morphism with connected positive-dimensional general fibers, on each of which a multiple of KVmin⁡K_{V_{\min}} is trivial. On a common resolution V^\widehat{V} of VV and Vmin⁡V_{\min}, there is a complete curve through a very general point with KV~K_{\widetilde{V}}-degree zero. Here is the avoidance needed for this assertion. The singular locus of the terminal model and the centers of the exceptional divisors have codimension at least two. A general fiber either misses a given vertical center or meets a dominant center in codimension at least two. General sufficiently ample complete intersections in that fiber through a prescribed very general point give a curve avoiding all such centers; for a one-dimensional fiber the fiber itself does so. Its strict transform has canonical degree zero by the exceptional discrepancy formula.

Pulling back (2) to V~\widetilde{V} and adding the effective discrepancies of V~→V\widetilde{V} \to V gives

KV~∼Qe~∗K+E~,E~≥0.K_{\widetilde{V}} \sim_{\mathbb{Q}} \widetilde{e}^{*}K+\widetilde{E}, \qquad\widetilde{E}\geq0.

Choose the preceding curve through a point outside Supp⁡E~\operatorname{Supp}\widetilde{E} and outside the exceptional locus of the birational map onto the image subvariety. It is not contained in E~\widetilde{E}, and its image in YY is a curve. Thus its pulled-back KK-degree is at most zero. Dominance of the total evaluation lets us choose the point in the very general locus of (1), which gives a contradiction.

We have proved that the very general fiber of the sliced family is of general type. By the choice of slice its plurigenera are the generic plurigenera of the original smooth family. Upper semicontinuity shows that all fibers of that family have at least these plurigenera, hence are of general type as well. Finally exclude the image closures of all non-dominant families. Countability of the parameter strata gives the asserted very general locus.

For the rest of the contradiction argument, fix YY, KK, ι\iota, and a very general locus on which both propositions apply. We next choose ample perturbations of KK with bounded volume and growing degree on every curve through this locus. The two propositions will then turn a section of excessive vanishing order into a contradiction.

Moving centers and scalar vanishing

We work on the terminal fourfold YY from Section 2, write K=KYK=K_Y, and put n=4n=4. Write YvgY^{\mathrm{vg}} for a fixed very general locus on which both Propositions 2.1 and 2.2 apply. Thus every curve through this locus has KK-degree at least 1/ι1/\iota, and every proper positive-dimensional subvariety through it is of general type. We will bound the order of every section of every Cartier multiple of a suitable ample rational divisor at a very general point. Fix a very ample Cartier divisor AA on YY. For a fixed positive rational ϵ\epsilon and positive rational tt tending to zero, define

μt=((K+tA)n)1/n,rt∈Z>0,rtμt⟶ϵ,L=Lt=rt(K+tA).(3)\mu_t=((K+tA)^n)^{1/n}, \qquad r_t\in\mathbb{Z}_{>0}, \quad r_t\mu_t\longrightarrow\epsilon, \qquad L=L_t=r_t(K+tA). \tag*{(3)}

Such integers rtr_t exist, for example by rounding ϵ/μt\epsilon/\mu_t. Since KK is nef and not big, μt>0\mu_t>0 tends to zero. Hence

rt⟶∞,Ltn⟶ϵn,Lt⋅C≥rt/ιr_t\longrightarrow\infty, \qquad L_t^n\longrightarrow\epsilon^n, \qquad L_t\cdot C\geq r_t/\iota

for every integral curve CC through that very general locus. The integers rtr_t are unrelated to the original Cartier index rr in Corollary 1.2.

A section with excessive vanishing will yield a curve through YvgY^{\mathrm{vg}} whose LtL_t-degree is bounded independently of tt, contradicting (3.2). To construct that curve, we follow the base loci of the full jet kernels as their marked point moves. A component that persists at two successive jet levels has high multiplicity; this bounds both its degree and its canonical intersection. General type then produces a curve of bounded degree. We first give the three moving-center estimates from [38], Lemmas 7.1–7.4, including the differentiation argument responsible for ordinary ideal powers. These inputs are independent of abundance and subadditivity. We then prove the curve obstruction and apply it to scalar vanishing.

Numerical subadjunction at a generic lc center

The numerical statement below only requires log canonicity near the generic point of the center. This is the form needed for boundaries obtained from a linear system.

The subadjunction method relates an lc center to the canonical bundle formula. Kawamata’s minimal-center theorem and the later unperturbed form of Fujino–Gongyo are important antecedents [24, 16]. The numerical form below permits a center that is only generically lc and need not be minimal. Its proof in the companion uses a dlt stratum, the generic rank-one condition, b-nef moduli, and finite-base ramification; it is not an application of those antecedents with their hypotheses omitted.

Lemma 3.1 (Numerical generic subadjunction). Let ZZ be a projective Q\mathbb{Q}-factorial klt variety over C\mathbb{C}, let Θ≥0\Theta\ge0 be a rational divisor, and let V⊂ZV \subset Z be an integral positive-dimensional subvariety. Suppose that (Z,Θ)(Z,\Theta) is lc at the generic point of VV and that a divisor of log discrepancy zero has center VV. Let f=dim⁡Vf = \dim V, let PP be a nef rational Cartier divisor on ZZ, and let ρ:V∗→V\rho: V^* \to V be a smooth projective resolution, factoring through the normalization. Then

KV∗⋅(ρ∗P)f−1≤(KZ+Θ)∣V⋅(P∣V)f−1.(4)K_{V^*} \cdot(\rho^*P)^{f-1} \le(K_Z+\Theta)|_V \cdot(P|_V)^{f-1}. \tag*{(4)}

The right side is the intersection of the restricted rational Cartier class with the cycle [V][V]. No Q\mathbb{Q}-Gorenstein hypothesis on the normalization of VV is required.

The proof is given in the independent moving-center part of [38], Lemma 7.1.

Degree and canonical bounds for a base component

The following companion lemma applies numerical subadjunction to a boundary built from an actual linear system. Its local multiplicity controls both the degree of the center and the coefficient of that boundary.

Lemma 3.2 (A base component of high multiplicity). Let ZZ be a projective Q\mathbb{Q}-factorial klt variety of dimension dd, let PP be an ample rational Cartier divisor, and let k>0k > 0 be an integer for which kPkP is Cartier. Let 0≠H⊂H0(Z,OZ(kP))0 \ne\mathcal{H} \subset H^0(Z,\mathcal{O}_Z(kP)) be a linear subspace with proper base locus and base ideal b\mathfrak{b}. Suppose that VV is an integral base-locus component of dimension f<df < d, isolated at its generic point ηV\eta_V, and that ηV∈Zsm\eta_V \in Z_{\mathrm{sm}}. Write a=d−fa = d-f and m=mOZ,ηV\mathfrak{m} = \mathfrak{m}_{\mathcal{O}_{Z,\eta_V}}. If

bOZ,ηV⊂mh(h∈Z>0),\mathfrak{b}\mathcal{O}_{Z,\eta_V} \subset\mathfrak{m}^h \qquad(h \in\mathbb{Z}_{>0}),

then

Pf⋅V≤(k/h)aPd.(5)P^f \cdot V \le(k/h)^a P^d. \tag*{(5)}

If f>0f > 0, there is a rational number cc with 0<c≤ak/h0 < c \le ak/h such that, on a smooth resolution V∗V^*,

KV∗⋅Pf−1≤(KZ+cP)∣V⋅Pf−1.(6)K_{V^*} \cdot P^{f-1} \le(K_Z+cP)|_V \cdot P^{f-1}. \tag*{(6)}

The coefficient cc may be chosen with an effective rational divisor Θ∼QcP\Theta\sim_{\mathbb{Q}} cP such that (Z,Θ)(Z,\Theta) is lc at the generic point of VV and has an lc place with center VV. Thus Lemma 3.1 can also be applied with a different nef testing class. The degree estimate includes f=0f=0; the canonical estimate is asserted only for positive-dimensional VV.

The proof is given in the independent moving-center part of [38], Lemma 7.2.

Differentiating the full moving jet kernel

We use the parameter-differentiation method developed in [9]. The form used here retains ordinary ideal powers and isolated base components. Fixing a high order at a varying point produces a family of linear subspaces of one fixed section space. A component common to two successive base loci acquires high multiplicity, because parameter derivatives of the higher kernel still belong to the lower kernel. We state both the parameter-family conclusion and the local slicing property that will be used later.

Lemma 3.3 (Moving multiplicity). Let ZZ be an integral projective variety of dimension dd, and let PP be an ample rational Cartier divisor. Fix an integer kk with kPkP Cartier and positive real numbers

τ0<τ1<⋯<τd,τi+1−τi=δ>0.\tau_0 < \tau_1 < \cdots< \tau_d, \qquad\tau_{i+1} - \tau_i = \delta> 0.

For a smooth point xx, let Hi(x)\mathcal{H}_i(x) be the entire subspace of sections of kPkP vanishing at xx to order at least ⌈kτi⌉\lceil k\tau_i\rceil. Suppose that for very general xx all these subspaces are nonzero and the base locus of H0(x)\mathcal{H}_0(x) has a positive-dimensional component through xx. If kδ≥4k\delta\ge4, then, after an algebraic parameter extension and restriction to nonempty opens, there are an irreducible parameter space TT, a fixed adjacent pair of levels, and a family of integral subvarieties VtV_t common to the two base loci such that the incidence

Γ={(t,z):z∈Vt}⊂T×Z\Gamma= \{(t,z) : z \in V_t\} \subset T \times Z

dominates ZZ. Each general VtV_t has dimension in [1,d−1][1,d-1], is an isolated component of the higher base locus at its generic point, and its entire higher-series base ideal is contained there in

IVth,h=⌈kδ/2⌉,k/h≤2/δ.(7)\mathcal{I}_{V_t}^{h}, \qquad h = \lceil k\delta/2\rceil, \qquad k/h \le2/\delta. \tag*{(7)}

These are ordinary local ideal powers in the smooth ambient open.

More precisely, the incidence base ideal lies in IΓh\mathcal{I}_{\Gamma}^{h} on a dense open of Γ\Gamma. If a further morphism Z→BZ \to B is given, one may choose a general incidence point where the base support is only VtV_t and VtV_t is smooth over the smooth open of its image in BB. For the fiber component FF through that point, assume that FF is proper in the integral ambient fiber component under consideration. The restricted series is then nonzero and has base ideal in the ordinary IFh\mathcal{I}_{F}^{h} and has FF as an isolated base component there. This last assertion concerns the scheme fiber locally at that chosen point, and does not assert transversality of every fiber. Smoothness near the generic point of FF, and the projectivity and klt hypotheses needed for Lemma 3.2 on the ambient fiber, must be checked in each application.

Proof. We recall the argument of [38] to explain why the estimate concerns the entire kernel and ordinary ideal powers. On the open where the jet maps have constant rank, their kernels are vector bundles with fibers Hi(x)\mathcal{H}_i(x). Their base loci increase with ii. Starting with a positive-dimensional component through the mark, follow a containing component at each level. The d+1d+1 components all have dimensions in [1,d−1][1,d-1], so two successive ones coincide. After a finite parameter extension and shrinking, their geometric generic components and inclusions spread to one family Γ⊂T×Z\Gamma\subset T \times Z. Its evaluation dominates ZZ, since each member contains its moving mark x(t)x(t).

Take a local frame of the higher kernel and trivialize kPkP near zz with a frame independent of tt. In a fixed basis of the global section space, each frame section has the form

s(t,z)=∑αcα(t)sα(z).s(t,z) = \sum_{\alpha} c_{\alpha}(t)s_{\alpha}(z).

Differentiation in the parameter with zz fixed therefore gives another global section of kPkP. A derivative of order rr lowers the vanishing order at x(t)x(t) by at most rr. It belongs to the entire lower kernel whenever

r≤⌈kτi+1⌉−⌈kτi⌉.r \le\lceil k\tau_{i+1}\rceil- \lceil k\tau_i\rceil.

The right side is at least kδ−1k\delta- 1, so every derivative of order less than h=⌈kδ/2⌉h = \lceil k\delta/2\rceil belongs to that kernel and vanishes on Γ\Gamma. This is where using the full kernels matters: an arbitrarily chosen subseries need not contain these derivatives.

To turn these vanishings into ordinary ideal membership, work at a general smooth incidence point. Since Γ→Z\Gamma\to Z is submersive, parameter directions span its normal space in T×ZT \times Z. Choose parameter coordinates t=(t′,t′′)\mathbf{t} = (t^\prime,t^{\prime\prime}) so that the implicit function theorem writes Γ\Gamma as t′=F(t′′,z)t^\prime= F(t^{\prime\prime},z). With t′′t^{\prime\prime} and zz fixed, derivatives in t′t^\prime are exactly derivatives in the normal coordinates u=t′−F(t′′,z)u = t^\prime- F(t^{\prime\prime},z). All normal Taylor coefficients of degree below hh therefore vanish, proving s∈IΓhs \in\mathcal{I}_{\Gamma}^{h}. Faithful flatness of analytic local rings over algebraic local rings gives the same membership algebraically. There are finitely many frame sections, so this containment holds for the entire incidence base ideal on a dense algebraic open.

Generic smoothness of Γ→T\Gamma\to T identifies its scheme fiber there with the reduced member VtV_t. Restriction gives IΓO{t}×Z=IVt\mathcal{I}_{\Gamma}\mathcal{O}_{\{t\}\times Z} = \mathcal{I}_{V_t}, and the frame specializes to a basis of the entire higher kernel. Isolation holds because VtV_t is a base-locus component. Finally remove all other base components and choose the incidence point where VtV_t is smooth over its actual image in BB. Its scheme fiber is then reduced locally, so restriction to the ambient fiber sends IVth\mathcal{I}_{V_t}^{h} to IFh\mathcal{I}_{F}^{h} and the base support to FF. If FF is proper in the chosen integral ambient fiber component, that support is proper there; hence the restricted series is nonzero and has FF as an isolated base component at its generic point.

For a fixed gap δ\delta, combining Lemmas 3.2 and 3.3 gives degree and canonical-intersection bounds for a repeated moving component, with coefficients independent of the large divisible integer kk. The next lemma converts such intersection bounds into a curve of bounded degree. Its general-type hypothesis supplies a birational linear system in a degree depending only on the dimension. The scalar application uses Proposition 2.2 and has no boundary. We include a reduced boundary in the statement because the two-slot argument will also need its logarithmic form.

A uniform obstruction from logarithmic general type

Lemma 3.4 (Bounded-degree curve obstruction). Keep YY, LtL_t, and ll as in (3) and (3.2). Fix f≥1f \ge1 and positive constants C0,C1C_0,C_1. Suppose, for arbitrarily small tt, that there are a smooth projective variety Vt∗V_t^* of dimension ff, a reduced simple normal crossings divisor GtG_t on it, a nef rational divisor PtP_t, and a morphism et:Vt∗→Ye_t: V_t^* \to Y satisfying the following conditions:

(i) KVt∗+GtK_{V_t^*} + G_t is big;

(ii) 0<Ptf≤C00 < P_t^f \le C_0 and (KVt∗+Gt)⋅Ptf−1≤C1Ptf(K_{V_t^*} + G_t) \cdot P_t^{f-1} \le C_1P_t^f;

(iii) ete_t is generically finite onto its positive-dimensional image, and that image meets the fixed very general locus of YY;

(iv) Pt−et∗LtP_t - e_t^*L_t is nef.

Then these conditions are impossible for all sufficiently small tt. The case Gt=0G_t = 0 includes ordinary general type. Proof. Uniform effective birationality for projective lc pairs of dimension ff with big adjoint and coefficients in the fixed DCC set {0,1}\{0,1\} supplies an integer b=b(f)b=b(f) such that ∣b(KVt∗+Gt)∣|b(K_{V_t^*}+G_t)| is birational [18]. Resolve its base ideal and denote the free moving divisor by HbH_b. We keep the same notation for the pullbacks of PtP_t and LtL_t. The fixed divisor is effective, so

Hb⋅Ptf−1≤b(KVt∗+Gt)⋅Ptf−1≤bC1Ptf.H_b \cdot P_t^{f-1} \le b(K_{V_t^*}+G_t)\cdot P_t^{f-1} \le bC_1P_t^f.

Both HbH_b and PtP_t are nef and big; PtP_t is big because Ptf>0P_t^f>0. The Khovanskii–Teissier log-concavity inequalities for their mixed intersections give, when f>1f>1,

Pt⋅Hbf−1≤(Ptf−1⋅Hb)f−1(Ptf)f−2≤(bC1)f−1Ptf≤(bC1)f−1C0.(8)P_t\cdot H_b^{f-1}\le\frac{(P_t^{f-1}\cdot H_b)^{f-1}}{(P_t^f)^{f-2}}\le(bC_1)^{f-1}P_t^f\le(bC_1)^{f-1}C_0. \tag*{(8)}

Indeed the successive ratios of the positive numbers Ptf−i⋅HbiP_t^{f-i}\cdot H_b^i decrease, which gives the first inequality.

Choose a point where the birational morphism defined by HbH_b is an isomorphism onto an open of its image, where ete_t is quasi-finite, and whose image lies in the very general locus of YY. These conditions are compatible. To spell out the last one, write the excluded subset of YY as a countable union of proper closed subsets. The image of ete_t is not contained in any of them because it meets their complement. Their inverse images are therefore proper closed subsets of Vt∗V_t^*. They can be avoided together with the finitely many dense-open conditions. For a sweeping family one first chooses a very general member not contained in any excluded subset, and then such a point on that member.

For f>1f>1, cut by f−1f-1 general members of ∣Hb∣|H_b| passing through the chosen point. These give a proper effective curve cycle: on the birational image they are general hyperplanes through a point of the isomorphism open, and their pullbacks have no positive-dimensional base component. A component CC through the selected point maps nonconstantly to YY, since ete_t is quasi-finite there. Nefness and Equation (8) give

Lt⋅et(C)≤et∗Lt⋅C≤Pt⋅C≤Pt⋅Hbf−1≤(bC1)f−1C0.L_t\cdot e_t(C)\le e_t^*L_t\cdot C\le P_t\cdot C\le P_t\cdot H_b^{f-1}\le(bC_1)^{f-1}C_0.

In the first inequality the positive degree of the finite map of the normalization of CC onto its image has merely been discarded. If f=1f=1, use Vt∗V_t^* itself as CC; the same argument gives Lt⋅et(C)≤Pt⋅C≤C0L_t\cdot e_t(C)\le P_t\cdot C\le C_0.

The image is an integral curve through the very general locus, so (3.2) bounds its degree below by rt/ιr_t/\iota. This tends to infinity, whereas the upper bound depends only on f,C0,C1f,C_0,C_1. The contradiction proves the lemma. If several dimensions 1≤f≤n1\le f\le n occur, take the maximum of the finitely many resulting constants.

The scalar order bound

Define

Ps=2rt(K+2tA),ρt=(Psn)1/n.(9)P_s=2r_t(K+2tA),\qquad\rho_t=(P_s^n)^{1/n}. \tag*{(9)}

The inequalities

2L≤Ps≤4L2L\le P_s\le4L

are inequalities in nef order. After decreasing tt, they imply

ϵ≤ρt≤8ϵ.\epsilon\le\rho_t\le8\epsilon.

Only the existence of a positive lower bound and the displayed upper bound will be used.

Proposition 3.5 (Scalar orders). For all sufficiently small positive rational tt, a very general point x∈Ysmx \in Y_{\mathrm{sm}} has the following property. For every positive integer kk for which kPskP_s is Cartier and every nonzero section s∈H0(Y,OY(kPs))s \in H^0(Y, \mathcal{O}_Y(kP_s)), one has

ord⁡x(s)≤4kρt≤32kϵ.(10)\operatorname{ord}_x(s) \le4k\rho_t \le32k\epsilon. \tag*{(10)}

Proof. Fix tt for the moment. For each Cartier multiple kPskP_s and each integer aa, the condition

H0(Y,OY(kPs)⊗Ixa)≠0H^0(Y,\mathcal{O}_Y(kP_s) \otimes\mathcal{I}_x^a) \ne0

is a rank condition on the jet evaluation map over YsmY_{\mathrm{sm}}. We choose xx outside all proper rank-jumping loci of these countably many maps. Thus if the order bound fails at such a point, the relevant high-order kernel is nonzero for general marks as well. Taking powers of the offending sections gives the same strict inequality in arbitrarily large divisible degrees. This permits all subsequent choices of a sufficiently large divisible kk.

Choose n+1n+1 levels equally spaced from 2ρt2\rho_t to 3ρt3\rho_t; their gap is

δs=ρt/n.\delta_s = \rho_t/n.

If ord⁡x(s)>4kρt\operatorname{ord}_x(s) > 4k\rho_t in a sufficiently large degree, every one of these jet kernels is nonzero. The base locus of the lowest kernel cannot have xx as an isolated component. Indeed its base ideal at xx is contained in mx⌈2kρt⌉\mathfrak{m}_x^{\lceil2k\rho_t\rceil}, so the zero-dimensional case of Lemma 3.2 would give

1≤(k⌈2kρt⌉)nPsn≤2−n,1 \le\left(\frac{k}{\lceil2k\rho_t\rceil}\right)^n P_s^n \le2^{-n},

a contradiction.

Apply Lemma 3.3. It produces a dominant family of proper positive-dimensional base components VV, of some dimension 1≤f<n1 \le f < n, such that the entire higher jet kernel’s generic base ideal along VV is primary and contained in IVh\mathcal{I}_V^h, where

h=⌈kδs/2⌉,k/h≤2/δs.h = \lceil k\delta_s/2\rceil,\qquad k/h \le2/\delta_s.

For a general member, Lemma 3.2 gives

Psf⋅V≤(2/δs)n−fPsn,(11)P_s^f \cdot V \le(2/\delta_s)^{n-f}P_s^n, \tag*{(11)}
KV∗⋅Psf−1≤(12rt+2(n−f)δs)Psf⋅V,(12)K_{V^*}\cdot P_s^{f-1} \le\left(\frac{1}{2r_t}+\frac{2(n-f)}{\delta_s}\right)P_s^f\cdot V, \tag*{(12)}

where V∗V^* is a smooth projective resolution. The second inequality uses K≤Ps/(2rt)K \le P_s/(2r_t). The constants on the right are bounded independently of small tt, of kk, and of the member VV, by (3.9). We choose a very general incidence point before choosing the member VV. Its image belongs to YvgY^{\mathrm{vg}}, so V∗V^* is of general type by Proposition 2.2. Moreover PsP_s dominates LL in nef order. The inclusion of VV into YY, composed with its resolution, satisfies all the hypotheses of Lemma 3.4. Equations (3.11) to (3.12) would therefore give a curve through YvgY^{\mathrm{vg}} of bounded LL-degree, contradicting (3.2) as tt becomes small.

The bounds used in this contradiction do not depend on the initial degree in which excessive vanishing occurred. Consequently, after one restriction to sufficiently small tt, all Cartier multiples satisfy (10) at a very general point.

The analytic inputs and the lifting problem

The geometry will produce a divisor representing KYK_Y with coefficients of both signs. We shall prove that its full support is of logarithmic general type. The difficulty is to find the first section of an auxiliary nef adjoint before invoking a semiampleness criterion. The two analytic results below, proved in the complete companion [37], address exactly that difficulty. They concern actual rational line bundles.

A semipositive singular Hermitian metric has minimal singularities if its local weight is, up to a bounded additive error, no more singular than the weight of any other semipositive metric on the same bundle. For a rational line bundle this definition is made after taking one Cartier multiple and dividing the weights by that multiple.

Theorem 4.1 (Zero Lelong numbers for nef klt adjoints). Let (H,Θ)(H,\Theta) be a normal connected projective complex klt pair, where Θ≥0\Theta\ge0 is rational and DH=KH+ΘD_H = K_H + \Theta is nef and Q\mathbb{Q}-Cartier. Let π:V→H\pi: V \to H be any projective log resolution. The rational line bundle π∗DH\pi^*D_H admits a semipositive metric with minimal singularities, and every such metric has zero Lelong number at every point of VV. Its multiplier ideal is trivial for every positive exponent. Neither KHK_H nor Θ\Theta is required to be separately Q\mathbb{Q}-Cartier.

This is [37]. The adjoint hypothesis is material: a general nef line bundle need not have this metric regularity [8].

Theorem 4.2 (Ordinary interior injectivity). Let VV be a smooth projective complex variety and LL an integral divisor. Let 0≤C0≤C20 \le C_0 \le C_2 be effective rational divisors whose combined support has simple normal crossings. Suppose the actual rational line bundles L−C0L-C_0 and L−C2L-C_2 have semipositive singular Hermitian metrics with zero Lelong numbers at every point. For a rational number 0<λ<10 < \lambda< 1 put C1=(1−λ)C0+λC2C_1=(1-\lambda)C_0+\lambda C_2. The natural inclusion of sheaves induces an injection

H1(V,OV(KV+L−⌊C1⌋))⟶H1(V,OV(KV+L−⌊C0⌋)).H^1\left(V,\mathcal{O}_V\left(K_V+L-\lfloor C_1\rfloor\right)\right)\longrightarrow H^1\left(V,\mathcal{O}_V\left(K_V+L-\lfloor C_0\rfloor\right)\right).

The complete proof, including its passage to ordinary coherent cohomology, is in [37]. The analytic methods have antecedents in Fujino’s singular-metric treatment of harmonic forms and Matsumura’s uniform control of primitives [15] and [32]. Those results are not being identified with the interior comparison.

Here is the lifting problem to which we will apply the theorem. For a nef rational adjoint NN on a normal projective variety HH and a reduced closed subscheme S⊂HS \subset H, choose m>0m>0 with mNmN Cartier. The restriction sequence is

0⟶OH(mN)⊗IS⟶OH(mN)⟶OS(mN)⟶0.0\longrightarrow\mathcal{O}_H(mN)\otimes\mathcal{I}_S\longrightarrow\mathcal{O}_H(mN)\longrightarrow\mathcal{O}_S(mN)\longrightarrow0.

The obstruction to lifting a section on SS is its image under the connecting homomorphism, whose image is the kernel of

H1(H,OH(mN)⊗IS)⟶H1(H,OH(mN)).H^1\left(H,\mathcal{O}_H(mN)\otimes\mathcal{I}_S\right)\longrightarrow H^1\left(H,\mathcal{O}_H(mN)\right).

Thus injectivity of this ordinary cohomology map suffices to lift every section on the whole scheme SS. In the next section, SS is the reduced non-klt floor of an auxiliary lc boundary. Two nearby nef klt adjoints supply the endpoint metrics, and multiplier-ideal local vanishing identifies the theorem’s map with this inclusion. Threefold abundance supplies a section on the entire floor, with the conductor identifications already imposed.

Signed representatives and logarithmic general type

Fix the terminal canonical counterexample YY of Proposition 2.1, with the very general locus supplied by Proposition 2.2. The particular need for a signed divisor comes from the slice bundle P(OY⊕OY(ιKY))\mathbb{P}(\mathcal{O}_Y \oplus\mathcal{O}_Y(\iota K_Y)). Its two summands determine disjoint sections. Intersecting an integral multisection of degree e>0e > 0, distinct from those sections, with them and pushing to YY gives effective divisors D0,D∞D_0,D_\infty with D0−D∞∼eιKYD_0-D_\infty\sim e\iota K_Y, as verified in (41). Thus the representative of KYK_Y has signed coefficients, whereas the boundary is the reduced union of the two supports, including any components that cancel in their difference. We prove the logarithmic bigness needed to apply Lemma 3.4 to this boundary once its intersection degree has been bounded.

The proposition allows any reduced boundary containing the signed support. Its proof constructs an auxiliary nef adjoint with a nonempty reduced floor. The analytic results in Section 4 lift a section from that whole floor; only after this establishes nonnegative Kodaira dimension do we apply the required semiampleness theorem.

Proposition 5.1 (Signed representative alternative). Let YY be a projective Q\mathbb{Q}-factorial terminal fourfold such that KYK_Y is nef and κ(Y,KY)=−∞\kappa(Y,K_Y)=-\infty. Suppose that there is a very general locus of YY through whose points every proper positive-dimensional subvariety is of general type on resolution. Let JJ be a rational Weil divisor, with coefficients of either sign, satisfying J∼QKYJ \sim_{\mathbb{Q}} K_Y. Let p:W→Yp:W \to Y be a projective log resolution, and let DWD_W be a reduced simple normal crossings divisor containing the strict support of JJ and every pp-exceptional divisor. Then KW+DWK_W+D_W is big.

Proof. Put PW=KW+DWP_W=K_W+D_W. Terminality gives

KW=p∗KY+EW,EW≥0.K_W=p^*K_Y+E_W,\qquad E_W\geq0.

with EWE_W exceptional. In particular, both KWK_W and PWP_W are pseudo-effective. We assume that PWP_W is not big and derive a contradiction. We first reduce its Kodaira dimension to at most zero, then construct a nef boundary with a nonempty reduced floor. We will lift a nonzero section from that entire floor before using any semiampleness theorem that requires nonnegative Kodaira dimension.

Positive Kodaira dimension would already imply bigness

Suppose first that κ(PW)>0\kappa(P_W)>0. Resolve the rational map defined by a moving subsystem of a sufficiently divisible multiple bPWbP_W:

π:W~⟶W,f:W~⟶U.\pi:\widetilde{W}\longrightarrow W,\qquad f:\widetilde{W}\longrightarrow U.

Here W~\widetilde{W} is smooth, UU is the projective image, and, for a very ample line bundle OU(1)\mathcal{O}_U(1),

bπ∗PW∼f∗OU(1)+F,F≥0.(13)b\pi^*P_W\sim f^*\mathcal{O}_U(1)+F,\qquad F\geq0. \tag*{(13)}

If ff is generically finite, then PWP_W is big, contrary to the assumption. Otherwise 0<dim⁡U<40<\dim U<4. A smooth fiber component through a very general point of W~\widetilde{W} is birational to a proper positive-dimensional subvariety of YY meeting the very general locus. It is therefore of general type. We work over a smooth open of UU where generic smoothness applies. On its smooth fibers the restriction of KW~K_{\widetilde{W}} is the canonical bundle of the fiber, up to the constant one-dimensional factor coming from the base.

Fix an ample Cartier divisor H0H_0 on W~\widetilde{W}. For some integer j>0j>0, the restriction of jKW~−H0jK_{\widetilde{W}}-H_0 has a nonzero section on such a fiber component. Distinct components of a smooth fiber are disjoint, so the section can be taken to be zero on the other components. Choose the fiber over a point where the fiber dimension of the space of sections is the generic one for every integer jj; this requires only countably many exclusions. Consequently

f∗OW~(jKW~−H0)f_* \mathcal{O}_{\widetilde{W}}(jK_{\widetilde{W}}-H_0)

is generically nonzero for one jj. After tensoring by a sufficiently large power OU(c)\mathcal{O}_U(c), this coherent sheaf has a nonzero global section. Thus

jKW~+cf∗OU(1)−H0∼E0,E0≥0.jK_{\widetilde{W}}+cf^*\mathcal{O}_U(1)-H_0\sim E_0,\qquad E_0\geq0.

The divisor on the left before subtracting H0H_0 is big. By (13), adding an effective divisor gives bigness of jKW~+cbπ∗PWjK_{\widetilde{W}}+cb\pi^*P_W. Birational pushforward gives bigness of jKW+cbPWjK_W+cbP_W. For completeness, the ample divisor H0H_0 has big pushforward: for a fixed ample divisor HWH_W on WW and small positive rational η\eta, H0−ηπ∗HWH_0-\eta\pi^*H_W is ample, and pushing an effective rational representative proves this assertion. Finally

(j+cb)PW=jKW+cbPW+jDW(j+cb)P_W=jK_W+cbP_W+jD_W

is big. This contradiction proves

κ(PW)≤0.(14)\kappa(P_W)\leq0. \tag*{(14)}

A minimal model and a crepant klt perturbation

Run a log minimal model program for the rational dlt pair (W,DW)(W,D_W). We use flip existence for klt pairs, the usual dlt contraction properties, and termination of flips for pseudo-effective lc fourfolds, applied with zero nef part [3, 7]. The dlt flips needed here are obtained by lowering the finitely many boundary coefficients slightly while retaining negativity of the given extremal ray. The resulting pair is klt. On the relative Picard-number-one contraction, the original and perturbed negative adjoints are relatively proportional with positive rational ratio; the contraction theorem descends a Cartier multiple of their numerically trivial difference. The klt flip therefore has the required positivity for the original adjoint as well. This supplies the flips used in this dlt program.

There are only finitely many divisorial contractions. Pseudo-effectivity persists under each pushforward and strict transform and excludes a negative fiber space, by intersection with covering curves in a general fiber. These pushforwards on numerical divisor classes are well-defined on the Q\mathbb{Q}-factorial models: on a common resolution they are pullback followed by pushforward, and exceptional divisor classes give no ambiguity. We obtain a projective Q\mathbb{Q}-factorial dlt minimal model (Z,DZ)(Z,D_Z) without extracting divisors. Write

M=KZ+DZ.M=K_Z+D_Z.

The divisor DZD_Z is reduced, MM is nef, and the standard exceptional comparison on a common resolution preserves section spaces in sufficiently divisible degrees. Hence

κ(M)=κ(PW)≤0.\kappa(M)=\kappa(P_W)\leq0.

Moreover KZK_Z is pseudo-effective, since KWK_W is pseudo-effective. The signed representative supplies an additional linear relation. Indeed

PW∼Qp∗J+EW+DW,P_W\sim_{\mathbb{Q}}p^*J+E_W+D_W,

and the divisor on the right is supported on DWD_W. Its strict pushforward to ZZ is a signed rational divisor GZG_Z supported on DZD_Z, with

M∼QGZ.(15)M \sim_{\mathbb{Q}} G_Z. \tag*{(15)}

We next make a small klt perturbation while keeping a fixed Cartier multiple of MM. Choose an integer ℓ>0\ell> 0 for which ℓM\ell M is Cartier, and fix a rational number

0<δ<min⁡{12,116ℓ+2}.(16)0 < \delta< \min\left\{\frac{1}{2}, \frac{1}{16\ell+2}\right\}. \tag*{(16)}

The klt adjoint

M−δDZ=KZ+(1−δ)DZM-\delta D_Z=K_Z+(1-\delta)D_Z

is pseudo-effective because KZK_Z is pseudo-effective and (1−δ)DZ(1-\delta)D_Z is effective. Run its minimal model program. We show inductively that every step is crepant for MM, preserves nefness of MM, and preserves the Cartier property of ℓM\ell M.

At a given step let RR be a negative extremal ray for the driving adjoint. Since MM is nef and δ<1/2\delta< 1/2, the ray is also negative for the klt adjoint M−DZ/2M-D_Z/2. The length bound gives a rational curve CC spanning RR such that

0<−(M−DZ/2)⋅C≤2dim⁡Z=8.0<-(M-D_Z/2)\cdot C\leq2\dim Z=8.

Set aC=M⋅Ca_C=M\cdot C and bC=DZ⋅Cb_C=D_Z\cdot C. Then

aC≥0,bC≤2aC+16,aC<δbC.a_C\geq0,\qquad b_C\leq2a_C+16,\qquad a_C<\delta b_C.

It follows that

0≤aC<16δ1−2δ<1ℓ.0\leq a_C<\frac{16\delta}{1-2\delta}<\frac{1}{\ell}.

Because ℓM\ell M is Cartier, aC∈ℓ−1Za_C\in\ell^{-1}\mathbb{Z}, and therefore aC=0a_C=0.

The line-bundle clause of the contraction theorem now descends OZ(ℓM)\mathcal{O}_Z(\ell M) to an actual line bundle on the contraction base [12]; the same theorem’s part (5) gives the length bound just used. For a divisorial contraction its pullback is the original bundle. For a flip it pulls back on both sides. Consequently MM remains nef, the same multiple ℓM\ell M remains Cartier, and its pullbacks to a common resolution agree. This is crepancy for the full adjoint, rather than numerical triviality alone. More explicitly, choose a rational section of the descended line bundle. The divisor ℓM\ell M differs from its pullback divisor by a principal divisor; transform the same rational function across the flip. The two exact divisor pullbacks then agree on a common resolution, with compatible canonical divisors. The driving pair stays klt. The boundary with coefficient 1/21/2 is smaller than the driving boundary, so it is again klt at the next step. The preceding argument therefore repeats with the same ℓ\ell and δ\delta.

Let Z′Z' be the resulting model, and denote strict transforms by D′D', M′M', and G′G'. Put K′=KZ′K'=K_{Z'}. We have

(Z′,D′) is lc,K′ is pseudo-effective,M′∼QG′,κ(M′)≤0,M′−uD′ is nef and (Z′,(1−u)D′) is klt(0<u≤δ).(17)\begin{aligned} &(Z',D')\text{ is lc},\qquad K'\text{ is pseudo-effective},\qquad M'\sim_{\mathbb{Q}}G',\qquad\kappa(M')\leq0,\\ &M'-uD'\text{ is nef and }(Z',(1-u)D')\text{ is klt}\qquad(0<u\leq\delta). \tag*{(17)} \end{aligned}

Here the last nefness assertion follows by interpolation between M′M' and M′−δD′M'-\delta D'. The klt assertion follows by interpolation between the klt driving pair and the lc full-boundary pair. The underlying variety Z′Z' is klt.

We have reduced the problem to a fixed nef interval of actual klt adjoints and a signed representative supported on its boundary. We next use that representative to locate a nonempty boundary floor.

A nonempty floor and the reduced non-klt ideal

Some coefficient of G′G' is positive. Suppose otherwise. Intersect K′+D′∼QG′≤0K' + D' \sim_{\mathbb{Q}} G' \le0 with the third power of an ample divisor. Pseudo-effectivity of K′K' and effectivity of D′D' show that all inequalities are equalities; positivity for nonzero effective divisors then gives D′=0D' = 0 and G′=0G' = 0.

To see why this is impossible, take a common smooth resolution VV of WW and Z′Z'. The pullback to VV of the signed divisor JJ is supported over DWD_W. Since the programs extract no divisors and D′=0D' = 0, this pullback is exceptional over Z′Z'. It is rationally linearly equivalent to the pullback of KYK_Y, and hence is nef. The negativity lemma makes this exceptional divisor nonpositive. Its intersection with an ample divisor to the third power is nonnegative by nefness and nonpositive by its sign; it must vanish. Thus the pullback of KYK_Y is rationally linearly trivial, contrary to κ(Y,KY)=−∞\kappa(Y,K_Y) = -\infty.

Write D′=∑jDj′D' = \sum_j D'_j and G′=∑jgjDj′G' = \sum_j g_jD'_j, allowing gj=0g_j = 0. Let a=max⁡jgj>0a = \max_j g_j > 0. Choose a sufficiently small positive rational ss and define

B=(1−s)D′+saG′,α=1+sa,N=K′+B.B = (1-s)D' + \frac{s}{a}G', \qquad\alpha= 1 + \frac{s}{a}, \qquad N = K' + B.

Choose ss so that every coefficient 1−s+(s/a)gj1-s+(s/a)g_j is nonnegative and s/α∈(0,δ)s/\alpha\in(0,\delta). All these coefficients are at most one, with equality precisely when gj=ag_j = a. Therefore

0≤B≤D′,S:=⌊B⌋≠0,N∼QαM′−sD′.0 \le B \le D', \qquad S := \lfloor B \rfloor\ne0, \qquad N \sim_{\mathbb{Q}} \alpha M' - sD'.

The divisor NN is nef by (17). The pair (Z′,B)(Z', B) is lc and klt outside SS. Indeed, outside SS its finitely many boundary coefficients are bounded above by a number less than one; interpolate the lc full-boundary pair with the underlying klt variety. The same reasoning shows that (Z′,bB)(Z', bB) is klt whenever 0<b<10 < b < 1.

The multiplier ideals are actual ideals

J(Z′,B)=IS,J(Z′,bB)=OZ′(0<b<1).(18)\mathcal{J}(Z', B) = \mathcal{I}_S, \qquad\mathcal{J}(Z', bB) = \mathcal{O}_{Z'} \quad(0 < b < 1). \tag*{(18)}

Here SS carries its reduced induced structure. To verify the first identity, use the discrepancy description on a log resolution. Since the pair is lc, a regular function satisfies every positive log-discrepancy condition automatically. At a log-discrepancy-zero divisor it must vanish to positive order. All such centers lie in SS, and each component of SS itself gives such a condition. A function vanishing on reduced SS has positive order at every valuation centered in SS; conversely the component valuations force vanishing on SS. This proves the identity. These are multiplier ideals for an lc pair, not a substitution of a non-lc ideal for the reduced ideal.

Lifting sections from the floor

We claim that, for every sufficiently large and divisible integer mm, the following restriction map to the whole reduced floor SS is surjective:

H0(Z′,OZ′(mN))⟶H0(S,OS(mN)).(19)H^0(Z', \mathcal{O}_{Z'}(mN)) \longrightarrow H^0(S, \mathcal{O}_S(mN)). \tag*{(19)}

The interior injectivity theorem will compare the boundary BB with b0Bb_0B for b0<1b_0 < 1, where the pair is klt. It also requires an endpoint b2Bb_2B beyond BB. The corresponding residual bundle is (m−1)N−(b2−1)B(m-1)N-(b_2-1)B; its positivity is supplied by the interval (17). We now verify this for both endpoints.

Fix rational numbers 0<b0<1=b1<b20 < b_0 < 1 = b_1 < b_2 and a projective log resolution h ⁣:R→Z′h \colon R \to Z' of (Z′,D′)(Z', D'), hence also of (Z′,B)(Z', B). Choose a fixed effective integral hh-exceptional divisor ARA_R, with coefficients large enough that

Ci=AR+h∗(K′+biB)−KR≥0(i=0,1,2).C_i = A_R + h^*(K' + b_iB) - K_R \ge0 \qquad(i = 0,1,2).

Their supports lie in one simple normal crossings divisor, and C0≤C1≤C2C_0 \le C_1 \le C_2. Moreover C1C_1 is the strict interior convex combination of C0C_0 and C2C_2 with parameter (1−b0)/(b2−b0)(1-b_0)/(b_2-b_0). For mNmN Cartier put

LR=AR+h∗(mN)−KR.L_R = A_R + h^*(mN) - K_R.

This is an integral divisor. Its endpoint residuals are

LR−Ci=h∗((m−1)N+(1−bi)B)∼Qh∗(ti(m)M′−vi(m)D′),(20)\begin{aligned} L_R - C_i &= h^*((m-1)N + (1-b_i)B) \\ &\sim_{\mathbb{Q}} h^*\bigl(t_i(m)M' - v_i(m)D'\bigr), \tag*{(20)} \end{aligned}
ti(m)=(m−1)α+(1−bi)s/a,vi(m)=(m−1)s−(1−bi)(1−s).t_i(m) = (m-1)\alpha+ (1-b_i)s/a, \qquad v_i(m) = (m-1)s - (1-b_i)(1-s).

For i=0,2i = 0,2, ti(m)>0t_i(m) > 0 once mm is large, and

ui(m):=vi(m)ti(m)⟶sα∈(0,δ).u_i(m) := \frac{v_i(m)}{t_i(m)} \longrightarrow\frac{s}{\alpha} \in(0,\delta).

Consequently each endpoint residual is rationally linearly equivalent to a positive rational multiple of h∗(K′+(1−ui(m))D′)h^*(K' + (1-u_i(m))D'), a nef klt adjoint pulled back to its log resolution. By Theorem 4.1, it admits a semipositive singular metric with zero Lelong numbers at every point. Taking positive rational powers and transporting by the actual rational line-bundle isomorphisms preserves this property. The endpoint hypotheses of Theorem 4.2 are therefore satisfied.

That theorem gives injectivity from the first ordinary cohomology group of KR+LR−⌊C1⌋K_R+L_R-\lfloor C_1\rfloor to that of KR+LR−⌊C0⌋K_R+L_R-\lfloor C_0\rfloor. The precise floor calculation is

KR+LR−⌊Ci⌋=h∗(mN)+⌈KR−h∗(K′+biB)⌉.(21)K_R + L_R - \lfloor C_i\rfloor= h^*(mN) + \lceil K_R - h^*(K' + b_iB)\rceil. \tag*{(21)}

Multiplier-ideal local vanishing and the projection formula [12] identify these groups with

H1(Z′,OZ′(mN)⊗J(Z′,biB)).H^1\bigl(Z', \mathcal{O}_{Z'}(mN) \otimes\mathcal{J}(Z',b_iB)\bigr).

The comparison map is the map induced by inclusion of the multiplier ideals. By (18), we have proved injectivity of

H1(Z′,OZ′(mN)⊗IS)⟶H1(Z′,OZ′(mN)).H^1\bigl(Z',\mathcal{O}_{Z'}(mN)\otimes I_S\bigr) \longrightarrow H^1\bigl(Z',\mathcal{O}_{Z'}(mN)\bigr).

The exact sequence of SS proves (19).

The restriction map is now surjective. To obtain a nonzero global section, we must produce one on the whole reduced scheme SS. We do this on a dlt floor using adjunction and threefold abundance. The next step therefore includes both gluing on that floor and actual line-bundle descent to SS.

Whole-floor abundance and descent

Take a projective Q\mathbb{Q}-factorial dlt blowup

g ⁣:(Q,BQ)⟶(Z′,B),KQ+BQ=g∗(K′+B)=g∗N,g \colon(Q,B_Q) \longrightarrow(Z',B), \qquad K_Q+B_Q = g^*(K'+B) = g^*N,

extracting only lc places; this is the lc case of the dlt blowup theorem [14]. Set T=⌊BQ⌋T=\lfloor B_Q\rfloor. It is nonempty. Whole-floor dlt adjunction equips TT with an effective rational different Diff⁡T\operatorname{Diff}_T such that

KT+Diff⁡T=(KQ+BQ)∣T=g∗N∣TK_T+\operatorname{Diff}_T=(K_Q+B_Q)|_T=g^*N|_T

as the actual rational adjoint line bundle, including the conductor and residue identifications on the normalization. The pair on TT is semi-dlt; see [10] and [13]. We record the depth condition needed for this whole-floor statement. The underlying QQ is klt and Q\mathbb{Q}-factorial. Both OQ\mathcal{O}_Q and OQ(−T)\mathcal{O}_Q(-T) are Cohen–Macaulay. For the latter assertion, locally trivialize a Cartier multiple of TT and take the normal cyclic index cover. It is finite and quasi-étale, hence klt and Cohen–Macaulay. Its finite pushforward decomposes into the corresponding rank-one reflexive sheaves, including OQ(−T)\mathcal{O}_Q(-T); in characteristic zero these are direct summands. They are therefore Cohen–Macaulay. The sequence

0⟶OQ(−T)⟶OQ⟶OT⟶00\longrightarrow\mathcal{O}_Q(-T)\longrightarrow\mathcal{O}_Q\longrightarrow\mathcal{O}_T\longrightarrow0

then gives S2S_2 for TT (in fact the required Cohen–Macaulay depth along its support). Its codimension-one crossings and the conductor description come from the dlt structure. Thus the semi-log-canonical adjunction in (5.11) is on the whole projective threefold, not on a disjoint collection of its components.

The adjoint in (5.11) is nef. Projective semi-dlt threefold abundance makes it semiample [10]. Hence

H0(T,OT(mg∗N))≠0H^0(T,\mathcal{O}_T(mg^*N))\ne0

for all sufficiently divisible positive mm.

These sections descend to SS. Indeed J(Q,BQ)=OQ(−T)\mathcal{J}(Q,B_Q)=\mathcal{O}_Q(-T), and crepancy together with multiplier-ideal local vanishing gives

g∗OQ(−T)=IS,Rig∗OQ(−T)=0(i>0).(22)g_*\mathcal{O}_Q(-T)=\mathcal{I}_S,\qquad R^i g_*\mathcal{O}_Q(-T)=0\quad(i>0). \tag*{(22)}

One can compute both assertions on a common log resolution of (Q,BQ)(Q,B_Q) and (Z′,B)(Z',B). The equality of their pulled-back adjoints identifies the discrepancy round-up sheaves, and local vanishing for each log resolution followed by Leray gives (22). Since Z′Z' is normal, g∗OQ=OZ′g_*\mathcal{O}_Q=\mathcal{O}_{Z'}. Pushing forward the divisor sequence therefore gives

g∗OT=OS.g_*\mathcal{O}_T=\mathcal{O}_S.

The projection formula identifies the nonzero section spaces above with H0(S,OS(mN))H^0(S,\mathcal{O}_S(mN)). Choose mm both sufficiently divisible for this semiampleness and sufficiently large for (19). A nonzero section on TT then descends to SS and lifts to Z′Z'. We have proved κ(N)≥0\kappa(N)\ge0.

The final klt adjoint

Because B≤D′B\le D', section inclusion in divisible degrees gives κ(N)≤κ(M′)≤0\kappa(N)\le\kappa(M')\le0. Thus κ(N)=0\kappa(N)=0. Now consider the klt pair

(Z′,(1−sα)D′).\left(Z',\left(1-\frac{s}{\alpha}\right)D'\right).

Its nef adjoint is rationally linearly equivalent to N/αN/\alpha, so its Kodaira dimension is zero. By Theorem 4.1, on a smooth projective log resolution a positive Cartier multiple of its pullback has a semipositive singular metric with zero point Lelong numbers. All hypotheses of the fourfold semiampleness result of Gongyo–Matsumura are now satisfied: the pair is projective klt with rational boundary, the adjoint has nonnegative Kodaira dimension, and the specified pullback metric exists [17].

Semi-ampleness and Kodaira dimension zero make this adjoint numerically trivial. On the other hand, K′K' is pseudo-effective, D′≠0D' \ne0 because G′G' has a positive coefficient, and 1−s/α>01-s/\alpha> 0. Intersecting K′+(1−s/α)D′K' + (1-s/\alpha)D' with the third power of an ample divisor gives a strictly positive number. This contradiction proves the proposition.

Moving jets on a two-slot bundle

We continue with the terminal fourfold YY, its nef non-big canonical divisor KK, and the polarizations of (3). Thus n=4n=4, the integer ι>0\iota> 0 makes ιK\iota K Cartier, and

L=Lt=rt(K+tA),Ln⟶ϵn,rt⟶∞.L=L_t=r_t(K+tA),\qquad L^n \longrightarrow\epsilon^n,\qquad r_t\longrightarrow\infty.

The positive number ϵ\epsilon is fixed throughout this section. Retain the fixed locus YvgY^{\mathrm{vg}} from Section 3, on which Proposition 2.2 holds and every integral curve has KK-degree at least 1/ι1/\iota. In particular,

L⋅C≥rt/ιif C passes through a point of Yvg.(23)L\cdot C\ge r_t/\iota\quad\text{if }C\text{ passes through a point of }Y^{\mathrm{vg}}. \tag*{(23)}

A very general locus here means the complement of a countable union of proper closed subsets. We may enlarge that union whenever finitely or countably many additional conditions are imposed.

The scalar estimate of Proposition 3.5 limits vanishing on one copy of YY. We now seek the complementary estimate: a polarization on a projective bundle over Y×YY\times Y generates many jets at a very general point. Its Seshadri constant measures this local positivity [29].

Failure of the estimate would produce a moving base component. Positive-dimensional fibers over either copy of YY are excluded on a bundle slice, using general type and, for a multisection, Proposition 5.1. If both projections are generically finite, the required contradiction has a different source: ramification bounds reduce the family to finitely many fixed covers, and their birational automorphisms cannot sweep the product. We isolate that argument before applying the moving-center method.

The bundle and its volumes

Put S0=ιKS_0=\iota K, an actual Cartier divisor on YY. On Y×YY\times Y, a subscript denotes pullback from the corresponding factor. Let

π:Z=P(O(S0,1)⊕O(S0,2))⟶Y×Y,ξ=c1(OZ(1)).(24)\pi:Z=\mathbb{P}\bigl(\mathcal{O}(S_{0,1})\oplus\mathcal{O}(S_{0,2})\bigr)\longrightarrow Y\times Y,\qquad\xi=c_1(\mathcal{O}_Z(1)). \tag*{(24)}

We use the convention

π∗OZ(aξ)=Sym⁡a(O(S0,1)⊕O(S0,2))(a≥0).\pi_*\mathcal{O}_Z(a\xi)=\operatorname{Sym}^a\bigl(\mathcal{O}(S_{0,1})\oplus\mathcal{O}(S_{0,2})\bigr)\qquad(a\ge0).

We suppress pullback symbols for divisors on the base. For a positive integer qq, define

P=L1+L2+qξ,d=dim⁡Z=2n+1=9.P=L_1+L_2+q\xi,\qquad d=\dim Z=2n+1=9.

This qq is a bundle weight; it is unrelated to the irregularity q(Y)=0q(Y)=0.

The two summands determine two disjoint sections, called the axes. The complement of the axes is the torus open of ZZ. Fixing either base coordinate at a point and trivializing the constant line gives a slice

πsl:Zsl=P(OY⊕OY(S0))⟶Y,Psl=L+qξsl.(25)\pi_{\mathrm{sl}}: Z_{\mathrm{sl}} = \mathbb{P}(\mathcal{O}_{Y} \oplus\mathcal{O}_{Y}(S_{0})) \longrightarrow Y, \qquad P_{\mathrm{sl}} = L + q\xi_{\mathrm{sl}}. \tag*{(25)}

The restriction of PP is identified with PslP_{\mathrm{sl}}; the remaining constant factor is trivialized when restricting sections.

Lemma 6.1. The varieties Y×YY \times Y, ZZ, and ZslZ_{\mathrm{sl}} are projective, Q\mathbb{Q}-factorial, and klt. The tautological classes of the two bundles are nef, and PP and PslP_{\mathrm{sl}} are ample rational divisors. Writing KΣ=K1+K2K_{\Sigma} = K_{1} + K_{2} on the product and KΣ=KK_{\Sigma} = K on a slice, one has

Kbundle=−2ξ+(ι+1)KΣ≤ι+1rtPbundle(26)K_{\mathrm{bundle}} = -2\xi+ (\iota+ 1)K_{\Sigma} \leq\frac{\iota+ 1}{r_{t}}P_{\mathrm{bundle}} \tag*{(26)}

in nef order.

Proof. Let p:Y~→Yp:\widetilde{Y} \to Y be a smooth projective resolution. Rational singularities and the irregularity conclusion in Proposition 2.1 give q(Y~)=0q(\widetilde{Y}) = 0. The product description of the Picard group, or the seesaw principle and the vanishing of Hom⁡(Alb⁡(Y~),Pic⁡0(Y~))\operatorname{Hom}(\operatorname{Alb}(\widetilde{Y}),\operatorname{Pic}^{0}(\widetilde{Y})), gives

Pic⁡(Y~×Y~)=pr⁡1∗Pic⁡(Y~)⊕pr⁡2∗Pic⁡(Y~).\operatorname{Pic}(\widetilde{Y} \times\widetilde{Y}) = \operatorname{pr}_{1}^{*}\operatorname{Pic}(\widetilde{Y}) \oplus\operatorname{pr}_{2}^{*}\operatorname{Pic}(\widetilde{Y}).

For a prime Weil divisor on Y×YY \times Y, take its strict transform on this smooth product. Its Cartier class is a sum of pullbacks from the two factors. Pushing down the corresponding linear equivalence expresses the original Weil divisor class as a sum of pullbacks of Weil divisor classes on YY. These are Q\mathbb{Q}-Cartier because YY is Q\mathbb{Q}-factorial. Thus Y×YY \times Y is Q\mathbb{Q}-factorial. Exceptional components have images of codimension at least two and do not affect this divisor-class calculation.

The bundle over Y~×Y~\widetilde{Y} \times\widetilde{Y} is a smooth resolution of ZZ. Its Picard group is the Picard group of the base plus the integral tautological class. Pushing down as above proves Q\mathbb{Q}-factoriality of ZZ. The identical argument over Y~\widetilde{Y} proves it for the slice. A product of canonical varieties is canonical, as follows directly from the product of resolutions and the canonical discrepancy formula. Projective bundles are smooth over their bases, so the bundles are klt as well.

The direct sum of nef line bundles is nef; hence its tautological class is nef. That class is also relatively ample. Adding a positive pullback of an ample class therefore makes it ample: for example, write the sum as a positive multiple of a relatively ample class made ample by a sufficiently large base twist, plus nef classes. This proves the assertions about PP and PslP_{\mathrm{sl}}. Finally, the canonical bundle formula for a rank-two projective bundle gives the equality in (26). Since ξ\xi is nef and KΣ≤LΣ/rtK_{\Sigma} \leq L_{\Sigma}/r_{t}, the stated nef inequality follows. □

Lemma 6.2. Assume qι/rt≤1q\iota/r_{t} \leq1. For sufficiently small tt, there are positive constants cn,Cnc_{n}, C_{n}, depending only on nn, such that

cnqϵ2n≤Pd≤Cnqϵ2n.(27)c_{n}q\epsilon^{2n} \leq P^{d} \leq C_{n}q\epsilon^{2n}. \tag*{(27)}

On either slice,

0<Psln+1≤2n+2qϵn.(28)0 < P_{\mathrm{sl}}^{n+1} \leq2^{n+2}q\epsilon^{n}. \tag*{(28)}

Proof. For a rank-two split bundle with first Chern classes E1,E2E_{1}, E_{2}, the projective-bundle formula is

π∗(ξi)=∑a+b=i−1E1aE2b(i≥1),π∗(1)=0.\pi_{*}(\xi^{i}) = \sum_{a+b=i-1} E_{1}^{a}E_{2}^{b}\quad(i \geq1), \qquad\pi_{*}(1) = 0.

All classes in the expansion of PdP^d are nef. Put LΣ=L1+L2L_\Sigma= L_1 + L_2. Each Ej=S0,jE_j = S_{0,j} is bounded above in nef order by (ℓ/rt)LΣ(\ell/r_t)L_\Sigma. Consequently

dqLΣ2n≤Pd≤qLΣ2n∑i=1di(di)(qℓ/rt)i−1≤d2d−1qLΣ2n.dqL_\Sigma^{2n} \leq P^d \leq qL_\Sigma^{2n}\sum_{i=1}^{d} i\binom{d}{i}(q\ell/r_t)^{i-1} \leq d2^{d-1}qL_\Sigma^{2n}.

Here LΣ2n=(2nn)(Ln)2L_\Sigma^{2n} = \binom{2n}{n}(L^n)^2, and Ln→ϵn>0L^n \to\epsilon^n > 0. This proves (27).

On a slice one summand is trivial, so

Psln+1=∑i=1n+1(n+1i)qiLn+1−iS0i−1≤qLn∑i=1n+1(n+1i).P_{\mathrm{sl}}^{n+1} = \sum_{i=1}^{n+1}\binom{n+1}{i}q^iL^{n+1-i}S_0^{i-1} \leq qL^n\sum_{i=1}^{n+1}\binom{n+1}{i}.

For small tt, we may use Ln≤2ϵnL^n \leq2\epsilon^n, giving (28). Positivity follows either from ampleness or from the i=1i=1 term.

We now choose the parameters in the order required by the proof. After fixing ϵ\epsilon, choose δ>0\delta> 0 such that

(2/δ)n2n+2ϵn<1.(2/\delta)^n 2^{n+2}\epsilon^n < 1.

Next choose an integer q>0q > 0 so large that the lower bound in (27) gives

Pd>(2n+3+dδ)dP^d > (2n+3+d\delta)^d

for all sufficiently small tt. This is possible because that lower bound is linear in qq. The integer qq is now fixed. Finally decrease tt, imposing qℓ/rt≤1q\ell/r_t \leq1 and all the preceding estimates. Further decreases of tt do not change ϵ\epsilon, δ\delta, or qq.

The large Seshadri estimate

For an ample rational divisor PP and a smooth point zz, write

ϵ(P;z)=inf⁡C∋zP⋅Cmult⁡zC.\epsilon(P;z)=\inf_{C\ni z}\frac{P\cdot C}{\operatorname{mult}_z C}.

where the infimum is over integral projective curves through zz.

Proposition 6.3 (Two-slot jets). Let ZZ and PP be defined by (24) to (6.3). Fix ϵ>0\epsilon> 0, choose δ\delta satisfying (6.8), and then fix qq large enough for (6.9). For all sufficiently small positive rational tt, one has

ϵ(P;z)>2n+2=10(29)\epsilon(P;z)>2n+2=10 \tag*{(29)}

at a very general smooth point of the torus open of ZZ.

Dominant finite correspondences

The final case of the jet argument will be a family of nn-dimensional subvarieties whose two projections to YY are generically finite. The following proposition excludes such a family using only bounds for its degree and canonical intersection. The family itself may change with tt.

Proposition 6.4 (Bounded correspondences cannot sweep the bundle). Fix ϵ>0\epsilon> 0, an integer q>0q > 0, and positive constants B0B_0, B1B_1. Keep YY, KK, AA, LtL_t and P=L1+L2+qξP = L_1 + L_2 + q\xi as above. For all sufficiently small positive rational tt, there is no irreducible finite-type parameter space TT and integral closed subvariety Γ⊂T×Z\Gamma\subset T \times Z, dominant over TT, with the following properties:

(i) The evaluation Γ→Z\Gamma\to Z is dominant, and a general fiber VV over TT is an integral subvariety of dimension nn.

(ii) On a smooth projective resolution V∗→VV^{*} \to V, both projections gi:V∗→Yg_i: V^{*} \to Y, i=1,2i = 1, 2, are dominant and generically finite.

(iii) Writing PP also for its pullback to V∗V^{*}, one has

0<Pn⋅V≤B0,KV∗Pn−1≤B1(Pn⋅V).0 < P^n \cdot V \le B_0, \qquad K_{V^{*}}P^{n-1} \le B_1(P^n \cdot V).

The restriction on tt depends only on the fixed geometry and ϵ\epsilon, qq, B0B_0, B1B_1, not on the parameter space or family.

Proof. We first rule out branch divisors that sweep YY, using the intersection bounds uniformly in tt. We then fix tt and the family: a common branch complement gives finitely many covers, whose birational graph families lead to an abelian variety dominating YY.

Since P−gi∗LP-g_i^{*}L is nef, the projection formula gives

deg⁡(gi)Ln≤Pn⋅V≤B0.\deg(g_i)L^n \le P^n \cdot V \le B_0.

The degrees are uniformly bounded because Ln→ϵn>0L^n \to\epsilon^n > 0. This degree bound alone does not give a finite list of covers; we must first control their branch loci.

Numerical bounds for branch divisors. Resolve the general members of the incidence family in family. After shrinking the irreducible parameter space, there is a smooth projective family V∗→TV^{*} \to T with integral fibers birational to the corresponding VV, together with the two generically finite morphisms gi:V∗→Yg_i: V^{*} \to Y on each fiber. For either projection, let Ti→YT_i \to Y denote the finite normal Stein factor. Its function field is C(V)\mathbb{C}(V).

If JJ is a branch prime of Ti→YT_i \to Y, a ramification prime on TiT_i has a strict transform RR on V∗V^{*}. A proper birational morphism to a normal variety is an isomorphism at the generic point of each target divisor, so this transform is present. Over the smooth locus of YY, its ramification coefficient is at least one. There is an effective canonical comparison

KV∗∼Qgi∗K+Ei,Ei≥R.(30)K_{V^{*}} \sim_{\mathbb{Q}} g_i^{*}K + E_i, \qquad E_i \ge R. \tag*{(30)}

For completeness, resolve the rational lift to a resolution of the terminal target. Ramification between smooth varieties and the effective terminal discrepancies give this formula upstairs; pushing down to V∗V^{*} gives Equation (6.12).

Set dJ=Ln−1⋅Jd_J = L^{n-1} \cdot J. Projection and nef order imply

0<dJ≤Pn−1⋅R≤KV∗Pn−1≤C3,(31)0 < d_J \le P^{n-1} \cdot R \le K_{V^{*}}P^{n-1} \le C_3, \tag*{(31)}

where C3=B1B0C_3 = B_1B_0 is independent of tt and of the family. The same estimate applies to every prime divisorial image of ramification that meets YsmY_{\mathrm{sm}}.

We also need a canonical bound on JJ, which need not be normal. On YsmY_{\mathrm{sm}}, the divisor JJ is a Gorenstein hypersurface. If ν:Jν→J\nu:J^{\nu} \to J is its normalization, finite duality gives, in codimension one,

KJν+Dcond∼Qν∗((K+J)∣J),Dcond≥0.K_{J^{\nu}} + D_{\mathrm{cond}} \sim_{\mathbb{Q}} \nu^{*}((K+J)|_J), \qquad D_{\mathrm{cond}} \ge0.

The conductor therefore has the sign that decreases the normalized canonical intersection. Terminal singularities are smooth in codimension two, so J∩YsingJ \cap Y_{\mathrm{sing}} has dimension at most n−3n-3. Its inverse image on the normalization has codimension at least two. It introduces no omitted codimension-one term in this comparison. On a resolution J∗J^\ast, the exceptional canonical cycles push to zero against n−2n-2 pullbacks of LL. Consequently

KJ∗Ln−2≤(K+J)JLn−2≤dJ/rt+dJ2/Ln≤C4dJ.(32)K_{J^\ast}L^{n-2} \le(K+J)JL^{n-2} \le d_J/r_t + d_J^2/L^n \le C_4d_J. \tag*{(32)}

Here K≤L/rtK \le L/r_t. The square term is the Hodge-index inequality

J2Ln−2≤(JLn−1)2Ln.J^2L^{n-2} \le\frac{(JL^{n-1})^2}{L^n}.

It applies to the Q\mathbb{Q}-Cartier divisor JJ; one can pull back to a resolution and approximate the nef class LL by ample classes. The bound in (31) and the positive lower bound for LnL^n make C4C_4 uniform.

If a family of these prime images dominates YY, choose a very general member and then a very general point on its resolution mapping to YvgY^{\mathrm{vg}}. Such a choice is legitimate despite the countable exceptional set. For each excluded proper closed subset of YY, dominance says that the generic image divisor is not contained in it; omit the corresponding proper parameter locus. On the remaining very general member, omit the inverse images of the countably many excluded subsets, together with the finite birational-system and quasi-finiteness exceptions. The chosen image divisor is of general type by Proposition 2.2. Its top LL-degree is dJd_J, and (32) is the required canonical bound. Lemma 3.4 excludes this sweeping family for sufficiently small tt.

A fixed branch complement and finitely many covers. The preceding exclusion holds uniformly over all families in the statement. Now fix one such sufficiently small tt and its incidence family. No further decrease of tt will be made in this proof. The smooth projective family V∗→TV^\ast\to T has integral fibers, and both projections to the normal variety YY are dominant and generically finite. Their degrees are bounded by (6.11). After a finite parameter extension and shrinking, follow the finitely many geometric generic components of the relative Jacobian over YsmY_{\mathrm{sm}}. Every followed component whose fiber image is a divisor has proper total image closure: the preceding argument excludes a dominant such family using Equations (31) and (32).

These are exactly the hypotheses of the simultaneous finite-cover lemma [38], Lemma 7.5. It gives one smooth nonempty open Y∘⊂YY^\circ\subset Y over which every general finite Stein cover in either slot is finite étale, and finite lists of the resulting normal covers of YY. The lemma accounts for every branch prime by its ramification strict transform, then applies purity and finiteness of bounded-degree étale covers of the fixed open. In particular, this is a finite-type family argument; a numerical branch bound alone would not suffice. The open and lists may depend on the fixed tt and incidence family. No uniformity in those choices is needed.

Countably many birational graph families. Each VV gives a birational map between one cover from each list: both finite Stein factors have function field C(V)\mathbb{C}(V). Its image in Y×YY \times Y is the finite image of the closure of that birational graph. Fix one pair of covers that are birational. A smooth projective resolution of their common birational class has pseudo-effective canonical class, by the effective canonical comparison with the nef KK on YY. It is non-uniruled by [5].

The birational-group structure theorem of Hanamura [19], in the form stated in [4], Proposition 3.7 and Theorem 3.8, permits a smooth projective model UU of this class for which the reduced flat-graph birational scheme is a group scheme locally of finite type and

AU=Aut⁡0(U)A_U = \operatorname{Aut}^{0}(U)

is its identity component, an abelian variety. The flat graphs are represented in graph Hilbert schemes. There are countably many Hilbert polynomials and finitely many components in each finite-type Hilbert scheme, so the birational maps occur in countably many translates AUbA_U b.

For such a translate, its graphs are parametrized on a dense open by the rational evaluation map

U×AU⇢U×U,(x,a)⟼(x,a⋅b(x)).U \times A_U \dashrightarrow U \times U,\qquad(x,a) \longmapsto(x,a\cdot b(x)).

If this map is not dominant, its image closure is a proper closed subset of U×UU \times U. Fix birational identifications of UU with the two covers. Every graph meets the product of their fixed birational opens densely, because it dominates both factors. Transporting the image closure through those opens, then taking its closure in the product of covers, preserves its dimension. The subsequent finite map to Y×YY \times Y also preserves dimension. Thus all correspondences belonging to this translate are contained in a proper closed subset of Y×YY \times Y. The possible boundary of an individual birational map introduces no new component: the generic graph has already been included.

There are finitely many cover pairs and countably many translates for each pair. If every map in (6.15) were nondominant, the image of the original incidence would be contained in a countable union of proper closed subsets of Y×YY \times Y. But Γ→Z\Gamma\to Z is dominant, so its composite to Y×YY \times Y is dominant and its image contains a nonempty open subset. Over the uncountable field C\mathbb{C}, such an open cannot be covered by countably many proper closed subsets. Therefore the map in (6.15) is dominant for at least one translate.

The abelian curve contradiction. For a general xx in this last evaluation, AU⋅b(x)A_U \cdot b(x) is a dense orbit in UU. A stabilizer element fixes every point of that orbit by commutativity; it fixes UU by density. The action of Aut⁡0(U)\operatorname{Aut}^{0}(U) is faithful, so the stabilizer is zero-dimensional. Hence the orbit map from AUA_U is generically finite dominant. Composing with the rational map through either fixed cover gives a generically finite dominant rational map

AU⇢Y.A_U \dashrightarrow Y.

In particular dim⁡AU=dim⁡Y=n\dim A_U = \dim Y = n.

Resolve this map as πA:TA→AU\pi_A : T_A \to A_U and g:TA→Yg : T_A \to Y, with TAT_A smooth and projective. Since the canonical bundle of AUA_U is trivial, and since YY is terminal, the canonical comparisons give

KTA∼QEπA,KTA∼Qg∗K+R,EπA,R≥0,(33)K_{T_A} \sim_{\mathbb{Q}} E_{\pi_A},\qquad K_{T_A} \sim_{\mathbb{Q}} g^*K + R,\qquad E_{\pi_A}, R \geq0, \tag*{(33)}

where EπAE_{\pi_A} is exceptional over AUA_U. The images of the exceptional divisors of πA\pi_A have codimension at least two on the smooth abelian variety.

Choose a point in the isomorphism open of πA\pi_A where gg is quasi-finite, outside Supp⁡(R)\operatorname{Supp}(R), and mapping to YvgY^{\mathrm{vg}}. Dominance and the countable-exclusion description ensure that such a point exists. A general sufficiently ample complete-intersection curve in AUA_U through its image avoids all the exceptional centers: they have codimension at least two and do not contain the prescribed point. Its strict transform CC is disjoint from EπAE_{\pi_A} and is not contained in RR. The map gg is nonconstant on CC, since it is quasi-finite at the chosen point. Intersecting (33) with CC gives

0=KTA⋅C=g∗K⋅C+R⋅C>0.0 = K_{T_A}\cdot C = g^*K\cdot C + R\cdot C > 0.

The final strict inequality uses K⋅g(C)≥1/ιK \cdot g(C) \ge1/\iota, the defining curve property of YvgY^{\mathrm{vg}}, multiplied by the positive degree of C→g(C)C \to g(C), together with R⋅C≥0R \cdot C \ge0. This contradiction excludes the remaining correspondence family.

Excluding moving base components

Proof of Proposition 6.3. All constants used to exclude moving centers below are independent of the section degree and of small tt, once ϵ\epsilon, δ\delta, qq have been fixed. We first produce such a center from failure of (29); we then exclude each possible dimension of its fibers over the two factors.

A moving component from failure of the estimate. Suppose that (29) fails at very general torus points. At such a point there is a curve whose ratio is strictly less than 2n+32n+3. This conclusion does not require the infimum defining the Seshadri constant to be attained.

Take d+1d+1 levels

τj=2n+3+jδ,0≤j≤d.\tau_j = 2n+3+j\delta,\qquad0 \le j \le d.

By (6.9), ample Hilbert asymptotics and the dimension of the jet space at a smooth point show that, for large divisible kk, every kernel of jets of order ⌈kτj⌉\lceil k\tau_j\rceil is nonzero. Explicitly, the leading coefficients of the two dimensions are Pd/d!P^d/d! and τjd/d!\tau_j^d/d!. If a section in the lowest kernel does not contain the curve just chosen, its local intersection with that curve at the marked point is at least ⌈kτ0⌉mult⁡zC\lceil k\tau_0\rceil\operatorname{mult}_z C. This exceeds kP⋅CkP\cdot C. Thus every section in that kernel contains the curve, and the lowest base locus has a positive-dimensional component through the mark.

These conditions produce a dominant marked-point family in the sense of Lemma 3.3. For generality, choose the marked point outside the proper rank-jumping and base-dimension loci for all divisible degrees; there are only countably many such conditions. For the degree kk now chosen, restrict to the open where the finitely many jet kernels have constant rank. The dimension of the base scheme at its marked point is upper semicontinuous. The existence of the witnessing curve at very general marks therefore forces the positive-dimensional-base condition on a dominant locus; no family of the witnessing curves is assumed. The finitely many generic base components and their inclusions can then be followed after a finite parameter extension and shrinking.

We may increase the divisible integer kk to arrange, in addition, that all divisors

kL+(2kq−j)S0,0≤j≤kq,kL+(2kq-j)S_0,\qquad0 \le j \le kq,

are Cartier and globally generated. Here is one simultaneous verification. For 1≤a≤n1\le a\le n, subtract aAaA and then KK. The resulting class is

(k r t+(2kq-j)\iota-1)K+(k r t-a)A,

which is ample once krtt>nkr_tt>n and krt≥1kr_t\ge1. Klt Kawamata--Viehweg vanishing followed by regularity with respect to AA proves global generation for every jj in (6.17).

The moving-multiplicity lemma supplies an irreducible parameter space TT, a dominant incidence Γ⊂T×Z\Gamma\subset T\times Z, and integral fiber components V=VuV=V_u of a fixed dimension 1≤f<d1\le f<d. The high-kernel subseries has VV as an isolated base component generically, with ordinary generic order at least

h=⌈kδ/2⌉,k/h≤2/δ.h=\lceil k\delta/2\rceil,\qquad k/h\le 2/\delta.

For a smooth resolution V∗V^*, the base-component estimates and (26) give

0<Pf⋅V≤(2/δ)d−fPd,(34)0 < P^f \cdot V \le(2/\delta)^{d-f}P^d, \tag*{(34)}
KV∗Pf−1≤(ℓ+1rt+2(d−f)δ)Pf⋅V.(35)K_{V^*}P^{f-1} \le\left(\frac{\ell+1}{r_t}+\frac{2(d-f)}{\delta}\right)P^f \cdot V. \tag*{(35)}

The right sides are bounded uniformly in the specified sense.

We first exclude positive-dimensional slot fibers. The chosen incidence point will ensure that all image subvarieties below meet the prescribed very general locus of YY. For an intermediate fiber FF in a slice, let W⊆YW \subseteq Y be its image and write s=dim⁡Fs=\dim F, w=dim⁡Ww=\dim W. The three possibilities are summarized below; the subsequent paragraphs prove all the indicated exclusions.

DimensionsGeometryContradiction
s=w<ns=w<nGenerically finite over a proper imageGeneral type and the degree obstruction on FF.
s=w+1, w<ns=w+1,\ w<nEntire bundle over WWDirect slice-volume bound if w=0w=0; fillers and subadjunction on WW if w>0w>0.
s=w=ns=w=nNon-axis multisection over YYIts two axis intersections give a signed representative; the logarithmic degree obstruction applies.

Table 6.

A full slot fiber is excluded by exchanging slots. This leaves generically finite projections. Proper images are again excluded by general type, and dominant images are excluded by Proposition 6.4.

Restriction to a slot fiber. Consider VV over either factor of Y×YY \times Y. Choose a very general incidence point first. We require that its two base coordinates belong to YvgY^{\mathrm{vg}}, that it lies in the torus, and that the ordinary ideal-power and isolated-component conclusions above hold near it. We also impose the smoothness conditions for the incidence over TT and for VV over the smooth open of its actual slot image. These are available on dense opens.

Now take the slot value of this point, and let FF be the reduced fiber component through it. Write s=dim⁡Fs=\dim F, the general fiber dimension. Suppose first that

0<s<n+1.0 < s < n+1.

The restricted high-kernel subseries on the opposite slice is nonzero and has FF as an isolated base component generically. Indeed, near the selected point the original base support is just VV. No other base component can contain the fiber component through that point. The scheme fiber over the ambient slot agrees with the scheme fiber over the actual image, and smoothness over that image makes it reduced at the selected generic component. Thus the image of Ih\mathcal{I}^{h} in the slice is contained in IFh\mathcal{I}^{h}_{F}, as an ordinary ideal power. A restriction that vanished identically on the whole slice would contradict this local proper base support. Applying Lemma 3.2 in the slice gives

0<Psls⋅F≤(2/δ)n+1−sPsln+1,(36)0 < P_{\mathrm{sl}}^s \cdot F \le(2/\delta)^{n+1-s}P_{\mathrm{sl}}^{n+1}, \tag*{(36)}
KF∗Psls−1≤(ℓ+1rt+2(n+1−s)δ)Psls⋅F.(37)K_{F^*}P_{\mathrm{sl}}^{s-1} \le\left(\frac{\ell+1}{r_t}+\frac{2(n+1-s)}{\delta}\right)P_{\mathrm{sl}}^s \cdot F. \tag*{(37)}

Let W⊆YW \subseteq Y be the image of FF in the other base, and put w=dim⁡Ww=\dim W. It meets the prescribed very general locus. Since the bundle fiber has dimension one, either w=sw=s or w=s−1w=s-1. We treat every possibility.

A generically finite proper image. If w=s<nw=s<n, the resolution of WW is of general type by Proposition 2.2. The same holds for F∗F^*: after resolving the generically finite map to a resolution of WW, ramification adds an effective divisor to the pulled-back canonical divisor. The polarization PslP_{\mathrm{sl}} dominates the pullback of LL. Equations (36) and (37) therefore contradict Lemma 3.4 for sufficiently small tt.

The whole bundle over a proper image. Suppose s=w+1s=w+1, where necessarily w<nw<n. A positive-dimensional closed subset of the generic P1\mathbb{P}^{1} fiber is the entire fiber. Consequently

F=πsl−1(W)F=\pi_{\mathrm{sl}}^{-1}(W)

as reduced integral subvarieties. Nef intersection and the projective-bundle formula give

qLw⋅W≤Pslw+1⋅F(38)qL^{w}\cdot W\le P_{\mathrm{sl}}^{w+1}\cdot F \tag*{(38)}

For w=0w=0, the left side is qq. The right side is at most

(2/δ)nPsln+1≤(2/δ)n2n+2qεn<q(2/\delta)^{n}P_{\mathrm{sl}}^{n+1}\le(2/\delta)^{n}2^{n+2}q\varepsilon^{n}<q

by Equation (6.8), a contradiction.

Assume w>0w>0. We will apply the degree obstruction to WW, rather than to the ruled variety FF. Expand the restricted high sections using the two homogeneous fiber coordinates. Their coefficients of weight jj, for 0≤j≤kq0\le j\le kq, are actual sections of

OY(kL+jS0).\mathcal{O}_{Y}(kL+jS_{0}).

Let a\mathfrak{a} be the ideal generated by all these coefficients in the regular local ring

R=OY,ηW,m=mR.R=\mathcal{O}_{Y,\eta_{W}},\qquad\mathfrak{m}=\mathfrak{m}_{R}.

This ring is regular because the generic point of WW lies in the smooth locus of YY. We need both the order and the support of this coefficient ideal. After choosing frames, the local ring of the slice at the generic point of FF is

R[u]mR[u].R[u]_{\mathfrak{m}R[u]}.

The residue of uu is transcendental over the residue field of RR. If a coefficient had order less than hh, the least m\mathfrak{m}-adic homogeneous part of its polynomial would remain nonzero after adjoining that residue variable. Therefore membership of every high section in mhR[u]mR[u]\mathfrak{m}^{h}R[u]_{\mathfrak{m}R[u]} implies a⊆mh\mathfrak{a}\subseteq\mathfrak{m}^{h}. Moreover, if a prime p⊊m\mathfrak{p}\subsetneq\mathfrak{m} contained a\mathfrak{a}, its extension to this local polynomial ring would be a proper prime strictly below the generic ideal of FF containing the whole high base ideal. This contradicts the isolated support of FF. Hence

a⊆mh,a=m.(39)\mathfrak{a}\subseteq\mathfrak{m}^{h},\qquad\sqrt{\mathfrak{a}}=\mathfrak{m}. \tag*{(39)}

Multiply every weight-jj coefficient by the globally generated space in Equation (6.17). The products all belong to one linear subseries of

H0(Y,OY(2k(L+qS0))).H^{0}\left(Y,\mathcal{O}_{Y}\left(2k(L+qS_{0})\right)\right).

At ηW\eta_{W}, each filler system generates a unit after choosing a frame. Thus this new subseries has precisely the joint ideal a\mathfrak{a}, not merely an ideal with the same support. Its threshold construction in Lemma 3.2 gives an effective rational divisor

Θ∼Qc 2(L+qS0),0<c≤(n−w)k/h,\Theta\sim_{\mathbb{Q}}c\,2(L+qS_{0}),\qquad0<c\le(n-w)k/h,

such that the pair is lc at the generic point of WW and has an lc place centered there. Apply Lemma 3.1 with the testing class LL. Since qS0≤LqS_0 \leq L in nef order, we obtain

KW∗Lw−1≤(K+2c(L+qS0))Lw−1⋅W≤(1rt+8(n−w)δ)Lw⋅W.(40)\begin{aligned} K_{W^*}L^{w-1} \leq(K+2c(L+qS_0))L^{w-1}\cdot W \\ &\leq\left(\frac{1}{r_t}+\frac{8(n-w)}{\delta}\right)L^w\cdot W. \tag*{(40)} \end{aligned}

The top degree Lw⋅WL^w\cdot W is bounded by Equation (6.22) and Equation (6.20). The variety W∗W^* is of general type. Equation (6.24) and the top-degree bound now contradict Lemma 3.4 on W∗W^*.

A non-axis multisection over all of YY. The only remaining intermediate-fiber case is s=w=ns=w=n. Here FF is a multisection of positive degree ee over YY. It is not an axis, since it contains the selected torus point. Let Σ0,Σ∞\Sigma_0,\Sigma_\infty be the axes on the slice, with classes

Σ0∼ξsl,Σ∞∼ξsl−S0.\Sigma_0 \sim\xi_{\mathrm{sl}}, \qquad\Sigma_\infty\sim\xi_{\mathrm{sl}}-S_0.

The intersections with FF are effective integral cycles. Their pushforwards define effective integral Weil divisors D0,D∞D_0,D_\infty on YY, allowing a divisor to be zero. Projection and rational equivalence of cycles give

D0−D∞∼eS0=eιK.(41)D_0-D_\infty\sim eS_0=e\iota K. \tag*{(41)}

This is linear equivalence of Weil divisors: codimension-one rational equivalence on the normal variety YY is precisely linear equivalence. In particular,

J=D0−D∞eι∼QKJ=\frac{D_0-D_\infty}{e\iota}\sim_{\mathbb{Q}} K

is an actual signed rational representative.

For either axis, Psl−qΣP_{\mathrm{sl}}-q\Sigma is nef: it is LL or L+qS0L+qS_0. As F∩ΣF\cap\Sigma is effective and Psl≥π∗LP_{\mathrm{sl}}\geq\pi^*L in nef order,

qLn−1⋅Di≤qPsln−1⋅(F∩Σi)≤Psl⋅F,i=0,∞.(42)qL^{n-1}\cdot D_i\leq qP_{\mathrm{sl}}^{n-1}\cdot(F\cap\Sigma_i)\leq P_{\mathrm{sl}}\cdot F,\qquad i=0,\infty. \tag*{(42)}

Take a log resolution p:Y†→Yp:Y^\dagger\to Y of D0+D∞D_0+D_\infty, and let GG be the reduced snc divisor consisting of their strict supports and all exceptional divisors. By Proposition 5.1, KY†+GK_{Y^\dagger}+G is big. The exceptional terms push to zero against Ln−1L^{n-1}, while the reduced strict support is bounded by the integral divisor D0+D∞D_0+D_\infty. Hence

(KY†+G)Ln−1≤Lnrt+Ln−1⋅(D0+D∞).(43)(K_{Y^\dagger}+G)L^{n-1}\leq\frac{L^n}{r_t}+L^{n-1}\cdot(D_0+D_\infty). \tag*{(43)}

The second term is uniformly bounded by Equation (6.26) and Equation (6.20). Also LnL^n is bounded above and bounded away from zero. Thus Equation (6.27) is the canonical-to-volume bound in the log version of Lemma 3.4, with polarization p∗Lp^*L and map pp. That lemma gives the contradiction in this final intermediate-fiber case.

Reduction to finite correspondences. We have excluded all slot-fiber dimensions 1,…,n1,\ldots,n. A fiber dimension n+1n+1 over one slot image WW would force VV to be the entire bundle over W×YW\times Y. Since V≠ZV\neq Z, one has dim⁡W<n\dim W<n; its fiber over the other slot then has dimension dim⁡W+1\dim W+1, which has just been excluded. It follows that both projections of VV to YY are generically finite onto their images.

If one image were proper, it would have dimension f<nf<n and be of general type. Its generically finite cover V∗V^* would also be of general type, and the total bounds Equations (6.18) to (6.19) would contradict Lemma 3.4. Therefore

f=n,gi:V∗⟶Y(i=1,2)f=n,\qquad g_i:V^*\longrightarrow Y\quad(i=1,2)

are generically finite dominant morphisms. The bounds (34) to (35) supply constants B0B_0, B1B_1 independent of small tt, of the section degree kk, and of the family. We are therefore in the situation excluded by Proposition 6.4.

Every possibility for a moving component has now been excluded. The slice degree obstructions and Proposition 6.4 impose restrictions on tt independent of kk and of the moving family. The assumed failure of (29) is therefore impossible for all sufficiently small tt, as required.

One finite system of jets on a smooth model

We now convert the strict Seshadri bound into a single surjective jet-evaluation map on a smooth model. Choose tt sufficiently small for both Propositions 3.5 and 6.3, and keep it fixed. The next corollary then supplies a point, a Cartier multiple, and finitely many sections whose jets span the required target. These are the finite data used in reduction to positive characteristic; no family of jet systems over varying tt is needed.

Corollary 6.5. Fix sufficiently small tt as in Propositions 3.5 and 6.3, and let p:W→Yp: W \to Y be any fixed smooth projective resolution. Continue to denote pullbacks by LL and S0S_0. On

ZW=P(OW(S0)1⊕OW(S0)2)⟶W×W,M=L1+L2+qξ,Z_W = \mathbb{P}\left(\mathcal{O}_W(S_0)_1 \oplus\mathcal{O}_W(S_0)_2\right) \longrightarrow W \times W,\qquad M = L_1 + L_2 + q\xi,

there are a smooth torus point z∗z_*, over the isomorphism opens of pp in both slots, and a sufficiently divisible integer k0>0k_0 > 0 such that k0Lk_0L is Cartier and

H0(ZW,OZW(k0M))⟶OZW(k0M)⊗(OZW,z∗/mz∗10k0+1)(44)H^0(Z_W,\mathcal{O}_{Z_W}(k_0M)) \longrightarrow\mathcal{O}_{Z_W}(k_0M) \otimes\left(\mathcal{O}_{Z_W,z_*}/\mathfrak{m}_{z_*}^{10k_0+1}\right) \tag*{(44)}

is surjective. In particular, finitely many sections can be fixed whose jets span its target.

Proof. Choose a very general smooth torus point zz of ZZ above the isomorphism open of pp in both slots and satisfying (29), so that ε(P;z)>10\varepsilon(P;z)>10. If b:Z^→Zb:\widehat{Z}\to Z is its blowup and EzE_z is the exceptional divisor, the Seshadri criterion shows that the following rational divisor is ample:

b∗P−10Ez.b^*P - 10E_z.

Indeed one may choose a rational number strictly between 1010 and ε(P;z)\varepsilon(P;z), and then use the usual ample interval below the Seshadri threshold. Choose a>0a>0 so that aPaP and a(b∗P−10Ez)a(b^*P-10E_z) are Cartier. Serre vanishing, applied to the fixed sheaf OZ^(−Ez)\mathcal{O}_{\widehat{Z}}(-E_z), gives

H1(Z^,OZ^(kb∗P−(10k+1)Ez))=0H^1\left(\widehat{Z},\mathcal{O}_{\widehat{Z}}\left(kb^*P-(10k+1)E_z\right)\right)=0

for all sufficiently large multiples kk of aa. The standard local calculation for the blowup of a smooth point identifies the pushforward of OZ^(−(10k+1)Ez)\mathcal{O}_{\widehat{Z}}(-(10k+1)E_z) with mz10k+1\mathfrak{m}_z^{10k+1}, with vanishing higher direct images. The restriction sequence therefore gives surjectivity onto jets through order $10katatz.

The natural morphism ZW→ZZ_W\to Z is an isomorphism near the lift z∗z_* of zz. Pullback preserves the sections in this jet surjection and identifies their jets. Increase the divisible integer kk if necessary so that kLkL is Cartier, and call it k0k_0. Choosing finitely many inverse images of a basis of the finite-dimensional jet target proves the assertion.

Fixed finite data and the final contradiction

The scalar bound and the two-slot jets will now be tested against one independent theorem. We state all its hypotheses before constructing the remaining data. Its independent proof in [38] uses neither abundance nor logarithmic subadditivity.

Theorem 7.1 (Finite-data Frobenius incompatibility). Let WW be a smooth connected projective complex variety of dimension n≥2n \ge2. Fix rational Cartier divisors LL, HH, with HH ample, an integral Cartier divisor SS, an integer q>0q > 0, and real numbers r>1r > 1, ϵ>0\epsilon> 0. Suppose

Hn≤(2ϵ)n,KWHn−1≤2Hn/r,(2L+qS)Hn−1≤4Hn,H^n \le(2\epsilon)^n,\qquad K_W H^{n-1} \le2H^n/r,\qquad(2L+qS)H^{n-1} \le4H^n,
(14ϵ)n<1/4,80ϵ<3/4.(14\epsilon)^n < 1/4,\qquad80\epsilon< 3/4.

The following three kinds of fixed data cannot all exist.

(i) A smooth integral complete-intersection flag ending in a curve CC, of successive divisor classes liHl_iH for positive integers lil_i, with μmin⁡(ΩW1∣C)≥0\mu_{\min}(\Omega^1_W|_C) \ge0.

(ii) On ZW=P(O(S)1⊕O(S)2)→W×WZ_W = \mathbb{P}(\mathcal{O}(S)_1 \oplus\mathcal{O}(S)_2) \to W \times W, in the symmetric-power convention, put M=L1+L2+qξM = L_1 + L_2 + q\xi. For some integer k0>0k_0 > 0 with k0Lk_0L Cartier, finitely many sections of k0Mk_0M surject onto OZW,z∗/mz∗(2n+2)k0+1\mathcal{O}_{Z_W,z_*}/\mathfrak{m}_{z_*}^{(2n+2)k_0+1} after trivialization at a smooth torus point z∗z_*.

(iii) A point x∈Wx \in W, the blowup πx:W^→W\pi_x:\widehat{W} \to W with exceptional divisor JxJ_x, and a curve class γ=f∗(A1⋯An−1)\gamma= f_*(A_1 \cdots A_{n-1}), where f:V→W^f: V \to\widehat{W} is a fixed birational morphism from a smooth integral projective variety and the AiA_i are ample Cartier divisors, such that Jxγ>0J_x\gamma> 0 and

πx∗(L+KW/2+λS)γ≤40ϵJxγ(0≤λ≤q).\pi_x^*(L + K_W/2 + \lambda S)\gamma\le40\epsilon J_x\gamma\qquad(0 \le\lambda\le q).

It suffices to check the two endpoint inequalities.

No nefness of L,S,KWL,S,K_W is assumed, and z∗z_* need not lie over xx. All divisors, the flag, the point, the curve representative, and the finite jet sections are fixed over C\mathbb{C} before the residual characteristic varies.

The proof is [38]. We shall apply it with n=4n = 4, S=S0=ιKS = S_0 = \iota K, and r=rtr = r_t. The remaining work is to obtain its ample perturbation, flag, and actual movable curve witness from the fourfold geometry.

Fixing the polarization, flag, and movable test

Choose a positive rational number ϵ\epsilon sufficiently small that

(14ϵ)n<14,80ϵ<34.(45)(14\epsilon)^n < \frac{1}{4},\qquad80\epsilon< \frac{3}{4}. \tag*{(45)}

Choose qq as in Proposition 6.3, then a sufficiently small rational t>0t > 0 so that both jet estimates hold, rt>qι+1r_t > q\iota+ 1, and Ln<(2ϵ)nL^n < (2\epsilon)^n. Fix tt and rtr_t. Let W→YW \to Y be a projective resolution, and continue to denote pullbacks by KK, AA, LL. Terminality gives

KW=K+E,E≥0 exceptional,S0=ιK Cartier.K_W = K + E,\qquad E \ge0\ \text{exceptional},\qquad S_0 = \iota K\ \text{Cartier}.

Since LL is pulled back from an ample divisor on YY,

KWLn−1=KLn−1≤Ln/rt.K_W L^{n-1} = K L^{n-1} \le L^n/r_t.

Perturb LL by a sufficiently small ample rational class on WW. By continuity, the resulting ample rational divisor HH satisfies

Hn≤(2ϵ)n,KWHn−1≤2Hnrt,(2L+qS0)Hn−1≤4Hn.H^n \le(2\epsilon)^n,\qquad K_W H^{n-1} \le\frac{2H^n}{r_t},\qquad(2L + qS_0)H^{n-1} \le4H^n.

For the last inequality, at H=LH=L use S0Ln−1≤Ln/rtS_0L^{n-1}\leq L^n/r_t and qv<rtq_v<r_t. We now fix HH; all further geometric data will be chosen once over C\mathbb{C} before reduction.

The divisor KWK_W is pseudo-effective. Generic semipositivity, in the smooth empty-boundary case of [6], gives nonnegative Hn−1H^{n-1}-slope to every positive-rank torsion-free quotient of ΩW1\Omega^1_W. Apply the Mehta–Ramanathan restriction theorem to the Harder–Narasimhan filtration and its factors [33]. We obtain a fixed flag of smooth integral general very ample sections, of types

hi=liH(1≤i≤n−1),h_i=l_iH \qquad(1\leq i\leq n-1),

ending in a smooth curve CC, such that

μmin⁡(ΩW1∣C)≥0.(46)\mu_{\min}(\Omega^1_W|_C)\geq0. \tag*{(46)}

The lil_i are sufficiently large divisible integers, chosen successively. The final general curve avoids the codimension-two loci where the filtration factors fail to be locally free. Set Λ=∏i=1n−1li\Lambda=\prod_{i=1}^{n-1}l_i. Then

[C]=ΛHn−1,hi⋅C=liΛHn.[C]=\Lambda H^{n-1},\qquad h_i\cdot C=l_i\Lambda H^n.

Next choose a very general point x∈Wx\in W above the isomorphism locus of W→YW\to Y, and let πx:W^→W\pi_x:\widehat{W}\to W be its blowup, with exceptional divisor JxJ_x. Put

D+=2rt(K+2tA)+2E.D^+=2r_t(K+2tA)+2E.

By Proposition 3.5, every nonzero section of a sufficiently divisible multiple kD+kD^+ satisfies

ord⁡x(s)≤32kϵ.(47)\operatorname{ord}_x(s)\leq32k\epsilon. \tag*{(47)}

Indeed, pushing down removes only the effective exceptional part, and is an isomorphism near xx.

Lemma 7.2. There is a strongly movable curve class γ\gamma on W^\widehat{W}, represented as the pushforward of an ample complete intersection on a fixed smooth projective birational model, such that

(πx∗D+)⋅γ<40ϵJx⋅γ,Jx⋅γ>0.(\pi_x^*D^+)\cdot\gamma<40\epsilon J_x\cdot\gamma,\qquad J_x\cdot\gamma>0.

Proof. If πx∗D+−40ϵJx\pi_x^*D^+-40\epsilon J_x were pseudo-effective, then for any rational cc with 32ϵ<c<40ϵ32\epsilon<c<40\epsilon the divisor πx∗D+−cJx\pi_x^*D^+-cJ_x would be big: it is a positive convex combination of the preceding pseudo-effective divisor and the big divisor πx∗D+\pi_x^*D^+. A sufficiently divisible effective multiple would contradict (47). Thus πx∗D+−40ϵJx\pi_x^*D^+-40\epsilon J_x is not pseudo-effective.

Movable-curve duality [5] gives a strongly movable class with negative pairing against that divisor. Since the inequality is strict, we may take an actual pushforward of an ample complete intersection on one smooth birational projective model, approximating the ample classes rationally and clearing their denominators if needed. The big divisor πx∗D+\pi_x^*D^+ has positive pairing with this nonzero class: write it as an ample class plus an effective class and pull back to the chosen model. The strict inequality therefore implies Jx⋅γ>0J_x\cdot\gamma>0. □\square

We omit πx∗\pi_x^* in subsequent intersection formulas involving γ\gamma. The concrete complete-intersection representative will continue to test effective divisors after reduction.

Endpoint comparison

For 0≤λ≤q0 \le\lambda\le q, put Qλ=L+KW/2+λS0Q_{\lambda}=L+K_{W}/2+\lambda S_{0}. The actual divisor classes on the fixed resolution satisfy

D+−Qλ=(rt−1/2−λι)K+3rttA+32E.(48)D^{+}-Q_{\lambda}=(r_{t}-1/2-\lambda\iota)K+3r_{t}tA+\frac{3}{2}E. \tag*{(48)}

The first coefficient is positive because rt>qι+1r_{t}>q\iota+1. The pullbacks of K,AK,A are nef, and EE is effective. A strongly movable curve pairs nonnegatively with each of these classes. Consequently Lemma 7.2 gives

Qλγ≤D+γ<40εJxγ(0≤λ≤q).Q_{\lambda}\gamma\le D^{+}\gamma< 40\varepsilon J_{x}\gamma\qquad(0 \le\lambda\le q).

This verifies the curve inequalities in Theorem 7.1. It does not require a pseudo-effective cone to specialize to positive characteristic: the curve has the fixed ample complete-intersection representative required by that theorem.

Take z∗z_{*}, k0k_{0}, and the finite sections supplied by Corollary 6.5 on this resolution. For clarity about the finite choices in the comparison, choose also an integral ample divisor T0T_{0} so that each T0+aS0T_{0}+aS_{0}, for 0≤a≤(k0−1)q0 \le a \le(k_{0}-1)q, has fixed sections nonvanishing at the two base coordinates of z∗z_{*}. Serre generation permits these finitely many choices. They supply the residual degrees when the common proof puts Bp=k0⌊p/k0⌋L+T0B_{p}=k_{0}\lfloor p/k_{0}\rfloor L+T_{0}. The differences Bp−pLB_{p}-pL belong to a fixed finite list.

We have now verified all the hypotheses of Theorem 7.1. The choices were made in the order n=4n=4, ε\varepsilon; then the gap δ\delta and integer qq; then tt, rtr_{t}; then the resolution, HH, flag, point, and curve; and finally the finite jets and fillers. Only after these choices does its proof let pp tend to infinity.

The two orders of the determinant

We recall the comparison in the proof of [38], identifying the determinant bundles to which our movable test applies. Spread the fixed data as in that proof and work on a smooth reduction in sufficiently large characteristic pp. The same notation denotes the reduced divisors and witnesses. For relative Frobenius F:W→W′F:W \to W', let S0′S'_{0} be the base-field twist of S0S_{0} and put

E=F∗OW(Bp),s=rk⁡E=pn,R=s2=p8,Ua=H0(W,OW(Bp+paS0)).\mathcal{E}=F_{*}\mathcal{O}_{W}(B_{p}), \qquad s=\operatorname{rk}\mathcal{E}=p^{n}, \qquad R=s^{2}=p^{8}, \qquad U_{a}=H^{0}(W,\mathcal{O}_{W}(B_{p}+paS_{0})).

The projection formula gives an evaluation map

Φp:⨁a+b=qa,b≥0Ua⊗Ub⊗OW′×W′(−aS0,1′−bS0,2′)⟶E⊠E.(49)\Phi_{p}:\bigoplus_{\substack{a+b=q\\a,b\ge0}}U_{a}\otimes U_{b}\otimes\mathcal{O}_{W'\times W'}(-aS'_{0,1}-bS'_{0,2})\longrightarrow\mathcal{E}\boxtimes\mathcal{E}. \tag*{(49)}

Products of the fixed jet sections, multiplied by the fixed fillers, generate the local quotient by the pp-th powers of the parameters at z∗z_{*}. Let A∗A_{*} be the tensor product of the two base Frobenius-fiber algebras. If the torus coordinate zz has value z0≠0z_{0}\ne0 at z∗z_{*}, this quotient is A∗[z]/(zp−z0p)A_{*}[z]/(z^{p}-z_{0}^{p}). Project to the coefficient of 11 in its A∗A_{*}-basis 1,z,…,zp−11,z,\ldots,z^{p-1}. Exactly the weights divisible by pp survive, showing that the values of (7.8) span A∗A_{*}. Its dimension is RR, so Φp\Phi_{p} has generic rank RR.

On the diagonal, the columns instead restrict to global sections of one line bundle on the Frobenius fiber product:

ΔF=W×W′W,Lp=OΔF(Bp,1+Bp,2+pqS0,1).\Delta_{F}=W\times_{W'}W,\qquad\mathcal{L}_{p}=\mathcal{O}_{\Delta_{F}}(B_{p,1}+B_{p,2}+pqS_{0,1}).

Here pS0,1pS_{0,1} and pS0,2pS_{0,2} are isomorphic line bundles on ΔF\Delta_F, so all the weight pairs a+b=qa+b=q give this same bundle. The rank at every diagonal point is at most h0(ΔF,Lp)h^0(\Delta_F,\mathcal{L}_p). The diagonal-ideal filtration has graded bundles

Gj=OW(2Bp+pqS0)⊗Aj(ΩW1),0≤j≤n(p−1),\mathcal{G}_j=\mathcal{O}_W(2B_p+pqS_0)\otimes A_j(\Omega_W^1),\qquad0\leq j\leq n(p-1),

where AjA_j is the degree-jj part of the symmetric algebra modulo the pp-th powers of its local generators. If ej=rk⁡Aje_j=\operatorname{rk} A_j, then ∑jej=pn\sum_j e_j=p^n. The slope estimate and our one fixed flag give the common bound proved in the companion:

h0(W,Gj)≤ejpn(7nHn+O(p−1)).h^0(W,\mathcal{G}_j)\leq e_jp^n(7^nH^n+O(p^{-1})).

The error is independent of jj. Summing therefore bounds every diagonal rank by R(7nHn+O(p−1))<R/4R(7^nH^n+O(p^{-1}))<R/4, since 7nHn≤(14ϵ)n<1/47^nH^n\leq(14\epsilon)^n<1/4.

Choose RR generically independent columns of Φp\Phi_p, and let mim_i be the sum of their weights in slot ii. Their nonzero determinant is a section

0≠σ∈H0(W′×W′,Q1⊠Q2),Qi=(det⁡E)⊗s⊗OW′(miS0′).0\ne\sigma\in H^0(W'\times W',\mathcal{Q}_1\boxtimes\mathcal{Q}_2),\qquad\mathcal{Q}_i=(\det\mathcal{E})^{\otimes s}\otimes\mathcal{O}_{W'}(m_iS'_0).

These are actual line bundles. Under the numerical identification with the base-field twist, their first Chern classes satisfy

c1(Qi)R=Bpp+p−12pKW+λiS0=Qλi+Bp−pL−KW/2p,λi=miR∈[0,q].(50)\frac{c_1(\mathcal{Q}_i)}{R}=\frac{B_p}{p}+\frac{p-1}{2p}K_W+\lambda_iS_0=Q_{\lambda_i}+\frac{B_p-pL-K_W/2}{p},\qquad\lambda_i=\frac{m_i}{R}\in[0,q]. \tag*{(50)}

The numerator of the last term belongs to a fixed finite list. Thus the endpoint comparison bounds the intersection of each normalized class with γ\gamma by (40ϵ+O(p−1))Jxγ(40\epsilon+O(p^{-1}))J_x\gamma, uniformly in the chosen columns.

This intersection bound controls sections on the reduction itself. Put x′=F(x)x'=F(x). For any nonzero section of Qi\mathcal{Q}_i, the strict transform of its zero divisor on the blowup at x′x' is effective and pairs nonnegatively with the twist of γ\gamma; that curve is still the pushforward of the fixed ample complete intersection. Since Jxγ>0J_x\gamma>0, every such section has order at x′x' at most R(40ϵ+O(p−1))R(40\epsilon+O(p^{-1})). Bases adapted to vanishing order in the two factors show that a nonzero section of their external product has order at most the sum of these bounds. Within each bidegree the leading tensors are linearly independent, and different bidegrees cannot cancel. Consequently

ord⁡(x′,x′)σ≤R(80ϵ+O(p−1)).\operatorname{ord}_{(x',x')}\sigma\leq R(80\epsilon+O(p^{-1})).

But the rank of Φp\Phi_p at (x′,x′)(x',x') is less than R/4R/4. Constant row operations make more than 3R/43R/4 rows of the selected matrix vanish at that point, forcing ord⁡(x′,x′)σ≥3R/4\operatorname{ord}_{(x',x')}\sigma\geq3R/4. The two orders contradict 80ϵ<3/480\epsilon<3/4 for large pp. The generic-rank calculation used z∗z_*, whereas this diagonal comparison uses the independently chosen point xx.

Thus the terminal counterexample in Proposition 2.1 cannot exist. Canonical section spaces are preserved by its birational construction, so this proves Theorem 1.1.

A section on the original normal variety

The geometric argument produces a pluricanonical section on a smooth fourfold. Hashizume’s reduction gives an effective real representative of an lc adjoint on the original variety. The following elementary lemma turns that representative into a rational one. It concerns finite linear algebra and uses no nonvanishing or abundance theorem.

Lemma 8.1 (Finite rational feasibility). Let M=(mij)∈Mat⁡w×v(Q)M=(m_{ij})\in\operatorname{Mat}_{w\times v}(\mathbb{Q}) and d∈Qwd\in\mathbb{Q}^{w}. If the system

di−yi=∑j=1vmijbj(1≤i≤w),yi≥0d_i-y_i=\sum_{j=1}^{v}m_{ij}b_j\quad(1\le i\le w),\qquad y_i\ge0

has a real solution, it has a rational solution. Moreover, one may require precisely the same yiy_i to be zero as in the given solution. Consequently, if DD is a rational Weil divisor on a normal integral variety XX over a field kk and D∼RGD\sim_{\mathbb{R}}G for an effective real Weil divisor GG, then D∼QGQD\sim_{\mathbb{Q}}G_{\mathbb{Q}} for an effective rational divisor with Supp⁡GQ=Supp⁡G\operatorname{Supp}G_{\mathbb{Q}}=\operatorname{Supp}G. If rDrD is Cartier for a prescribed positive integer rr, then H0(X,OX(mrD))≠0H^{0}(X,\mathcal{O}_{X}(mrD))\ne0 for some m>0m>0.

Proof. Fix the equations yi=0y_i=0 at all coordinates vanishing in the given real solution. Together with the displayed equations they define a nonempty affine space over Q\mathbb{Q}. Gaussian elimination over Q\mathbb{Q} gives a rational particular solution and a basis over Q\mathbb{Q} for its direction space. Thus its rational points are dense in its real points. Approximate the given point closely enough to keep all of the finitely many remaining coordinates yiy_i strictly positive. This proves the first assertion, including the case where all yiy_i vanish or the affine space has dimension zero.

For the divisor assertion, choose a finite expression

D−G=∑j=1vajDiv⁡(fj),aj∈R,fj∈k(X)∗.D-G=\sum_{j=1}^{v}a_j\operatorname{Div}(f_j),\qquad a_j\in\mathbb{R},\quad f_j\in k(X)^{*}.

List the prime divisors in the supports of DD, GG, and these finitely many principal divisors as P1,…,PwP_1,\ldots,P_w. Write D=∑diPiD=\sum d_iP_i and let mij∈Zm_{ij}\in\mathbb{Z} be the coefficient of PiP_i in Div⁡(fj)\operatorname{Div}(f_j). The coefficients of GG and the aja_j give a real solution of (8.1). A rational solution gives GQ=∑yiPi≥0G_{\mathbb{Q}}=\sum y_iP_i\ge0 with the same support and D−GQ=∑bjDiv⁡(fj)D-G_{\mathbb{Q}}=\sum b_j\operatorname{Div}(f_j).

Choose a positive integer NN divisible by rr and by the denominators of all yi,bjy_i,b_j. Then

ND−NGQ=Div⁡(∏jfjNbj).ND-NG_{\mathbb{Q}}=\operatorname{Div}\left(\prod_j f_j^{Nb_j}\right).

The effective integral divisor NGQNG_{\mathbb{Q}} is Cartier, since NDND is Cartier and their difference is principal. It defines a nonzero section of OX(ND)\mathcal{O}_{X}(ND). Write N=mrN=mr. No Q\mathbb{Q}-factoriality is needed: all equalities were equalities of Weil divisors on XX.

Proof of Corollary 1.2. Hashizume’s reduction [20], Theorem 1.4 takes smooth canonical nonvanishing in dimension four, supplied by Theorem 1.1, and gives nonvanishing for projective lc pairs with effective real boundaries and pseudo-effective real Cartier adjoints in dimensions at most four. Applied to the given rational lc pair, it produces D∼RG≥0D\sim_{\mathbb{R}}G\ge0 on the original normal variety; nefness implies pseudo-effectivity. Lemma 8.1 gives a nonzero section of mrDmrD for some positive integer mm, with the prescribed index rr.

References

  1. [1]Florin Ambro. The moduli b-divisor of an lc-trivial fibration. Compositio Mathematica, 141(2):385–403, 2005. Theorem 4.3, pp. 397–398.
  2. [2]Thomas Bauer, Frédéric Campana, Thomas Eckl, Stefan Kebekus, Thomas Peternell, Sławomir Rams, Tomasz Szemberg, and Lorenz Wotzlaw. A reduction map for nef line bundles. In Complex Geometry: Collection of Papers Dedicated to Hans Grauert, pages 27–36. Springer, Berlin, 2002. Theorem 2.1.
  3. [3]Caucher Birkar, Paolo Cascini, Christopher D. Hacon, and James McKernan. Existence of minimal models for varieties of log general type. Journal of the American Mathematical Society, 23(2):405–468, 2010.arxiv.org/abs/math/0610203
  4. [4]Jérémy Blanc. Algebraic structures of groups of birational transformations. In Algebraic Groups: Structure and Actions, volume 94 of Proceedings of Symposia in Pure Mathematics, pages 17–30. American Mathematical Society, 2017. Proposition 3.7 and Theorem 3.8, pp. 25–26.
  5. [5]Sébastien Boucksom, Jean-Pierre Demailly, Mihai Păun, and Thomas Peternell. The pseudo-effective cone of a compact Kähler manifold and varieties of negative Kodaira dimension. Journal of Algebraic Geometry, 22(2):201–248, 2013. Theorem numbering refers to arXiv:math/0405285v1.
  6. [6]Frédéric Campana and Mihai Păun. Orbifold generic semi-positivity: an application to families of canonically polarized manifolds. Annales de l’Institut Fourier, 65(2):835–861, 2015.
  7. [7]Guodu Chen and Nikolaos Tsakanikas. On the termination of flips for log canonical generalized pairs. Acta Mathematica Sinica, English Series, 39(6):967–994, 2023. Theorem 1.1 in arXiv:2011.02236v2.DOI
  8. [8]J.-P. Demailly, T. Peternell, and M. Schneider, Compact complex manifolds with numerically effective tangent bundles, J. Algebraic Geom. 3 (1994), 295–345. Author manuscript.
  9. [9]Lawrence Ein, Oliver Küchle, and Robert Lazarsfeld. Local positivity of ample line bundles. Journal of Differential Geometry 42 (1995), no. 2, 193–219. doi:10.4310/jdg/1214457231.DOI
  10. [10]Osamu Fujino. Abundance theorem for semi log canonical threefolds. Duke Mathematical Journal, 102(3):513–532, 2000.DOI
  11. [11]Osamu Fujino. Finite generation of the log canonical ring in dimension four. Kyoto Journal of Mathematics, 50(4):671–684, 2010.DOI
  12. [12]Osamu Fujino. Fundamental theorems for the log minimal model program. Publications of the Research Institute for Mathematical Sciences, 47(3):727–789, 2011.arxiv.org/abs/0909.4445
  13. [13]Osamu Fujino and Yoshinori Gongyo. Log pluricanonical representations and the abundance conjecture. Compositio Mathematica, 150(4):593–620, 2014. Remark 2.7.DOI
  14. [14]Osamu Fujino and Kenta Hashizume. Existence of log canonical modifications and its applications. European Journal of Mathematics, 9(1), 2023. Article 13; Theorem 2.10 in the revised author manuscript dated 28 April 2022.arxiv.org/abs/2103.01417
  15. [15]O. Fujino, A transcendental approach to Kollár’s injectivity theorem, Osaka J. Math. 49 (2012), no. 3, 833–852. Locators refer to the author manuscript dated 30 April 2011, version 1.25, Lemma 3.1 and Section 3.
  16. [16]Osamu Fujino and Yoshinori Gongyo. On canonical bundle formulae and subadjunctions. Michigan Mathematical Journal 61(2) (2012), 255–264. Theorem 4.1 and Remark 4.2 in the author manuscript, version 1.17, September 12, 2010.
  17. [17]Yoshinori Gongyo and Shin-ichi Matsumura. Versions of injectivity and extension theorems. Annales scientifiques de l’École Normale Supérieure, 50(2):479–502, 2017. Corollary 5.3 is cited from arXiv:1406.6132v2, p. 19.arxiv.org/abs/1406.6132
  18. [18]Christopher D. Hacon, James McKernan, and Chen-yang Xu. Boundedness of varieties of log general type. In Algebraic Geometry: Salt Lake City 2015, Part 1, volume 97.1 of Proceedings of Symposia in Pure Mathematics, pages 309–348. American Mathematical Society, 2018. Theorem 4.0.1, p. 335, in the published version.
  19. [19]Masaki Hanamura. Structure of birational automorphism groups, I: non-uniruled varieties. Inventiones Mathematicae, 93:383–403, 1988. Theorem 2.1; see also Blanc, Theorem 3.8.DOI
  20. [20]Kenta Hashizume. On the non-vanishing conjecture and existence of log minimal models. Publications of the Research Institute for Mathematical Sciences, 54(1):89–104, 2018. Theorem 1.4, p. 90.
  21. [22]Y. Kawamata, Pluricanonical systems on minimal algebraic varieties, Invent. Math. 79 (1985), 567–588. doi:10.1007/BF01388524.DOI
  22. [23]Yujiro Kawamata. Abundance theorem for minimal threefolds. Inventiones Mathematicae, 108:229–246, 1992.DOI
  23. [24]Yujiro Kawamata. Subadjunction of log canonical divisors, II. American Journal of Mathematics 120(5) (1998), 893–899. Theorem 1 in arXiv:alg-geom/9712014v1.DOI
  24. [25]Sean Keel, Kenji Matsuki, and James McKernan. Log abundance theorem for threefolds. Duke Mathematical Journal, 75(1):99–119, 1994.DOI
  25. [26]Sean Keel, Kenji Matsuki, and James McKernan. Corrections to: “log abundance theorem for threefolds”. Duke Mathematical Journal, 122(3):625–630, 2004.DOI
  26. [29]Robert Lazarsfeld. Positivity in Algebraic Geometry I: Classical Setting: Line Bundles and Linear Series, volume 48 of Ergebnisse der Mathematik und ihrer Grenzgebiete, 3. Folge. Springer, Berlin, 2004.
  27. [30]Vladimir Lazić and Thomas Peternell. Abundance for varieties with many differential forms. Épijournal de Géométrie Algébrique 2 (2018), 1–35. doi:10.46298/epiga.2018.volume2.3867. Article 1, 35 pp.DOI
  28. [31]Jihao Liu and Zheng Xu. Non-vanishing implies numerical dimension one abundance. Preprint, arXiv:2505.05250v2, 2025.arxiv.org/abs/2505.05250
  29. [32]Shin-ichi Matsumura. An injectivity theorem with multiplier ideal sheaves of singular metrics with transcendental singularities. Journal of Algebraic Geometry, 27(2):305–337, 2018. The section and theorem locators used here refer to arXiv:1308.2033v4, revised 27 April 2016.
  30. [33]V. B. Mehta and A. Ramanathan. Semistable sheaves on projective varieties and their restriction to curves. Mathematische Annalen, 258:213–224, 1982.DOI
  31. [34]Yoichi Miyaoka. On the Kodaira dimension of minimal threefolds. Mathematische Annalen, 281(2):325–332, 1988. doi:10.1007/BF01458437.DOI
  32. [35]Yoichi Miyaoka. Abundance conjecture for 3-folds: case ν = 1. Compositio Mathematica, 68(2):203–220, 1988. Published article.
  33. [37]OpenAI, Minimal metrics and interior injectivity for nef adjoints, OpenAI Math Release preprint OAI:Minimal-metrics-and-interior-injectivity-for-nef-adjoints-September-27-2026, 2026.
  34. [38]OpenAI, Log abundance in characteristic zero, OpenAI Math Release preprint OAI:Log-abundance-in-characteristic-zero-September-24-2026, 2026.
  35. [39]OpenAI, Lifting sections from the reduced support of an adjoint, OpenAI Math Release preprint OAI:Lifting-sections-from-the-reduced-support-of-an-adjoint-September-27-2026, 2026.

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