Introduction

A nef divisor has nonnegative degree on every curve. A semiample divisor has a positive Cartier multiple generated by global sections, and therefore defines a morphism to a projective variety. The passage from numerical positivity to such a morphism is central to the minimal model program. For an ordinary log canonical divisor, this is the abundance problem. Adding an arbitrary nef divisor changes the natural conclusion: one must allow replacement by a numerically equivalent divisor.

We call a rational Cartier divisor numerically semiample if it is numerically equivalent to a semiample rational Cartier divisor on the same variety. Here numerical equivalence means equality of degrees on all integral curves. We prove the following statement.

Theorem 1.1. Let (X,B)(X, B) be a projective klt Q\mathbb{Q}-pair over an algebraically closed field of characteristic zero. Suppose that KX+BK_X + B is pseudo-effective, and let MM be a nef Q\mathbb{Q}-Cartier divisor on XX. If

D=KX+B+MD = K_X + B + M

is nef, then there is a semiample Q\mathbb{Q}-Cartier divisor LL on XX such that D≡LD \equiv L.

The rationality assumptions apply to the boundary and the nef summand; in particular the latter is a divisor on XX itself. The proof uses the log-abundance theorem of [28] and the terminating minimal-model programs of [29]. Their precise forms are stated in Section 2.

Date: October 3, 2026.

2020 Mathematics Subject Classification. Primary 14E30; Secondary 14C20, 14J32.

Key words and phrases. generalised abundance, numerical semiampleness, nef divisor, minimal model, Frobenius morphism.

Theorem 1.1 contains the Generalised Abundance Conjecture formulated by Lazić–Peternell [22], where the nef summand is Cartier. Numerical equivalence is necessary even in dimension one. Indeed, a nontorsion degree-zero line bundle on a complex elliptic curve is nef and numerically trivial, but none of its positive powers has a nonzero section. Since the canonical bundle of the curve is trivial, this is an example with B=0B = 0 in Theorem 1.1. For the ordinary adjoint, Fukuda’s theorem [15], Theorem 0.1 shows that a semiample numerical representative makes KX+BK_X + B itself semiample. For M=0M = 0, the conclusion is therefore equivalent to ordinary klt abundance, which is an input to this proof.

Corollary 1.2. Let (X,B)(X,B) be a projective klt Q\mathbb{Q}-pair in characteristic zero with KX+B≡0K_X+B \equiv0. Every nef Q\mathbb{Q}-Cartier divisor on XX is numerically semiample.

Proof. For a nef divisor MM, the divisor KX+B+MK_X+B+M is nef and numerically equivalent to MM. Apply Theorem 1.1. □

Background and the role of the present argument

The generalized-pair formalism retains a nef divisor on a higher birational model as part of the adjoint data. Birkar–Zhang [4] developed effective birationality for these polarized pairs, extending the tools used to study Iitaka fibrations. The canonical bundle formula of Ambro [1] is one source of such nef data. In this paper the original nef summand descends to XX, but a minimal-model program forces us to keep track of it as a fixed nef divisor on a higher model.

Lazić–Peternell [22] formulated generalized abundance as a numerical extension of abundance and related it to semi ampleness on varieties with trivial canonical class. Their Theorem B, assuming termination of flips and abundance in dimensions at most nn, proves numerical semiampleness when the ordinary adjoint has positive numerical dimension. Its numerical-dimension-zero case also assumes their Semiampleness Conjecture. Their Corollaries C and D give unconditional results for surfaces and for threefolds with ordinary adjoint of positive numerical dimension. These results identify the main remaining positivity issue: an arbitrary nef summand on a variety with trivial canonical class need not supply sections directly.

Subsequent work has addressed numerical nonvanishing, which asks for an effective numerical representative, and refinements of numerical semiampleness. Lazić–Peternell [23], Theorems B and C obtained numerical nonvanishing under additional numerical or metric hypotheses and, in the metric case, conjectural MMP and abundance assumptions. For a Cartier nef summand, Chaudhuri [8], Corollary 3 proved generalized abundance when the nef-reduction base of DD has dimension two and KX+BK_X+B is effective, or when that base has dimension three and κ(KX+B)>0\kappa(K_X+B)>0. Here nef reduction contracts the curves of degree zero through very general points; its precise properties are recalled in Section 2. On surfaces, Fontanari [10], Theorem 1.4 proved actual semiampleness when the nef summand is Cartier and its numerical class is not proportional to that of the ordinary adjoint.

The birational reductions below follow [22], Sections 4–7. The companion results [28, 29] supply ordinary log abundance and the existence of the particular terminating programs required in those reductions. The further ingredient proved here is that a nef divisor of full nef dimension on a klt Calabi–Yau pair is big. Full nef dimension means that every curve through a very general point has positive degree. Bigness is stronger: it requires the volume of the divisor to be positive. The gap between these two conditions is the geometric issue addressed by the proof.

Our treatment adapts the moving-jet and Frobenius arguments of [28], Sections 7–9. The moving-point method has antecedents in the local-positivity work of Ein–Küchle–Lazarsfeld [9]. The finite-data comparison uses Frobenius jets, as studied by Mustaţă–Schwede [26], the canonical filtrations of Sun and Kitadai–Sumihiro [30, 18], and Langer’s control of Frobenius slopes [20]. We reproduce the comparison proof with its uniformity conditions.

The adaptation to an arbitrary nef summand occurs in the geometric exclusions preceding it: the polarized birationality theorem of Birkar–Zhang gives curves of bounded degree, contradicting a growing integral lower bound for their degrees. We give explicit proofs of those exclusions, including the case of correspondences between finite covers.

1.2. Structure of the proof. There are two simultaneous induction statements. The first says that KX+B+cMK_X+B+cM is big for every rational c>0c>0 whenever one positive combination of KX+BK_X+B and MM has positive degree on all curves through a very general point. The second says that the positive part of KX+B+MK_X+B+M on a suitable smooth birational model is rational and numerically semiample. The positive part is the divisor left after removing the asymptotically fixed prime divisors. When the original adjoint is nef, it has no such negative part, and the second assertion descends to Theorem 1.1.

Section 3 sets up this induction. A pair of compatible minimal-model programs retains both a semiample ordinary adjoint and a nearby nef generalized adjoint. Positive Iitaka dimension then permits induction on the fibres. The remaining full-dimension case is a klt Calabi–Yau pair.

Sections 4 and 5 treat the essential terminal case with trivial canonical bundle. If a nef Cartier divisor LL of full nef dimension were not big, its ample approximations could be rescaled to bounded volume while their degrees on very general curves tend to infinity. The bounded-degree obstruction controls the base loci of moving jet kernels. It produces a small vanishing-order bound on the variety itself and a large jet system on a projective bundle over its square. Section 6 shows that these two conclusions are incompatible. The comparison is made on fixed complex data before reduction to positive characteristic.

Section 7 passes through an index-one cover and a boundary perturbation to obtain the full-dimension assertion for all klt Calabi–Yau pairs. Section 8 proves the positive-part assertion by nef reduction and the canonical bundle formula, then descends numerical semiampleness to the original variety and to any algebraically closed field of characteristic zero.

Conventions and birational inputs

Varieties are integral and projective over an algebraically closed field of characteristic zero unless stated otherwise. A Q\mathbb{Q}-pair (X,B)(X,B) consists of a normal variety, an effective rational boundary BB, and a rational Cartier divisor KX+BK_X+B. We use log discrepancies: on a resolution h:Y→Xh:Y\to X, the equality KY+BY=h∗(KX+B)K_Y+B_Y=h^*(K_X+B) assigns log discrepancy 1−bE1-b_E to a prime divisor with coefficient bEb_E in BYB_Y. The pair is klt if all log discrepancies are positive, and log canonical if they are nonnegative. We use the standard cone, contraction, negativity, and resolution theorems as in [19, 3].

The symbols ∼Q\sim_{\mathbb{Q}} and ≡\equiv denote rational linear and numerical equivalence. A divisor is pseudo-effective if its numerical class is in the closure of the cone generated by effective divisors, and big if its class lies in the interior of that cone. Its Iitaka dimension is denoted by κ\kappa. Over C\mathbb{C}, a very general point means a point outside a specified countable union of proper closed subsets.

For a nef divisor NN, its nef reduction is an almost holomorphic dominant rational map with connected compact general fibres, on which NN is numerically trivial, such that every curve through a very general point not contracted by the map has positive NN-degree [2]. Its base dimension is the nef dimension n(X,N)n(X,N). Thus n(X,N)=dim⁡Xn(X,N)=\dim X precisely when every curve through a very general point has positive NN-degree. This numerical condition does not assert bigness.

For a pseudo-effective real divisor DD on a smooth variety and a prime divisor Γ\Gamma, fix an ample divisor AA and set

σΓ(D)=lim⁡δ↓0inf⁡{mult⁡ΓD′:D′≥0, D′∼RD+δA}.\sigma_{\Gamma}(D)=\lim_{\delta\downarrow0}\inf\{\operatorname{mult}_{\Gamma}D' : D'\geq0,\ D'\sim_{\mathbb{R}}D+\delta A\}.

These numbers are independent of AA and depend only on the numerical class of DD. The divisorial Zariski decomposition is

Nσ(D)=∑ΓσΓ(D)Γ,Pσ(D)=D−Nσ(D).N_{\sigma}(D) = \sum_{\Gamma} \sigma_{\Gamma}(D)\Gamma,\qquad P_{\sigma}(D) = D - N_{\sigma}(D).

The sum has finite support. A nef divisor has Nσ(D)=0N_{\sigma}(D) = 0. Further properties from [27, 22] are recorded at their point of use in Section 8.

Lemma 2.1. Let DD be a pseudo-effective rational Cartier divisor on a projective complex variety XX. Every integral curve through a sufficiently very general point has nonnegative DD-degree.

Proof. Fix an ample Cartier divisor AA and positive rational numbers δi→0\delta_i \to0. Each D+δiAD + \delta_i A is big, so there is an effective rational divisor Ei∼QD+δiAE_i \sim_{\mathbb{Q}} D + \delta_i A. Choose a point outside ⋃iSupp⁡Ei\bigcup_i \operatorname{Supp} E_i. A curve through it is contained in none of these supports; hence (D+δiA)⋅C≥0(D + \delta_i A) \cdot C \ge0 for every ii. Let i→∞i \to\infty. □\square

We state explicitly the companion results used throughout. We require existence of a terminating choice of program, rather than termination of every sequence of flips.

Theorem 2.2 (Log abundance, [28], Theorem 1.1). Let (X,B)(X, B) be a projective log canonical Q\mathbb{Q}-pair over an algebraically closed field of characteristic zero. If KX+BK_X + B is nef, then it is semiample.

For the next input a nef rational Cartier b-divisor is specified by a nef rational Cartier divisor on a projective birational model; it is pulled back unchanged on all higher models. Its trace on a lower model is its pushforward and need not be nef. Generalized discrepancies are defined by pulling back the adjoint while keeping this fixed nef data.

Theorem 2.3 (Minimal-model programs, [29], Theorem 1.1 and Section 3.3). Let (X,B+M)(X, B + M) be a projective generalized klt Q\mathbb{Q}-pair over C\mathbb{C}, with XX Q\mathbb{Q}-factorial and with fixed nef rational Cartier b-divisor data. If KX+B+MXK_X + B + M_X is pseudo-effective, there is a terminating choice of its minimal-model program, with Q\mathbb{Q}-factorial generalized klt models and a nef endpoint. The program extracts no divisors and generalized log discrepancies do not decrease. On a common resolution of its initial and final models, the pullback of the initial adjoint is the pullback of the final adjoint plus an effective divisor exceptional over the final model.

The ordinary klt case follows by taking the nef data to be zero. In that case Theorem 2.2 makes the endpoint a good minimal model. The moving-center and Frobenius results used from [28] are stated separately in Sections 4 and 6; neither theorem above asserts abundance for a nonzero generalized nef summand.

Reduction of full nef dimension to Calabi–Yau pairs

We work over C\mathbb{C} until the final descent argument. The reductions in this section follow the strategy of Lazic–Peternell [22], Sections 4 and 5. We use the terminating programs in Theorem 2.3, together with the abundance input Theorem 2.2, to make the precise reductions needed below. The essential point is to retain control of two adjoints: an ordinary semiample adjoint and a nearby generalized nef adjoint.

The induction statements

For a projective klt Q\mathbb{Q}-pair (X,B)(X, B) and a nef Q\mathbb{Q}-Cartier divisor MM on XX, write

T=KX+B.T = K_X + B.

Suppose that TT is pseudo-effective. We will use the condition that, for some a∈Q>0a \in\mathbb{Q}_{>0},

(T+aM)⋅C>0for every integral curve C through a very general point of X.(1)(T + aM) \cdot C > 0 \quad\text{for every integral curve } C \text{ through a very general point of } X. \tag*{(1)}

The divisor T+aMT+aM need not be nef. By Lemma [2], Condition (1) holds whenever MM has full nef dimension. When T+aMT+aM is nef, the condition says exactly that its nef dimension is dim⁡X\dim X.

We prove the following two assertions together, by induction on nn. The notation PσP_{\sigma} denotes the positive part of the divisorial Zariski decomposition; its properties used in the proof are recalled in Section 8.

(PnP_n): If (X,B)(X,B) is a projective klt Q\mathbb{Q}-pair of dimension nn, T=KX+BT=K_X+B is pseudo-effective, MM is a nef Q\mathbb{Q}-Cartier divisor on XX, and (1) holds, then T+cMT+cM is big for every c∈Q>0c\in\mathbb{Q}_{>0}.

(ZnZ_n): If (X,B)(X,B) and MM have the same hypotheses, without (1), then there is a projective birational morphism w ⁣:W→Xw\colon W\to X from a smooth projective variety such that

Pσ(w∗(T+M))P_{\sigma}\left(w^*(T+M)\right)

is a rational divisor numerically equivalent to a semiample Q\mathbb{Q}-divisor on WW.

Both assertions hold in dimensions zero and one. In dimension one, pseudo-effectivity of TT and nefness of MM mean that their degrees are nonnegative. Condition (1) makes every positive combination have positive degree, hence be ample. A divisor of degree zero is numerically equivalent to zero, and a divisor of positive degree is ample. These observations also give (Z1)(Z_1), since a nef divisor has zero negative part. On a point the assertions use the usual conventions.

Fix n≥2n\geq2, and assume (Pj)(P_j) and (Zj)(Z_j) for j<nj<n. At any stage we may replace XX by a small projective Q\mathbb{Q}-factorialization. The ordinary adjoint pulls back crepantly, MM pulls back to a nef divisor, and (1) persists by using points in the isomorphism locus. Bigness descends under this birational pullback. A smooth model proving (Zn)(Z_n) for the Q\mathbb{Q}-factorialization also proves it for XX. We therefore impose Q\mathbb{Q}-factoriality when running the programs below.

Keeping a semiample adjoint fixed

We first record the elementary ray comparison used in the second program. The nef part of a generalized pair in this argument is the fixed nef Q\mathbb{Q}-Cartier b-divisor determined by MM on the original variety. Its trace on a later model need not be nef.

Lemma 3.1. Let (V,Δ+N)(V,\Delta+N) be a projective generalized klt Q\mathbb{Q}-pair of dimension nn, with effective boundary, Q\mathbb{Q}-factorial VV, and nef rational Cartier b-divisor data. Every (KV+Δ+NV)(K_V+\Delta+N_V)-negative extremal ray has an integral rational curve generator CC for which

−4n≤(KV+Δ+NV)⋅C<0.-4n\leq(K_V+\Delta+N_V)\cdot C<0.

The contraction, and the flip when it is small, can be realized using an ordinary klt adjoint negative on the same ray. Birational MMP outputs remain Q\mathbb{Q}-factorial. On a common resolution of a birational step, the pullback of the input generalized adjoint equals the pullback of its output transform plus an effective divisor exceptional over the output.

Proof. Set G=KV+Δ+NVG=K_V+\Delta+N_V, and fix a GG-negative extremal ray. For an ample rational divisor AA on VV, choose η>0\eta>0 rational and small enough that G+ηAG+\eta A is still negative on the ray and

−(G+ηA)⋅γ≥−12G⋅γ-(G+\eta A)\cdot\gamma\geq-\frac{1}{2}G\cdot\gamma

for its nonzero classes γ\gamma. We may represent G+ηAG+\eta A as an ordinary klt adjoint. Here is the reason this remains valid when the nef b-divisor does not descend to VV.

Choose a projective log resolution h ⁣:V′→Vh\colon V'\to V carrying its nef part N′N' and write

KV′+Δ′+N′=h∗G.K_{V'}+\Delta'+N'=h^*G.

The coefficients of Δ′\Delta' are strictly less than one. The resolution can be chosen with an effective exceptional divisor FF such that −F-F is hh-ample. For sufficiently small rational ε>0\varepsilon> 0, the divisor N′+ηh∗A−εFN' + \eta h^*A - \varepsilon F is ample. A general effective rational representative of this ample class can be chosen with sufficiently small coefficients that, after adding εF\varepsilon F, it preserves the sub-klt condition of Δ′\Delta'. Its pushforward, added to Δ\Delta, is effective and defines a klt boundary Θ\Theta on VV with

KV+Θ∼QG+ηA.K_V + \Theta\sim_{\mathbb{Q}} G + \eta A.

The crepant equality can be checked upstairs: its difference is exceptional and relatively numerically trivial, hence zero by negativity.

The ordinary cone theorem now gives a rational curve generator CC with 0<−(G+ηA)⋅C≤2n0 < -(G + \eta A) \cdot C \le2n. The preceding comparison yields −G⋅C≤4n-G \cdot C \le4n. The contraction c:V→Sc: V \to S is the contraction of the same ray for this ordinary klt pair. Since its relative Picard number is one, there is a rational λ>0\lambda> 0 such that G−λ(KV+Θ)G - \lambda(K_V + \Theta) is numerically trivial over SS. The Cartier descent statement for an ordinary klt extremal contraction, after clearing denominators, gives a rational Cartier divisor DSD_S with

G−λ(KV+Θ)∼Qc∗DS.G - \lambda(K_V + \Theta) \sim_{\mathbb{Q}} c^*D_S.

In the small case, let c+:V+→Sc^+: V^+ \to S be the ordinary flip. Taking strict transforms gives

G+∼Qλ(KV++Θ+)+(c+)∗DS,G^+ \sim_{\mathbb{Q}} \lambda(K_{V^+} + \Theta^+) + (c^+)^*D_S,

which is ample over SS. Thus the ordinary flip is also the flip of GG. The ordinary contraction and flip preserve Q\mathbb{Q}-factoriality on the birational output. Their effective exceptional adjoint comparison, multiplied by λ\lambda, gives the asserted comparison for GG, since the terms pulled back from SS cancel. With the nef b-divisor fixed, this comparison is also the improvement of generalized discrepancies used below. □

Lemma 3.2. Let (X,B)(X, B) be a projective Q\mathbb{Q}-factorial klt Q\mathbb{Q}-pair of dimension nn, let T=KX+BT = K_X + B be pseudo-effective, and let MM be a nef Q\mathbb{Q}-Cartier divisor on XX. Suppose (3.1) holds. Then there are a birational contraction X⇢YX \dashrightarrow Y, a number s0∈Q>0s_0 \in\mathbb{Q}_{>0}, and a common smooth projective resolution

X←pW→qYX \xleftarrow{p} W \xrightarrow{q} Y

with the following properties. If BYB_Y and NN denote the transforms of BB and MM, and U=KY+BYU = K_Y + B_Y, then

  1. (Y,BY)(Y, B_Y) is klt and Q\mathbb{Q}-factorial, UU is semiample, and κ(Y,U)=κ(X,T)≥0\kappa(Y, U) = \kappa(X, T) \ge0;

  1. NN is pseudo-effective, and U+s0NU + s_0N is nef of full nef dimension;

  1. there are effective qq-exceptional rational divisors E0,E1E_0, E_1 on WW such that

p∗T=q∗U+E0,p∗(T+s0M)=q∗(U+s0N)+E1.p^*T = q^*U + E_0,\qquad p^*(T + s_0M) = q^*(U + s_0N) + E_1.

Proof. By Theorem 2.3, there is a terminating TT-MMP, ending on a Q\mathbb{Q}-factorial klt pair (Y0,B0)(Y_0, B_0) with nef adjoint U0=KY0+B0U_0 = K_{Y_0} + B_0. Theorem 2.2 makes U0U_0 semiample. The effective exceptional comparisons for the program give

κ(X,T)=κ(Y0,U0)≥0.\kappa(X, T) = \kappa(Y_0, U_0) \ge0.

Let N0N_0 be the transform of MM. It is the trace on Y0Y_0 of the fixed nef b-divisor determined by MM on XX.

Because this first program has finitely many steps, there is a rational s>0s > 0 such that every one of them remains negative for the transform of T+uMT + uM, for every rational u∈(0,s]u \in(0, s]. Choose ss also small enough to retain the strict sign on the flipped side of each flip. These are therefore programs for the corresponding generalized klt pairs: they start generalized klt on XX, and their discrepancies improve at each step. In particular, (Y0,B0+sM)(Y_0, B_0 + sM) is generalized klt. Pushforward to a Q\mathbb{Q}-factorial model preserves pseudo-effectivity, so N0N_0 is pseudo-effective.

For completeness, this last numerical assertion applies also to birational contractions with flips. On a common resolution, numerical pushforward to a Q\mathbb{Q}-factorial target is well defined: if a divisor upstairs is numerically trivial, its difference from the pullback of its pushforward is exceptional and relatively numerically trivial, and the negativity lemma makes that difference zero. Effective approximation then proves preservation of pseudo-effectivity.

Choose d>0d > 0 so that dU0dU_0 is Cartier and globally generated. Choose a rational s0∈(0,s)s_0 \in(0,s) such that

1−s0/sd>4ns0s.\frac{1-s_0/s}{d} > 4n\frac{s_0}{s}.

The generalized adjoint U0+s0N0U_0+s_0N_0 is pseudo-effective. Apply Theorem 2.3 to obtain a terminating program for it. We claim that every step is U0U_0-trivial and is also negative for the generalized adjoint with coefficient ss, where throughout this claim the symbols denote their transforms.

Suppose the claim holds up to the next step, and denote the current transforms by Ui,NiU_i,N_i. Then dUidU_i is still Cartier and free, and the pair with nef b-divisor coefficient ss is generalized klt. For a (Ui+s0Ni)(U_i+s_0N_i)-negative ray, the equality

Ui+s0Ni=(1−s0/s)Ui+(s0/s)(Ui+sNi)U_i+s_0N_i=(1-s_0/s)U_i+(s_0/s)(U_i+sN_i)

and nefness of UiU_i show that the ray is (Ui+sNi)(U_i+sN_i)-negative. Choose its rational curve generator CC by Lemma 3.1. If Ui⋅C>0U_i\cdot C>0, then integrality of dUidU_i gives Ui⋅C≥1/dU_i\cdot C\geq1/d, whence

(Ui+s0Ni)⋅C≥1−s0/sd−4ns0s>0,(U_i+s_0N_i)\cdot C\geq\frac{1-s_0/s}{d}-4n\frac{s_0}{s}>0,

a contradiction. Thus UiU_i is trivial on the ray.

The morphism defined by dUidU_i is constant on every fibre of the extremal contraction and factors through it. Its descended line bundle is globally generated; pulling it to the flipped model, when there is a flip, gives the transform of dUidU_i. Hence that transform is again Cartier and free, with equal pullbacks on a common resolution. Since the step is also negative for coefficient ss, generalized klt singularities with that coefficient persist. This proves the claim by induction through the finite program.

Let YY be its output. The ordinary adjoint UU is crepant throughout the second program, so (Y,BY)(Y,B_Y) is klt, UU is semiample, and its Iitaka dimension equals that of TT. The generalized adjoint U+s0NU+s_0N is nef. Combining the pullback comparisons of the two programs gives (3.2) with effective qq-exceptional divisors. The transform NN remains pseudo-effective.

It remains to prove full nef dimension. Suppose instead that the nef reduction of U+s0NU+s_0N has a positive-dimensional very general compact fibre FF. Shrink the base of the almost holomorphic map so that these compact fibres lie entirely in its morphism locus. The image in YY of the exceptional locus of qq has codimension at least two. A general fibre FF meets each of its components in codimension at least two, or not at all: discard the images of components that do not dominate the nef-reduction base, and use the fibre dimension theorem for the others. We may therefore choose a curve C⊂FC\subset F through a very general point, avoiding this exceptional image. If dim⁡F>1\dim F>1, take sufficiently general complete intersections in FF through that point; if dim⁡F=1\dim F=1, take FF itself.

Choose the point also in the common isomorphism locus of the birational contraction and with the very general conditions of (1) transported from XX. Since UU is nef and NN is pseudo-effective, Lemma 2.1 gives

U⋅C=N⋅C=0,U\cdot C=N\cdot C=0,

because their positive combination has degree zero on FF. The strict lift C~⊂W\widetilde C\subset W avoids E0E_0 and E1E_1. Both equalities in (3.2) then give

p∗T⋅C~=p∗M⋅C~=0.p^*T\cdot\widetilde C=p^*M\cdot\widetilde C=0.

The curve p(C~)p(\widetilde C) passes through the chosen very general point of XX and contradicts (1). ∩ევნ

Positive Iitaka dimension and the remaining case

The preceding construction leaves only one obstruction to bigness: the ordinary semiample adjoint may define a map to a point. If it defines a positive-dimensional base, the induction hypothesis handles its fibres.

Proposition 3.3. Assume (Pj)(P_j) for j<nj<n. Let (X,B)(X,B) be a projective klt Q\mathbb{Q}-pair of dimension nn, let T=KX+BT=K_X+B be pseudo-effective, and let MM be a nef Q\mathbb{Q}-Cartier divisor on XX. If (1) holds and κ(X,T)>0\kappa(X,T)>0, then T+cMT+cM is big for every c∈Q>0c\in\mathbb{Q}_{>0}.

Proof. After a small Q\mathbb{Q}-factorialization, apply Lemma 3.2. Let h:Y→Sh:Y\to S be the contraction defined by the semiample divisor UU. There is an ample rational divisor ASA_S on SS with U∼Qh∗ASU\sim_{\mathbb{Q}}h^*A_S, and dim⁡S=κ(X,T)>0\dim S=\kappa(X,T)>0. Put Q=U+s0NQ=U+s_0N.

If a very general fibre FF has positive dimension, it has dimension strictly less than nn. The restriction pair (F,BY∣F)(F,B_Y|_F) is klt and

KF+BY∣F∼QU∣F∼Q0.K_F+B_Y|_F\sim_{\mathbb{Q}}U|_F\sim_{\mathbb{Q}}0.

Moreover, Q∣FQ|_F is nef of full nef dimension. Indeed, a very general point of a very general FF can be chosen outside the countable union excluded in the full-nef-dimension assertion for QQ on YY. Since U∣F≡0U|_F\equiv0, the divisor N∣FN|_F is nef. Apply (Pdim⁡F)(P_{\dim F}) to this restriction pair and s0N∣Fs_0N|_F to conclude that Q∣FQ|_F is big. When the fibre dimension is zero, relative bigness is automatic.

Thus QQ is big over SS. To justify the passage to the generic fibre, fix an ample Cartier divisor HH on YY and shrink SS so that hh is flat. For every positive integer ℓ\ell clearing the denominators of QQ, upper semicontinuity makes the locus

{s∈S:H0(Fs,OFs((ℓQ−H)∣Fs))≠0}\{s\in S:H^0(F_s,\mathcal{O}_{F_s}((\ell Q-H)|_{F_s}))\ne0\}

closed. Bigness on a very general fibre puts its base point in one of these countably many loci. Choose that point outside every locus that is proper; the locus containing it must then be all of SS. On the generic fibre, ℓQ\ell Q is consequently the sum of the ample divisor HH and an effective divisor, which proves the asserted relative bigness. A relatively big divisor becomes big after adding a sufficiently large pullback of an ample divisor on the base; equivalently, apply the usual relative form of Kodaira’s lemma [3]. It follows that

Q+bU=(1+b)U+s0NQ+bU=(1+b)U+s_0N

is big for some rational b>0b>0. Equation (3.2) then shows that (1+b)T+s0M(1+b)T+s_0M is big.

Finally, fix c>0c>0 rational and choose λ>0\lambda>0 rational with λ(1+b)<1\lambda(1+b)<1 and λs0<c\lambda s_0<c. Then

T+cM=λ((1+b)T+s0M)+(1−λ(1+b))T+(c−λs0)M.T+cM=\lambda\bigl((1+b)T+s_0M\bigr)+(1-\lambda(1+b))T+(c-\lambda s_0)M.

The first summand is big and the other two are pseudo-effective. Their sum is big, as required. □

Proposition 3.4. Assume (Pj)(P_j) for j<nj<n. Suppose that on every projective klt Q\mathbb{Q}-pair (V,Δ)(V,\Delta) of dimension nn with KV+Δ≡0K_V+\Delta\equiv0, every nef Q\mathbb{Q}-Cartier divisor of full nef dimension is big. Then (Pn)(P_n) holds.

Proof. Use a small Q\mathbb{Q}-factorialization and Lemma 3.2. The nonnegative Iitaka dimension of TT is either positive, in which case Proposition 3.3 applies, or zero. In the latter case, semiample-ness of UU implies U∼Q0U\sim_{\mathbb{Q}}0. The pair (Y,BY)(Y,B_Y) is therefore a klt Calabi–Yau pair. The nef divisor U+s0NU+s_0N has full nef dimension, so it is big by the stated hypothesis. The second equality in (3.2) gives bigness of T+s0MT+s_0M. The positive-combination argument at the end of Proposition 3.3 gives bigness of T+cMT+cM for every rational c>0c>0.

Consequently, the remaining work for (Pn)(P_n) is the full-nef-dimension statement on klt Calabi–Yau pairs. Theorem 5.1 establishes its terminal, zero-boundary form. We then pass from that form to all klt Calabi–Yau pairs in Section 7.

Bounded-degree curves and moving jet kernels

The geometric argument will produce subvarieties with bounded degree and bounded canonical intersection. We first explain how these bounds contradict a growing lower bound for the degrees of curves. We then record the moving-center results from [28] that supply the required subvarieties. All varieties in this section are over C\mathbb{C}.

The bounded-degree obstruction.

Lemma 4.1 (Bounded-degree curves). For every integer f≥1f \ge1 there is an integer mf>0m_f > 0 with the following property. Let YY be a smooth integral projective variety of dimension ff, let D0D_0 be a reduced simple normal crossing divisor or the zero divisor, and let L0L_0 be a nef integral Cartier divisor of full nef dimension on YY. Suppose that P0P_0 is a nef rational Cartier divisor and that rr, C0C_0, C1C_1 are positive real numbers satisfying

0<P0f≤C0,P0−rL0 is nef.0 < P_0^f \le C_0,\qquad P_0-rL_0\text{ is nef}.

If A0=KY+D0+L0A_0=K_Y+D_0+L_0 is big and

A0⋅P0f−1≤C1P0f,(2)A_0\cdot P_0^{f-1}\le C_1P_0^f, \tag*{(2)}

then

r≤(mfC1)f−1C0.(3)r\le(m_fC_1)^{f-1}C_0. \tag*{(3)}

The integer mfm_f depends only on ff, and not on the variety or the divisors. For dimensions 1≤f≤n1\le f\le n, one may replace all mfm_f by a single integer mm depending only on nn.

Proof. The pair (Y,D0)(Y,D_0) is log canonical, its boundary coefficients belong to {0,1}\{0,1\}, and its nef polarizing divisor L0L_0 has Cartier index one. By [4], Theorem 1.3, an integer mfm_f depending only on these data makes ∣mfA0∣|m_fA_0| birational. Here A0A_0 is integral Cartier, so no rounding or additional denominator is involved.

Resolve the base ideal by a projective birational morphism μ:Y~→Y\mu:\widetilde{Y}\to Y, with Y~\widetilde{Y} smooth, and write

μ∗(mfA0)=H+F,\mu^*(m_fA_0)=H+F,

where HH is the basepoint-free moving part and FF is effective. The morphism defined by HH is birational onto its image; in particular HH is nef and big. In the rest of this proof, P0P_0 and L0L_0 denote their pullbacks to Y~\widetilde{Y}. Effectivity of FF and nefness of P0P_0 give

H⋅P0f−1≤mfC1P0f.(4)H\cdot P_0^{f-1}\le m_fC_1P_0^f. \tag*{(4)}

For f≥2f\ge2, put si=P0f−i⋅His_i=P_0^{f-i}\cdot H^i for 0≤i≤f0\le i\le f. Both divisors are nef and big, so the sis_i are positive. The Khovanskii–Teissier inequalities [21], Corollary 1.6.3(i) and Example 1.6.4,

si2≥si−1si+1s_i^2\ge s_{i-1}s_{i+1}

show that the ratios si/si−1s_i/s_{i-1} decrease. Hence

P0⋅Hf−1≤P0f(H⋅P0f−1P0f)f−1≤(mfC1)f−1C0.(5)P_0\cdot H^{f-1}\le P_0^f\left(\frac{H\cdot P_0^{f-1}}{P_0^f}\right)^{f-1}\le(m_fC_1)^{f-1}C_0. \tag*{(5)}

Choose a very general point y∈Y~y\in\widetilde{Y} over the isomorphism opens of both μ\mu and the morphism defined by HH. We also choose μ(y)\mu(y) in the very general locus that tests full nef dimension of L0L_0. Pull back f−1f-1 general hyperplanes through the image of yy under the morphism defined by HH. This subsystem has only the base point yy, so the general members meet properly and define an effective curve cycle of class Hf−1H^{f-1}; the component CC through yy is a curve because their local equations are independent at yy. Nefness gives

P0⋅C≤P0⋅Hf−1.P_0\cdot C\le P_0\cdot H^{f-1}.

The curve CC is not contracted by μ\mu, and its image passes through the chosen very general point. Full nef dimension and integrality therefore give L0⋅C≥1L_0\cdot C\ge1. Since P0−rL0P_0-rL_0 is nef, we obtain P0⋅C≥rP_0\cdot C\ge r, which proves (3).

If f=1f = 1, take C=YC = Y directly. Then P0⋅Y≥rL0⋅Y≥rP_0 \cdot Y \ge rL_0 \cdot Y \ge r, and the required bound is r≤C0r \le C_0. Finally, [4] applies to every multiple of its prescribed integer. A common multiple of the finitely many integers m1,…,mnm_1,\ldots,m_n therefore gives the last assertion. □\square

In particular, the hypotheses of Lemma 4.1 cannot hold along a sequence with r→∞r \to\infty and with C0,C1C_0,C_1 bounded, even if the varieties and divisors vary. The following observation explains how full nef dimension and pseudo-effectivity of the canonical divisor pass to the moving subvarieties used below.

Lemma 4.2 (Very general images). Let XX be a normal integral projective variety that is not uniruled, and let LL be a nef Cartier divisor of full nef dimension on XX. There is a complement X∘X^\circ of a countable union of proper closed subsets of XX with the following property. If YY is a smooth integral projective variety and g:Y→Xg : Y \to X is generically finite onto a positive-dimensional image meeting X∘X^\circ, then g∗Lg^*L has full nef dimension, YY is not uniruled, and KYK_Y is pseudo-effective.

Proof. Choose X∘X^\circ so that every curve through any of its points has positive LL-degree and no rational curve meets X∘X^\circ. The first condition is the very general characterization of full nef dimension. For the second, rational curves are parametrized by countably many algebraic families; the closure of the evaluation image of each such family is proper because XX is not uniruled.

Since g(Y)g(Y) meets X∘X^\circ, it is contained in none of the closed sets excluded in its definition. A very general point of YY thus maps into X∘X^\circ and lies in the quasi-finite locus of gg. Every curve through such a point has a curve as its image, so its g∗Lg^*L-degree is positive. This proves full nef dimension. A covering family of rational curves on YY would similarly give a nonconstant rational curve meeting X∘X^\circ, a contradiction. The pseudo-effectivity of KYK_Y now follows from [6]. □\square

Subadjunction and high-multiplicity components

We use the following five results from the section Tools for moving base components of [28]. Their hypotheses distinguish generic information along a center from global information about the ambient variety. Intersections on an integral subvariety are computed after pullback to its normalization and a smooth projective resolution. A base ideal is isolated at the generic point of a subvariety when its localization there is primary for the maximal ideal.

Lemma 4.3 (Numerical generic subadjunction, [28], Lemma 7.1). Let ZZ be a projective Q\mathbb{Q}-factorial klt variety, let Θ≥0\Theta\ge0 be a rational divisor, and let V⊂ZV \subset Z be integral of dimension f>0f > 0. Suppose that (Z,Θ)(Z,\Theta) is log canonical at the generic point of VV and has a divisor of log discrepancy zero with center VV. If PP is a nef rational Cartier divisor on VV and ρ:V∗→V\rho: V^* \to V is a smooth projective resolution factoring through its normalization, then

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

Only generic log canonicity is required. The proof in [28] uses the dlt modification of [13], whose truncated boundary leaves an effective surplus supported over the non-lc locus. On a minimal stratum over VV, adjunction gives a pair that is klt over the generic point of its connected-fiber base. This suffices for the klt-trivial canonical bundle formula and its b-nef moduli divisor [12]. The effective discriminant, the moduli divisor, and finite ramification have nonnegative intersections with the pulled-back nef class. The comparison uses canonical Weil cycles, so it requires no Q\mathbb{Q}-Gorenstein assumption on the normalization of VV.

Lemma 4.4 (A base component of high multiplicity, [28], Lemma 7.2). Let ZZ be a projective Q\mathbb{Q}-factorial klt variety of dimension dd, let RR be a nef rational Cartier divisor, and let k>0k > 0 be an integer such that kRkR is Cartier. Let 0≠H⊂H0(Z,OZ(kR))0 \ne\mathcal{H} \subset H^0(Z,\mathcal{O}_Z(kR)) 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}}. Let m\mathfrak{m} be the maximal ideal of OZ,ηV\mathcal{O}_{Z,\eta_V}. If bOZ,ηV⊂mh\mathfrak{b}\mathcal{O}_{Z,\eta_V}\subset\mathfrak{m}^{h} for an integer h>0h>0, there are a rational number 0<c≤(d−f)k/h0<c\leq(d-f)k/h and an effective rational divisor Θ∼QcR\Theta\sim_{\mathbb{Q}}cR such that (Z,Θ)(Z,\Theta) is log canonical at ηV\eta_V and has a log canonical place centered on VV. The degree and canonical bounds are

Rf⋅V≤(k/h)d−fRd,R^f\cdot V\leq(k/h)^{d-f}R^d,
KV∗⋅Rf−1≤(KZ+cR)∣V⋅Rf−1(f>0),(6)K_{V^*}\cdot R^{f-1}\leq(K_Z+cR)|_V\cdot R^{f-1}\qquad(f>0), \tag*{(6)}

where V∗V^* is a smooth projective resolution. The degree bound also holds for f=0f=0.

The degree estimate is the local multiplicity bound hd−fh^{d-f} combined with successive general cuts by the given linear series. The boundary is obtained by averaging general members with total coefficient equal to the generic log canonical threshold of b\mathfrak{b}. Thus it is an actual divisor to which Lemma 4.3 applies.

Full jet kernels and restriction to a fiber.

Lemma 4.5 (Moving multiplicity, [28], Lemma 7.3). Let ZZ be an integral projective variety of dimension dd, let RR be a nef, big, semiample rational Cartier divisor, and fix an integer k>0k>0 such that kRkR is Cartier. Choose positive real numbers τ0<⋯<τd\tau_0<\cdots<\tau_d with consecutive gap δ>0\delta>0. For x∈Zsmx\in Z_{\mathrm{sm}}, put

Hi(x)=H0(Z,OZ(kR)⊗mx⌈kτi⌉).\mathcal{H}_i(x)=H^0\left(Z,\mathcal{O}_Z(kR)\otimes\mathfrak{m}_x^{\lceil k\tau_i\rceil}\right).

Suppose that for very general xx all these spaces are nonzero and the base locus of H0(x)\mathcal{H}_0(x) has a positive-dimensional component through xx. If kδ≥4k\delta\geq4, then, after an algebraic parameter extension and restriction to nonempty opens, there are an integral parameter variety TT with a dominant marked-point map x:T→Zsmx:T\to Z_{\mathrm{sm}}, a fixed index i∈{0,…,d−1}i\in\{0,\ldots,d-1\}, and a family of integral subvarieties VtV_t containing x(t)x(t) and common to the base loci of Hi(x(t))\mathcal{H}_i(x(t)) and Hi+1(x(t))\mathcal{H}_{i+1}(x(t)). In particular, the incidence

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

dominates ZZ.

For general tt, the dimension ff of VtV_t lies in [1,d−1][1,d-1], VtV_t is an isolated component of the higher base locus at its generic point, and the entire higher-kernel base ideal is contained there in the ordinary power IVth\mathcal{I}_{V_t}^{h}, where

h=⌈kδ/2⌉,k/h≤2/δ.h=\lceil k\delta/2\rceil,\qquad k/h\leq2/\delta.

The incidence base ideal is likewise contained in IΓh\mathcal{I}_{\Gamma}^{h} on a dense open of Γ\Gamma. These containments are taken in the smooth ambient open. If ZZ is also Q\mathbb{Q}-factorial and klt, then

Rf⋅Vt≤(2/δ)d−fRd,R^f\cdot V_t\leq(2/\delta)^{d-f}R^d,
KVt∗⋅Rf−1≤(KZ+cR)∣Vt⋅Rf−1,0<c≤2(d−f)/δ.(7)K_{V_t^*}\cdot R^{f-1}\leq(K_Z+cR)|_{V_t}\cdot R^{f-1},\qquad0<c\leq2(d-f)/\delta. \tag*{(7)}

The top intersection on VtV_t is positive when VtV_t meets the open on which the big semiample contraction is an isomorphism.

The use of the full kernels matters: differentiation in the parameter lowers vanishing at the moving mark and still gives a global section in the lower kernel. Incidence dominance makes these parameter directions span the normal directions. The vanishing of all derivatives of order less than hh then gives the ordinary-power containment, which can be restricted to general fibers as follows.

Lemma 4.6 (Restriction of an isolated base ideal, [28], Lemma 7.4). In the setting of Lemma 4.5, let g:Z→Bg: Z \to B be a morphism. There is a dense open of the incidence with the following property. Choose (t,z)(t,z) in this open, put b=g(z)b=g(z), and suppose that VtV_t is smooth over a smooth open of its actual image at zz. Let FF be the reduced component through zz of the scheme fiber of Vt→g(Vt)V_t \to g(V_t). Near zz in ZbZ_b, the restricted higher-kernel base ideal has support exactly FF and is contained in the ordinary power IFhI_F^h.

If FF is proper in an integral ambient fiber component containing it, the restricted series is nonzero there and FF is an isolated base component at its generic point. Applying Lemma 4.4 on that ambient component additionally requires its projectivity, Q\mathbb{Q}-factoriality, klt singularities, and smoothness at the generic point of FF.

Here the fiber is chosen through a general incidence point. The statement does not assert the same conclusion for an arbitrary special fiber. Smoothness over the actual image identifies the restricted ideal of VtV_t with the reduced ideal of FF locally; this is what preserves ordinary powers.

The Q\mathbb{Q}-factoriality needed for the base-component estimates can also be supplied by a small projective Q\mathbb{Q}-factorialization σ:Z′→Z\sigma: Z' \to Z of a klt ambient variety. This passage is made only for components that meet the isomorphism open of σ\sigma. Their strict transforms retain the generic base-ideal and multiplicity conditions for the pulled-back series, and the testing class σ∗R\sigma^*R is nef. Since KZ′=σ∗KZK_{Z'}=\sigma^*K_Z, projection formula gives the same degree and canonical-intersection bounds on a common resolution. The pullback testing class need not be ample; nefness is the property used in these estimates. Passing to higher resolutions does not change the canonical intersections, because their additional exceptional divisors have zero intersection with the pulled-back testing class to the required power.

Finite covers with a fixed branch complement

A bound on the degree of a branched cover does not make the possible covers finite. The final companion input supplies the needed fixed branch complement from a family whose branch divisors do not sweep the base.

Lemma 4.7 (Finite covers after excluding sweeping branch divisors, [28], Lemma 7.5). Let YY be a normal integral projective variety, let V→TV \to T be a smooth projective family with integral fibers over an integral parameter variety, and let g:V→Yg: V \to Y be a morphism. Suppose that the general fiber maps gt:Vt→Yg_t: V_t \to Y are dominant and generically finite of degree at most a fixed integer ee.

After a finite parameter extension and shrinking, spread the geometric generic components of the zero divisor of the relative Jacobian over YsmY_{\mathrm{sm}} to divisors R1,…,RN\mathcal{R}_1,\ldots,\mathcal{R}_N in VV. Retain this notation after the base change. Let II consist of the indices jj for which gt((Rj)t)g_t((\mathcal{R}_j)_t) is a divisor in YY for general tt. Assume that

g(Rj)≠Y(j∈I).g(\mathcal{R}_j) \ne Y \qquad(j \in I).

After shrinking again, there is a smooth nonempty open Y∘⊂YY^\circ\subset Y over which every general finite normal Stein cover of YY is finite étale. Only finitely many such normal covers of Y∘Y^\circ occur, up to isomorphism over Y∘Y^\circ. The conclusion holds simultaneously for finitely many projections; the open and the finite lists may depend on all fixed parameters of the family.

To see the role of the hypothesis, remove YsingY_{\mathrm{sing}} and the finitely many proper image closures g(Rj)g(\mathcal{R}_j) for j∈Ij \in I. Every branch prime of a general Stein cover is accounted for by one of these relative Jacobian components. Purity therefore makes the restricted covers étale. The fundamental group of the resulting smooth complex variety is finitely generated, so it has only finitely many covers of degree at most ee. Finally, a finite normal cover of YY is determined by its function field, hence by its restriction to this fixed open.

Jets on a terminal variety with trivial canonical class

The reduction to a Calabi–Yau pair leaves a positivity problem for a nef divisor: full nef dimension must imply bigness. We first treat the case with trivial canonical bundle and terminal singularities. The argument follows the scalar and two-slot jet constructions of [28], Sections 7–8. Its geometric exclusions differ from the nonvanishing argument there: lower-dimensional instances of (Pj)(P_j) and the polarized effective birationality theorem replace the exclusions for a canonical nonvanishing counterexample.

Theorem 5.1. Let n≥2n \ge2, and assume (Pj)(P_j) for j<nj < n. Let XX be a projective Q\mathbb{Q}-factorial terminal complex variety of dimension nn with KX∼0K_X \sim0. If LL is a nef Cartier divisor on XX with full nef dimension, then LL is big.

The proof occupies this section and Section 6. Assuming that LL is not big, we obtain two contrasting jet estimates: sections on XX have small normalized vanishing order, whereas a projective bundle over X×XX \times X admits a large jet system. The Frobenius comparison will show that these estimates are incompatible.

Normalization and the curve obstruction

Throughout this section suppose that XX, LL form a counterexample to Theorem 5.1. Fix an ample Cartier divisor AA on XX and a positive rational number ϵ\epsilon such that

(14ϵ)n<14,80ϵ<34.(8)(14\epsilon)^n < \frac{1}{4}, \qquad80\epsilon< \frac{3}{4}. \tag*{(8)}

Let t>0t > 0 tend to zero along a sequence of rational numbers. Since LL is nef and not big, Ln=0L^n = 0. We may therefore choose positive integers r=r(t)r = r(t) satisfying

P=Pt=r(L+tA),r⟶∞,Pn⟶ϵn.P = P_t = r(L + tA), \qquad r \longrightarrow\infty, \qquad P^n \longrightarrow\epsilon^n.

For example, round ϵ/((L+tA)n)1/n\epsilon/((L+tA)^n)^{1/n} to the nearest positive integer. The divisor PP is ample and rational Cartier, and P−rLP-rL is nef. After discarding finitely many terms, we have

ϵn2≤Pn≤2ϵn.\frac{\epsilon^n}{2} \le P^n \le2\epsilon^n.

Every curve through a very general point of XX has positive integral LL-degree, hence PP-degree at least rr. Thus a covering family of curves of bounded PP-degree will give a contradiction.

We specify how the same obstruction applies to subvarieties and covers. A resolution W→XW \to X has an effective canonical divisor: pull back a nowhere-zero canonical form on the smooth locus of XX and use terminality. Hence WW, and therefore XX, is not uniruled [6]. By Lemma 4.2, if a smooth projective variety YY maps generically finitely to a positive-dimensional subvariety containing a sufficiently very general point of XX, then YY is not uniruled and the pulled-back Cartier divisor LYL_Y has full nef dimension. In particular, KYK_Y is pseudo-effective. If f=dim⁡Y<nf = \dim Y < n, the induction hypothesis (Pf)(P_f) applied to (Y,0)(Y,0) gives

KY+LY big.(9)K_Y + L_Y \text{ big}. \tag*{(9)}

All occurrences of “very general” below include the fixed conditions of Lemma 4.2.

Consequently, for f<nf < n it suffices to find on such a YY a nef testing divisor PYP_Y with

0<PYf≤C0,PY−rLY nef,KYPYf−1≤CPYf,0 < P_Y^f \le C_0, \qquad P_Y-rL_Y \text{ nef}, \qquad K_Y P_Y^{f-1} \le C P_Y^f,

where C0C_0, CC are independent of tt. Indeed, LYPYf−1≤PYf/rL_Y P_Y^{f-1} \le P_Y^f/r, so Lemma 4.1 applies. We will also use that lemma in dimension nn, after proving the required bigness separately. For the rest of this section, a bound is called uniform if it is independent of tt; it may depend on parameters fixed before tt tends to zero. Since the dimensions lie in a finite range, Lemma 4.1 excludes all such configurations once rr is sufficiently large.

The scalar jet estimate

Put ρ=(Pn)1/n\rho= (P^n)^{1/n}. The first estimate bounds the vanishing order of every section at a very general point; it is stronger than a bound on a single fixed linear system.

Lemma 5.2. In the setting of (5.2), for all sufficiently small tt and at a very general point x∈Xx \in X, every nonzero section of kPkP, where kk is a positive integer and kPkP is Cartier, satisfies

ord⁡x(s)≤4kρ.(10)\operatorname{ord}_x(s) \le4k\rho. \tag*{(10)}

Proof. Suppose that violations occur for arbitrarily small tt. Fix such a tt. At a very general point a violation for some kk implies that the corresponding complete jet kernel is nonzero at the general point. Indeed the kernel ranks are algebraic rank conditions on the smooth locus, and there are only countably many choices of kk and of the required integral order. Raising the violating section to powers allows kk to be arbitrarily large and divisible.

Choose n+1n+1 levels

τi=32ρ+iδ(0≤i≤n),δ=2ρn.\tau_i = \frac{3}{2}\rho+ i\delta\quad(0 \le i \le n), \qquad\delta= \frac{2\rho}{n}.

They all lie strictly between ρ\rho and 4ρ4\rho. For a sufficiently large divisible kk, their full jet kernels are nonzero and kδ≥4k\delta\ge4. The lowest kernel has a positive-dimensional base component through its marked point. Otherwise that point would be an isolated base component of multiplicity at least h0=⌈kτ0⌉h_0 = \lceil k\tau_0\rceil. The zero-dimensional case of Lemma 4.4 would give

1≤(k/h0)nPn<1,1 \le(k/h_0)^n P^n < 1,

a contradiction.

Lemma 4.5 now supplies a moving family of proper base components VV, with dominant incidence and dimension 1≤f<n1 \le f < n. On a resolution V∗V^*, write PV,LVP_V,L_V for the restrictions followed by pullback. The lemma gives

0<PVf≤(2/δ)n−fPn,KV∗⋅PVf−1≤cPVf,0<c≤2(n−f)δ.0 < P_V^f \le(2/\delta)^{n-f}P^n, \qquad K_{V^*}\cdot P_V^{f-1} \le cP_V^f, \qquad0 < c \le\frac{2(n-f)}{\delta}.

Here the canonical term of the ambient variety vanishes because KX∼0K_X \sim0. The volume window (5.3) bounds δ\delta above and away from zero, so these are uniform estimates. The incidence point may be chosen over a very general point of XX. Thus (9) gives bigness of KV∗+LVK_{V^*}+L_V, and PV−rLVP_V-rL_V is nef. Lemma 4.1 contradicts r→∞r \to\infty. □

The projective bundle and its volume

We now seek a jet system whose order is much larger than the scalar bound. The additional direction comes from the fibres of a projective bundle; its two summands keep track of the two copies of XX. For a divisor on XX, subscripts 1,21,2 denote pullback from the two factors of X×XX \times X. Set

Z=P(OX(L)1⊕OX(L)2)→πX×X,ξ=c1(OZ(1)),R=P1+P2+qξ,(11)Z = \mathbb{P}\left(\mathcal{O}_X(L)_1 \oplus\mathcal{O}_X(L)_2\right) \xrightarrow{\pi} X \times X, \qquad\xi= c_1(\mathcal{O}_Z(1)), \qquad R = P_1 + P_2 + q\xi, \tag*{(11)}

where qq is a positive integer to be fixed shortly. We use the convention π∗OZ(a)=Sym⁡a(OX(L)1⊕OX(L)2)\pi_*\mathcal{O}_Z(a) = \operatorname{Sym}^a(\mathcal{O}_X(L)_1 \oplus\mathcal{O}_X(L)_2) for a≥0a \ge0. The tautological class ξ\xi is nef, and RR is ample. The product and projective-bundle descriptions show that ZZ is klt. The two natural sections, called the axes, have classes ξ−L1\xi-L_1 and ξ−L2\xi-L_2. The canonical bundle formula gives

KZ∼−(sum of the two axes).(12)K_Z \sim-(\text{sum of the two axes}). \tag*{(12)}

We call the complement of the axes the torus open.

The fibre of either projection Z→XZ \to X over a smooth point is, up to a constant one-dimensional factor,

Zsl=P(OX⊕OX(L)),Rsl=P+qξ.Z_{\mathrm{sl}} = \mathbb{P}(\mathcal{O}_X \oplus\mathcal{O}_X(L)), \qquad R_{\mathrm{sl}} = P + q\xi.

Its axes have classes ξ\xi and ξ−L\xi-L, and its canonical divisor is again minus their sum. The slice is projective and klt. In particular it has the singularity hypotheses needed to apply the base-component estimates, using a small Q\mathbb{Q}-factorialization if necessary as explained after Lemma 4.5.

Write d=2n+1d=2n+1. There are positive constants depending only on nn such that, for each fixed qq and all sufficiently small tt,

cnqε2n≤Rd≤Cnqε2n,Rsln+1≤Csl,nqεn.(13)c_n q\varepsilon^{2n}\le R^d\le C_n q\varepsilon^{2n},\qquad R_{\mathrm{sl}}^{n+1}\le C_{\mathrm{sl},n}q\varepsilon^n. \tag*{(13)}

To see this, expand in nef classes and use

π∗(ξj)=∑a=0j−1L1aL2j−1−a(j≥1).\pi_*(\xi^j)=\sum_{a=0}^{j-1}L_1^aL_2^{j-1-a}\qquad(j\ge1).

The term containing exactly one ξ\xi is (2n+1)(2nn)q(Pn)2(2n+1)\binom{2n}{n}q(P^n)^2, giving the lower bound. For the upper bound, every occurrence of LiL_i can be bounded in mixed nef intersections by Pi/rP_i/r. After factoring out qq, the remaining powers of q/rq/r are bounded by one once r≥qr\ge q. There are only finitely many terms depending on nn. The slice calculation is the same, using π∗(ξj)=Lj−1\pi_*(\xi^j)=L^{j-1}. Together with (5.3), this proves (5.8).

For a nef rational Cartier divisor RR and a smooth point zz, its Seshadri constant is

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

where CC ranges over integral curves through zz. Thus a lower bound for this constant controls degree relative to multiplicity at the point.

Proposition 5.3. For a suitable fixed positive integer qq, and all sufficiently small tt in (5.2), there is a smooth point z∈Zz\in Z in the torus open, lying over smooth points of both factors, such that

ε(R;z)>2n+2.\varepsilon(R;z)>2n+2.

More generally, for any prescribed dense open subsets U1,U2U_1,U_2 of the smooth locus of XX, the point may be chosen over U1×U2U_1\times U_2. In particular, these opens may be the isomorphism loci of fixed resolutions of XX.

We prove the proposition in the remainder of this section. Choose a positive rational gap δ\delta such that

(2/δ)nCsl,nεn<1.(14)(2/\delta)^n C_{\mathrm{sl},n}\varepsilon^n<1. \tag*{(14)}

Next choose qq so large that d+1d+1 increasing levels of gap δ\delta, with lowest level strictly greater than 2n+22n+2, lie strictly below (cnqε2n)1/d(c_nq\varepsilon^{2n})^{1/d}. These choices precede the limit t→0t\to0.

Fix the prescribed opens U1,U2U_1,U_2, if any. Suppose that (5.9) fails throughout their smooth torus preimage for arbitrarily small tt. For any such tt, asymptotic Riemann–Roch and the elementary jet count at a smooth point show that all the full kernels at the chosen levels are nonzero for sufficiently large divisible kk. Indeed the highest level has dd-th power smaller than RdR^d. Failure of (5.9) supplies, through each very general point, a curve with degree divided by multiplicity smaller than the lowest level. Every section in the lowest kernel vanishes identically on that curve: otherwise its intersection with the curve is at least its vanishing order times the curve’s multiplicity, contradicting the degree inequality. Thus the lowest base locus has a positive-dimensional component through the mark. Take kδ≥4k\delta\ge4 and apply Lemma 4.5.

We obtain a family of proper integral components V⊂ZV\subset Z whose incidence dominates ZZ. For its general members, of dimension ff, the estimates are

0<Rf⋅V≤(2/δ)d−fRd,0<R^f\cdot V\le(2/\delta)^{d-f}R^d,
KV∗⋅Rf−1≤(KZ+cR)∣VRf−1,0<c≤2(d−f)/δ.(15)K_{V_*}\cdot R^{f-1}\le(K_Z+cR)|_V R^{f-1},\qquad0<c\le2(d-f)/\delta. \tag*{(15)}

Here and below classes on a resolution are understood by pullback. The positivity follows from ampleness of RR. General members meet the torus open, so (5.7) makes the ambient canonical contribution nonpositive. All constants in these bounds are uniform now that qq, ϵ\epsilon, δ\delta have been fixed.

Excluding positive-dimensional slice fibres

We first constrain the two projections of VV to XX. For either projection, consider the component FF of a general fibre of V→im⁡(V→X)V \to\operatorname{im}(V \to X) through a general incidence point. Choose that incidence point in the opens of Lemma 4.6, over very general points of both factors of XX, and in the smooth torus open. We claim that

dim⁡F∉{1,…,n}.\dim F \notin\{1,\ldots,n\}.

Suppose instead that 1≤fsl=dim⁡F≤n1 \leq f_{\mathrm{sl}} = \dim F \leq n. The ambient fibre is ZslZ_{\mathrm{sl}}, of dimension n+1n+1. The restriction lemma gives a nonzero restricted subseries with FF an isolated base component and base ideal contained generically in IFh\mathcal{I}_{F}^{h}, where h=⌈kδ/2⌉h = \lceil k\delta/2\rceil. Generic smoothness is imposed over the actual image of VV; this is why a general fibre through the incidence point was chosen. The point is also smooth in the ambient slice. Applying Lemma 4.4 on that slice gives

0<Rslfsl⋅F≤(2/δ)n+1−fslRsln+1,KF∗Rslfsl−1≤(KZsl+cRsl)∣FRslfsl−1,(16)0 < R_{\mathrm{sl}}^{f_{\mathrm{sl}}} \cdot F \leq(2/\delta)^{n+1-f_{\mathrm{sl}}}R_{\mathrm{sl}}^{n+1}, \\ K_{F^*}R_{\mathrm{sl}}^{f_{\mathrm{sl}}-1} \leq(K_{Z_{\mathrm{sl}}}+cR_{\mathrm{sl}})|_{F}R_{\mathrm{sl}}^{f_{\mathrm{sl}}-1}, \tag*{(16)}

with c≤2(n+1−fsl)/δc \leq2(n+1-f_{\mathrm{sl}})/\delta. Cartier multiples are chosen before restriction, so the constant line from the fixed factor causes no change in this calculation.

Let W0⊂XW_0 \subset X be the image of FF in the other factor. There are three cases: FF is generically finite over a proper subvariety of XX; FF contains the projective-line fibres over its image; or FF is a multisection over all of XX.

A generically finite map to a proper subvariety. If F→W0F \to W_0 is generically finite and dim⁡W0<n\dim W_0 < n, use PY=Rsl∣F∗P_Y = R_{\mathrm{sl}}|_{F^*} and the pullback LYL_Y from XX. The first inequality in (16) gives a uniform positive volume bound. Since FF meets neither axis generically, its ambient canonical term is nonpositive. Hence the second inequality gives a uniform canonical-intersection ratio. Moreover PY−rLYP_Y-rL_Y is nef. The image W0W_0 contains the very general projection of the incidence point, so (9) applies. Lemma 4.1 excludes this case for large rr.

A projective-line bundle over a proper subvariety. If F→W0F \to W_0 is not generically finite, its general fibre has dimension one. Since the ambient projection is a projective-line bundle and FF is integral, FF is the full bundle over W0W_0. Write w=dim⁡W0=fsl−1w=\dim W_0=f_{\mathrm{sl}}-1. If w=0w=0, then FF is a projective-line fibre and Rsl⋅F=qR_{\mathrm{sl}}\cdot F=q. The first inequality in (16), together with (13) and (14), gives

q≤(2/δ)nRsln+1≤(2/δ)nCsl,nqϵn<q,q \leq(2/\delta)^n R_{\mathrm{sl}}^{n+1} \leq(2/\delta)^n C_{\mathrm{sl},n}q\epsilon^n < q,

which is impossible.

Suppose w>0w>0. Resolve W0W_0 to W0∗W_0^* and take as a resolution of FF the induced projective bundle p0:F∗→W0∗p_0:F^*\to W_0^*. Its relative canonical divisor is −2ξ+p0∗L-2\xi+p_0^*L, exactly the restriction of KZslK_{Z_{\mathrm{sl}}}. Cancelling this term in (16) gives

p0∗KW0∗Rslw≤cRslw+1⋅F.(17)p_0^*K_{W_0^*}R_{\mathrm{sl}}^w \leq cR_{\mathrm{sl}}^{w+1}\cdot F. \tag*{(17)}

The divisor KW0∗K_{W_0^*} is pseudo-effective by the very general point condition. On expanding the left side and pushing down, its term with exactly one ξ\xi is wqKW0∗Pw−1wqK_{W_0^*}P^{w-1}; every other nonzero term is nonnegative, since it pairs the pseudo-effective canonical divisor with nef classes. On the right, the same expansion used for (13) gives

(w+1)qPw⋅W0≤Rslw+1⋅F≤Cn′qPw⋅W0,(18)(w+1)qP^w\cdot W_0 \leq R_{\mathrm{sl}}^{w+1}\cdot F \leq C'_n qP^w\cdot W_0, \tag*{(18)}

using r≥qr \ge q. The slice degree bound and the first inequality in (5.15) bound 0<Pw⋅W00 < P^{w} \cdot W_{0} uniformly. Equations (5.14)–(5.15) also give

KW0∗Pw−1≤CCn′wPw⋅W0.K_{W_{0}^{*}}P^{w-1} \le\frac{CC'_{n}}{w}P^{w}\cdot W_{0}.

Apply (5.4) and Lemma 4.1 on W0∗W_{0}^{*} with the pullbacks of P,LP,L. This excludes the second case.

A multisection over XX. The only remaining possibility is that fsl=nf_{\mathrm{sl}}=n and F→XF \to X is generically finite of degree e>0e>0. Intersect FF with each of the two Cartier axes and push the resulting cycles down to XX. This gives effective integral Weil divisors D1,D2D_{1},D_{2}. The axes do not contain FF, and their classes differ by LL; projection of the associated rational section, or equivalently its norm, gives

D1−D2∼±eL.(19)D_{1}-D_{2}\sim\pm eL. \tag*{(19)}

For either axis SS, the classes Rsl−qSR_{\mathrm{sl}}-qS and Rsl−PR_{\mathrm{sl}}-P are nef. Intersecting with the effective cycle S⋅FS\cdot F and then using nefness on FF yields

qDiPn−1≤qS⋅F⋅Rsln−1≤Rsln⋅F.(20)qD_{i}P^{n-1}\le qS\cdot F\cdot R_{\mathrm{sl}}^{n-1}\le R_{\mathrm{sl}}^{n}\cdot F. \tag*{(20)}

Thus both axis-image degrees are uniformly bounded.

Set G=D1+D2G=D_{1}+D_{2}. It is Q\mathbb{Q}-Cartier because XX is Q\mathbb{Q}-factorial. Choose b>0b>0 rational sufficiently small that (X,bG)(X,bG) is klt. We claim

κ(KX+bG)>0.(21)\kappa(K_{X}+bG)>0. \tag*{(21)}

The Iitaka dimension is at least zero, since KX+bG∼QbGK_{X}+bG\sim_{\mathbb{Q}} bG. If it were zero, Theorems 2.3 and 2.2 would give a finite ordinary MMP to a good model YY with transformed adjoint rationally linearly trivial. The transform of KXK_{X} is linearly trivial as well. Consequently the effective transform of GG is zero: all its components have been contracted. On a common resolution a:U→Xa:U\to X, bY:U→Yb_{Y}:U\to Y, relation (5.16) then expresses a∗La^{*}L up to rational linear equivalence as a signed bYb_{Y}-exceptional divisor EE. Divisors exceptional over XX are also exceptional over YY, since the MMP extracts none. Nefness of a∗La^{*}L and the negativity lemma imply E≤0E\le0. Its class is also pseudo-effective. A nonzero anti-effective divisor has negative intersection with a sufficiently high power of an ample divisor, so E=0E=0. This contradicts full nef dimension of LL, and proves (5.18).

The already proved positive-Iitaka-dimension case (Proposition 3.3) now gives

KX+bG+L big.K_{X}+bG+L\text{ big}.

Its full-positivity hypothesis holds because LL has full nef dimension and KX+bGK_{X}+bG is pseudo-effective. Take a log resolution a:Y→Xa:Y\to X of GG and let D0D_{0} be the reduced simple normal crossings divisor consisting of the strict support of GG and every exceptional divisor. Decrease bb if necessary; Proposition 3.3 still applies. Terminality and the support of a∗Ga^{*}G then give

KY+D0+a∗L≥a∗(KX+bG+L)K_{Y}+D_{0}+a^{*}L\ge a^{*}(K_{X}+bG+L)

up to rational linear equivalence and an effective difference. Indeed the finitely many exceptional discrepancies are positive, and decreasing bb makes each coefficient of ba∗Gba^{*}G no larger than the corresponding coefficient of KY−a∗KX+D0K_{Y}-a^{*}K_{X}+D_{0}. Hence the left side is big.

Test on YY with a∗Pa^{*}P. Exceptional divisors contribute zero to intersection with (a∗P)n−1(a^{*}P)^{n-1}, and KX∼Q0K_{X}\sim_{\mathbb{Q}}0. The degree of the reduced strict support is no larger than GPn−1GP^{n-1}, bounded by (5.17); also LPn−1≤Pn/rLP^{n-1}\le P^{n}/r. Since (5.3) bounds PnP^{n} away from zero, we obtain a uniform constant CC such that

(KY+D0+a∗L)(a∗P)n−1≤C(a∗P)n.(K_{Y}+D_{0}+a^{*}L)(a^{*}P)^{n-1}\le C(a^{*}P)^{n}.

Lemma 4.1, now with its reduced boundary D0D_{0}, gives the final contradiction. This proves (5.12).

Thus a general moving component VV has fibre dimension either zero or n+1n+1 over its image in either factor. Fibre dimension n+1n+1 would make VV the full inverse image of its image in that factor. Since VV is proper, the image has dimension at most n−1n-1, so the other projection would have fibre dimension between 11 and nn, already excluded. Both projections of VV are therefore generically finite onto their images, and dim⁡V≤n\dim V \le n. If dim⁡V<n\dim V < n, the bounds (15), the nef class R−rLiR-rL_i, and (9) again contradict Lemma 4.1. Only nn-dimensional correspondences, dominant over both factors, remain.

Correspondences and their branch divisors

For these remaining VV, (15) gives uniform bounds

Rn⋅V≤C,KV∗Rn−1≤cRn⋅V≤C,R^n \cdot V \le C,\qquad K_{V^*}R^{n-1} \le cR^n \cdot V \le C,

after increasing CC. Each projection has bounded degree: R−PiR-P_i is nef, and PnP^n is bounded below.

For each fixed tt, resolve the general members in their algebraic family and shrink the parameter space so that the resolutions form a smooth projective family with integral fibres and morphisms to XX in both slots. The dominant incidence and all numerical bounds persist. Finite extensions of the parameter space are allowed. Over XsmX_{\mathrm{sm}}, name the components of the relative Jacobian divisors as in Lemma 4.7. Consider a component whose image on a general member is a divisor J⊂XJ \subset X.

Such divisors JJ cannot sweep XX. If they did, choose a general one through a very general point. Let EJE_J be a ramification divisor over it on the corresponding V∗V^*. Pullback of a canonical form from XX gives an effective canonical divisor on V∗V^*. Regularity follows by factoring through a resolution of XX and using its canonical singularities; the coefficient of EJE_J is positive because its image meets XsmX_{\mathrm{sm}} generically. The difference R−PiR-P_i is nef, so (5.19) and projection formula bound

0<dJ:=Pn⋅J≤C.0 < d_J := P^n \cdot J \le C.

On a resolution J∗J^*, Lemma 4.3, applied to (X,J)(X,J) at the generic point of JJ, gives

KJ∗Pn−2≤(KX+J)⋅J⋅Pn−2=J2Pn−2≤(JPn−1)2Pn≤C′dJ.(22)\begin{aligned} K_{J^*}P^{n-2} \le(K_X+J)\cdot J\cdot P^{n-2} \\ &= J^2P^{n-2} \le\frac{(JP^{n-1})^2}{P^n} \le C'd_J. \tag*{(22)} \end{aligned}

The pair is lc at that generic point because XX is normal and hence smooth there. The middle inequality is the Hodge index inequality, applied on a resolution and obtained by ample approximation of the pulled-back testing class. It does not require JJ to be nef. The final constant is uniform by the volume lower bound and the bound for dJd_J.

Since JJ sweeps XX, its resolution satisfies the very general point conditions used in (9). With testing class P∣J∗P|_{J^*}, whose top self-intersection is dJd_J, (22) gives precisely the hypotheses of Lemma 4.1 in dimension n−1n-1. This contradiction excludes sweeping branch divisors.

Lemma 4.7 now gives, for each slot and this fixed tt, only finitely many possible finite normal Stein covers of XX, up to isomorphism over XX. The point of the preceding step is that degree bounds alone would not give this conclusion: non-sweeping branch images provide a fixed smooth branch complement for the family. Neither that complement nor the resulting finite lists need be uniform in tt.

Fixed covers and an abelian model

Each V∗V^* maps birationally to both of its normal Stein covers, and hence determines a graph of a birational map between a pair of covers in the finite lists. We explain why some such fixed pair has a family of graphs dominating its product. Restrict the finite set of pairs to those realized by at least one original member V∗V^* satisfying (5.19). The original incidence dominates ZZ, so the projected incidences for these pairs cover a dense open of X×XX \times X. For a fixed pair, graphs of birational maps lie in countably many Hilbert schemes. Stratify these schemes so that the fibres are integral and flat and both projections are birational; the latter conditions may be tested by dominance and degree one after shrinking. Because CC is uncountable, a dense open of X×XX \times X cannot be covered by countably many proper closed subsets. Thus, for one fixed pair T1,T2T_1,T_2, some integral graph family has dominant evaluation to X×XX \times X. Since T1×T2T_1 \times T_2 is finite over X×XX \times X and has the same dimension, this evaluation is dominant onto T1×T2T_1 \times T_2 as well.

Both covers are non-uniruled because they are finite over XX. The birational-group theorem of Hanamura [17], in the form recalled in [5], implies that they are birational to an abelian variety. Here are the details of the application. Identify the two covers birationally by one map in the family. On a suitable smooth projective birational model of the resulting non-uniruled variety, the reduced birational group is a group scheme locally of finite type, with identity component an abelian variety acting regularly. Conjugate the graph family to this model and shrink again to obtain a flat family of integral graphs. By the flat-graph representability statement, its reduced integral parameter space maps to the reduced birational group. Its connected image lies in one translate of the identity component. Product-dominant evaluation therefore gives a dense orbit for that abelian identity component. The orbit is a quotient of an abelian variety by a stabilizer, hence is itself an abelian variety. The fixed cover is birational to it. This is the birational-group part of the fixed-cover argument in [28]; no canonical nonvanishing conclusion from that proposition is being used.

This structural conclusion depends only on the two covers. We may therefore return to an original member V∗V^* belonging to this pair, which retains (5.19), and resolve further to obtain a birational morphism

p0:V∗⟶A0p_0 : V^* \longrightarrow A_0

to an abelian variety. Higher resolutions do not change the canonical intersection with the pulled-back (n−1)(n-1)-st power of RR. Let L0L_0 be the pullback of LL from either slot. It is nef, Cartier, and of full nef dimension. We claim

KV∗+L0 big.(23)K_{V^*} + L_0 \text{ big}. \tag*{(23)}

The pushforward N0=(p0)∗L0N_0 = (p_0)_*L_0 is pseudo-effective on A0A_0, and is therefore nef. Indeed translations make the pseudo-effective and nef cones of an abelian variety coincide. If N0N_0 were not big, the standard description of nef line bundles on abelian varieties would give a positive-dimensional abelian subvariety on whose translates N0N_0 is numerically trivial. One can see this from the semipositive Hermitian form of the numerical class: its kernel is rational for the lattice, since the alternating form of the integral Cartier class is integral, and therefore defines an abelian subvariety. A general translate meets the image of the exceptional locus of p0p_0 in codimension at least two, if at all. Complete-intersection curves in that translate can thus be chosen through very general points and avoiding this image. Their lifts have L0L_0-degree zero, contradicting full nef dimension. Hence N0N_0 is big.

By the negativity lemma,

p0∗N0−L0=E0≥0p_0^*N_0 - L_0 = E_0 \ge0

is exceptional. The canonical divisor of V∗V^* has an effective representative EKE_K with positive coefficient along every p0p_0-exceptional divisor, because the target is smooth with trivial canonical bundle. Choose a rational 0<u<10 < u < 1 sufficiently small that EK−uE0≥0E_K - uE_0 \ge0. Then

KV∗+uL0∼Qup0∗N0+(EK−uE0)K_{V^*} + uL_0 \sim_{\mathbb{Q}} up_0^*N_0 + (E_K - uE_0)

is big. Adding the nef divisor (1−u)L0(1-u)L_0 proves (23).

We may now apply Lemma 4.1 in dimension nn on V∗V^*, with testing class RR and empty boundary. The bounds (5.19) give both the top intersection bound and the canonical ratio, while R−rL0R-rL_0 is nef and (23) supplies bigness. This final contradiction excludes the correspondence case.

Conclusion of the proof of Proposition 5.3. The alternatives for every moving base component have been exhausted: first its slice fibres, then components of dimension less than nn, sweeping branch divisors, and finally the fixed covers. In each case the contradiction comes from Lemma 4.1 with constants uniform in tt. The finite cover lists were used only for one fixed tt, and their sizes do not enter the degree bounds. Thus failures of (5.9) cannot occur along a sequence t→0t \to0. This proves the proposition, including the additional open conditions on the chosen point. □

We have now constructed, under the hypothetical failure of Theorem 5.1, the scalar estimate of Lemma 5.2 and the projective-bundle estimate of Proposition 5.3. The next section fixes one sufficiently small value of tt and places these data in the finite-data Frobenius comparison.

Frobenius comparison

The scalar estimate of Lemma 5.2 and the projective-bundle estimate of Proposition 5.3 will now give the contradiction needed for Theorem 5.1. Their incompatibility is expressed by the following theorem about fixed complex data. It is the finite-data Frobenius theorem of [28]. We give its proof, including the bounds that must be uniform when the residual characteristic varies.

The argument compares two orders of vanishing of one determinant. Ordinary jets make the determinant nonzero after reduction to positive characteristic. A small polarization bounds the rank on the diagonal, forcing high vanishing at each diagonal point. A fixed movable curve on a point blowup bounds the vanishing of every section of each determinant factor and gives the opposite inequality.

The finite-data statement

For a vector bundle on a smooth projective curve, its slope is degree divided by rank. The least and greatest Harder–Narasimhan slopes are denoted by μmin⁡\mu_{\min} and μmax⁡\mu_{\max}. For a line bundle on a smooth variety, to generate jets through order aa at a point means surjectivity to its stalk modulo the (a+1)(a+1)-st power of the maximal ideal.

Theorem 6.1 (Finite-data Frobenius incompatibility). Let WW be a smooth connected projective complex variety of dimension n≥2n \ge2. Let DD, HH be rational Cartier divisors, with HH ample, let SS be an integral Cartier divisor, and fix an integer q>0q > 0 and real numbers r>1r > 1, ϵ>0\epsilon> 0. Suppose

Hn≤(2ϵ)n,KWHn−1≤2Hnr,(2D+qS)Hn−1≤4Hn,(14ϵ)n<14,80ϵ<34.(24)\begin{aligned} H^n &\le(2\epsilon)^n, & K_W H^{n-1} &\le\frac{2H^n}{r}, & (2D+qS)H^{n-1} &\le4H^n,\\ (14\epsilon)^n &< \frac{1}{4}, & 80\epsilon&< \frac{3}{4}. \tag*{(24)} \end{aligned}

Assume that the following fixed data exist.

(i) A smooth integral complete-intersection flag from WW to a curve CC, whose successive divisor classes are hi=liHh_i=l_iH for fixed positive integers lil_i for which liHl_iH is Cartier, with μmin⁡(ΩW1∣C)≥0\mu_{\min}(\Omega^1_W|_C) \ge0.

(ii) On the projective bundle

Z=P(OW(S)1⊕OW(S)2)⟶W×W,ξ=c1(OZ(1)),M=D1+D2+qξ,Z=\mathbb{P}\bigl(\mathcal{O}_W(S)_1\oplus\mathcal{O}_W(S)_2\bigr)\longrightarrow W\times W,\qquad \xi=c_1\bigl(\mathcal{O}_Z(1)\bigr),\qquad M=D_1+D_2+q\xi,

use the convention that the direct image of OZ(aξ)\mathcal{O}_Z(a\xi) is the aa-th symmetric power of the displayed sum for a≥0a\ge0; subscripts indicate pullback from the corresponding factor of W×WW\times W. The two axes are the sections defined by the two summands. A smooth point z∗z_* in their complement and finitely many sections of k0Mk_0M, for some integer k0>0k_0>0 with k0Dk_0D Cartier, generate jets through order (2n+2)k0(2n+2)k_0 at z∗z_*. (iii) A point x∈Wx \in W, its blowup πx:W^→W\pi_x:\widehat{W} \to W with exceptional divisor JJ, 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 one fixed birational morphism, VV is smooth integral projective, and the AiA_i are ample integral Cartier divisors, such that J⋅γ>0J\cdot\gamma>0 and

πx∗(D+KW/2+λS)⋅γ≤40ϵJ⋅γ(0≤λ≤q).\pi_x^*(D+K_W/2+\lambda S)\cdot\gamma\le40\epsilon J\cdot\gamma\qquad(0\le\lambda\le q).

It suffices to check the two endpoints in this affine inequality.

These data cannot coexist.

The point xx is independent of the two base coordinates of z∗z_*. No nefness is required of DD, SS, or KWK_W, and the theorem does not assume that KWK_W is pseudo-effective. Its hypotheses specify the flag and the movable curve class themselves. All these data will be fixed before the residual characteristic tends to infinity.

Reduction and Frobenius jets

We begin the proof of Theorem 6.1 by spreading its hypotheses and converting the fixed ordinary jets into jets of order proportional to the residual characteristic. Put Λ=∏i=1n−1li\Lambda=\prod_{i=1}^{n-1}l_i. The flag satisfies

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

Choose one sufficiently ample integral Cartier divisor T0T_0 so that every T0+aST_0+aS, for integers 0≤a≤(k0−1)q0\le a\le(k_0-1)q, has a section nonvanishing at each of the two base coordinates of z∗z_*. Fix these finitely many sections. All models, morphisms, divisors, points, the flag, the complete-intersection witness for γ\gamma, and the jet and filler sections spread over an integral finitely generated Z\mathbb{Z}-algebra of characteristic zero. Shrink its spectrum so that the fibers and flag are smooth projective and geometrically integral, the birational morphisms remain birational, the fixed ample bundles remain ample, and the finite jet surjection and nonvanishings persist. Birationality is preserved by spreading an isomorphism between dense opens. All displayed intersection numbers are constant.

We also preserve μmin⁡(ΩW1∣C)≥0\mu_{\min}(\Omega^1_W|_C)\ge0. One way is to spread its characteristic-zero Harder–Narasimhan filtration, make all its factors locally free, and use openness of their semistability on curves; their degrees and ranks are fixed. Equivalently, a single relative ample twist globally generates the curve bundle. Every quotient of rank aa then has degree bounded below by −ad-ad for a fixed integer dd. A negative-degree quotient therefore has one of finitely many ranks and degrees. The proper relative Quot schemes for those Hilbert polynomials have images missing the generic point: after removal of torsion, a negative-degree coherent quotient there would give a negative-degree vector-bundle quotient. Removing those finitely many images proves the same openness assertion directly.

This base has closed points in arbitrarily large characteristics. Take algebraic closures of their residue fields and exclude denominator primes. Retain the notation for the reductions. The curve γ\gamma continues to pair nonnegatively with every effective divisor: pull that divisor back under the fixed birational morphism and intersect with its fixed ample divisors. This tests effective divisors on the reduction itself. No specialization of a characteristic-zero effective cone is used.

Lemma 6.2. For a sufficiently large residual characteristic pp, set

Np=⌊p/k0⌋,Bp=k0NpD+T0.N_p=\lfloor p/k_0\rfloor,\qquad B_p=k_0N_pD+T_0.

The sections of pqξ+Bp,1+Bp,2pq\xi+B_{p,1}+B_{p,2} generate jets through order (2n+2)k0Np(2n+2)k_0N_p at z∗z_*. In particular, they surject onto the quotient of its local ring by the pp-th powers of all regular parameters. Proof. Multiply NpN_p copies of the fixed jet system. Every monomial of total degree at most (2n+2)k0Np(2n+2)k_0N_p is a product of NpN_p monomials of degree at most (2n+2)k0(2n+2)k_0. Taking sections with those leading monomials gives a triangular system, ordered by total degree. Starting at degree zero and removing the error in each successive degree proves the required jet surjection. This argument takes place in the local ring and never divides by factorials.

Put dp=(p−k0Np)qd_p=(p-k_0N_p)q, so 0≤dp≤(k0−1)q0\leq d_p\leq(k_0-1)q. Among the sections fixed before reduction, choose

u0∈H0(W,OW(T0)),vdp∈H0(W,OW(T0+dpS))u_0\in H^0(W,\mathcal{O}_W(T_0)),\qquad v_{d_p}\in H^0(W,\mathcal{O}_W(T_0+d_pS))

nonzero at the first and second base coordinates of z∗z_*, respectively. Their tensor product belongs to the summand of first-slot weight zero in the projective-bundle formula; its fiber monomial is the dpd_p-th power of the second coordinate. It defines a section of dpξ+T0,1+T0,2d_p\xi+T_{0,1}+T_{0,2} nonzero at z∗z_*, since z∗z_* lies off both axes. Multiplying the product jet system by this section changes its divisor from Npk0MN_pk_0M to pqξ+Bp,1+Bp,2pq\xi+B_{p,1}+B_{p,2}. Multiplication is invertible on the local jet algebra. Only the finitely many previously fixed values of dpd_p occur.

Since dim⁡Z=2n+1\dim Z=2n+1, the quotient by the pp-th powers of regular parameters has top total degree (2n+1)(p−1)(2n+1)(p-1). For large pp this is at most (2n+2)k0Np(2n+2)k_0N_p. The underlying ordinary/Frobenius ideal comparison is also recorded in [26], proof of Proposition 2.12, eq:2.8.

Full rank from the two-slot jets

Let F:W→W′F:W\to W' be relative Frobenius to the base-field twist. It is finite flat because WW is smooth. Write S′S' for the twist of SS, so F∗S′=pSF^*S'=pS, and define

E=F∗OW(Bp),s=rk⁡E=pn,R=s2.\mathcal{E}=F_*\mathcal{O}_W(B_p),\qquad s=\operatorname{rk}\mathcal{E}=p^n,\qquad R=s^2.

For integers 0≤a≤q0\leq a\leq q, put Ua=H0(W,OW(Bp+paS))U_a=H^0(W,\mathcal{O}_W(B_p+paS)). Projection formula gives an evaluation map on W′×W′W'\times W':

⨁a+b=qa,b≥0Ua⊗Ub⊗O(−aS1′−bS2′)⟶E⊠E.(25)\bigoplus_{\substack{a+b=q\\a,b\geq0}}U_a\otimes U_b\otimes\mathcal{O}(-aS'_1-bS'_2)\longrightarrow\mathcal{E}\boxtimes\mathcal{E}. \tag*{(25)}

Lemma 6.3. The map in (25) has generic rank RR.

Proof. Trivialize the two summands defining ZZ near the selected base points. Let zz be the torus coordinate, whose value at z∗z_* is z0≠0z_0\ne0. By the projective-bundle formula, the sections in Lemma 6.2 are weight polynomials in zz with weight-jj coefficients in

H0(W,Bp+jS)⊗H0(W,Bp+(pq−j)S),0≤j≤pq.H^0(W,B_p+jS)\otimes H^0(W,B_p+(pq-j)S),\qquad0\leq j\leq pq.

Let A∗A_* be the tensor product of the local algebras of the two base Frobenius fibers. The local quotient in Lemma 6.2 is

A∗[z]/(zp−z0p),A_*[z]/(z^p-z_0^p),

free over A∗A_* with basis 1,z,…,zp−11,z,\ldots,z^{p-1}. Project to the coefficient of 11 in this basis. Exactly the weights j=paj=pa survive, with multipliers z0paz_0^{pa}. Their coefficients are the values of the corresponding summands of (25), in the chosen frames and the induced twisted frames. As the full jet map is surjective, these coefficients span A∗A_*, of dimension p2n=Rp^{2n}=R. Thus the evaluation has full rank at this pair of base points, and hence generically. The calculation uses a basis over the possibly nonreduced algebra A∗A_*, so reducedness of the Frobenius fibers is unnecessary.

The jet calculation at z∗z_* proves generic full rank; the diagonal estimate below will be tested at (x′,x′)(x',x'), obtained from the separately fixed point xx.

Sections on the Frobenius diagonal

The Frobenius fiber product has the cartesian square

ΔF=W×W′W→pr⁡2Wpr⁡1↓↓FW→FW′(26)\begin{CD} \Delta_F = W \times_{W'} W @>{\operatorname{pr}_2}>> W \\ @V{\operatorname{pr}_1}VV @VV{F}V \\ W @>{F}>> W' \tag*{(26)} \end{CD}

Its reduced subscheme is the diagonal WW. Put

Lp=OΔF(Bp,1+Bp,2+pqS1).\mathcal{L}_p = \mathcal{O}_{\Delta_F}(B_{p,1} + B_{p,2} + pqS_1).

Write h=F∘pr⁡1=F∘pr⁡2:ΔF→W′h = F \circ\operatorname{pr}_1 = F \circ\operatorname{pr}_2 : \Delta_F \to W'. On this fiber product,

O(pS1)≃h∗OW′(S′)≃O(pS2).\mathcal{O}(pS_1) \simeq h^*\mathcal{O}_{W'}(S') \simeq\mathcal{O}(pS_2).

Consequently every pair of weights a+b=qa+b=q gives the same line bundle:

OΔF(Bp,1+Bp,2+paS1+pbS2)≃Lp.\mathcal{O}_{\Delta_F}(B_{p,1} + B_{p,2} + paS_1 + pbS_2) \simeq\mathcal{L}_p.

On the diagonal of W′×W′W' \times W', every source twist of (6.4) becomes −qS′-qS'. Finite base change and projection formula identify the twisted target as

(E⊗E)(qS′)≃h∗Lp.(\mathcal{E} \otimes\mathcal{E})(qS') \simeq h_*\mathcal{L}_p.

The product sections defining the columns restrict to global sections of this one bundle Lp\mathcal{L}_p. Their values at a diagonal point therefore lie in the image of H0(ΔF,Lp)H^0(\Delta_F,\mathcal{L}_p) in the corresponding fiber of h∗Lph_*\mathcal{L}_p. This proves that the rank at every diagonal point is at most

h0(ΔF,Lp).(27)h^0(\Delta_F,\mathcal{L}_p). \tag*{(27)}

For a rank-nn bundle VV in characteristic pp, denote by Aj(V)A_j(V) the degree-jj part of its symmetric algebra modulo the pp-th powers of local generators. This construction is independent of frame: the pp-th power of a linear combination is the sum of the pp-th powers in characteristic pp. Each Aj(V)A_j(V) is locally free and a quotient of V⊗jV^{\otimes j}. Set

u=n(p−1),ej=rk⁡Aj(V),∑j=0uej=pn.u = n(p-1), \qquad e_j = \operatorname{rk} A_j(V), \qquad\sum_{j=0}^{u} e_j = p^n.

Filtering Lp\mathcal{L}_p by powers of the ideal of the reduced diagonal in ΔF\Delta_F gives the graded bundles

Gj=OW(2Bp+pqS)⊗Aj(ΩW1),0≤j≤u.(28)\mathcal{G}_j = \mathcal{O}_W(2B_p + pqS) \otimes A_j(\Omega_W^1), \qquad0 \leq j \leq u. \tag*{(28)}

Indeed, in smooth local coordinates the algebra is generated by parameter differences with their pp-th powers zero, and its degree-one conormal is ΩW1\Omega_W^1. This coordinate calculation can be made étale locally or in completions and identifies the global associated graded. This is the diagonal-ideal form of the canonical Frobenius filtration [18]. The same calculation, using only the bundle from the second factor, filters F∗EF_*\mathcal{E} with pieces [30]

OW(Bp)⊗Aj(ΩW1).(29)\mathcal{O}_W(B_p) \otimes A_j(\Omega_W^1). \tag*{(29)}

Complementary multiplication is a perfect pairing, giving

Au−j(V)≃Aj(V)∨⊗(det⁡V)p−1.A_{u-j}(V) \simeq A_j(V)^\vee\otimes(\det V)^{p-1}.

On monomials, each exponent vector pairs with its complement to (p−1,…,p−1)(p-1,\ldots,p-1). The top line transforms by the character (det⁡V)p−1(\det V)^{p-1}: this is immediate on diagonal matrices and hence identifies the character of GLn\mathrm{GL}_n on that line.

A uniform bound for the diagonal rank

We bound the sections of every graded bundle in (28) by its rank times the same scalar polynomial in pp. This uniformity lets us sum the ranks of the graded pieces without an additional factor for their number. We begin with a slope bound on the fixed curve; here slope means ordinary degree divided by rank.

Lemma 6.4. There is a constant c≥0c \ge0, independent of the sufficiently large residual characteristic pp and of jj, such that for V=ΩW1∣CV = \Omega^1_W|_C one has

μmax⁡(Aj(V))≤(p−1)KW⋅C+nc.\mu_{\max}(A_j(V)) \le(p-1)K_W \cdot C + nc.

Proof. Write FCF_C for absolute Frobenius of CC. Langer’s instability estimate [20] (Corollary 2.5) gives

Lmin⁡(V):=lim⁡e→∞p−eμmin⁡(FCe∗V)≥−cp−1.L_{\min}(V) := \lim_{e\to\infty} p^{-e}\mu_{\min}(F_C^{e*}V) \ge-\frac{c}{p-1}.

To make the uniformity explicit, let gg be the fixed genus of CC. One can choose a nef line bundle ACA_C of degree at most dg=max⁡{4g−2,0}d_g = \max\{4g-2,0\} such that TC⊗ACT_C \otimes A_C is globally generated; for g≤1g \le1, take AC=OCA_C = \mathcal{O}_C. Langer’s bound is

μmin⁡(V)−Lmin⁡(V)≤(rk⁡V−1)deg⁡ACp−1.\mu_{\min}(V) - L_{\min}(V) \le\frac{(\operatorname{rk} V - 1)\deg A_C}{p-1}.

Since rk⁡V=n\operatorname{rk} V = n and μmin⁡(V)≥0\mu_{\min}(V) \ge0, we may take c=(n−1)dgc = (n-1)d_g, independently of the reduction. We also need, for every integer $i \ge 0,

μmin⁡(V⊗i)≥iLmin⁡(V).\mu_{\min}(V^{\otimes i}) \ge iL_{\min}(V).

Fix pp and ii. Choose a line bundle AeA_e of degree −μmin⁡(FCe∗V)+O(1)-\mu_{\min}(F_C^{e*}V)+O(1), rounded up with a fixed genus-dependent additive constant, so that FCe∗V⊗AeF_C^{e*}V \otimes A_e is globally generated. This follows from Serre duality: after subtracting any point, its minimum slope can be made greater than 2g(C)−22g(C)-2, which annihilates H1H^1 and makes evaluation at that point surjective. For every vector-bundle quotient QQ of V⊗iV^{\otimes i}, the bundle FCe∗Q⊗Ae⊗iF_C^{e*}Q \otimes A_e^{\otimes i} is then globally generated. Consequently

peμ(Q)+ideg⁡Ae≥0.p^e\mu(Q) + i\deg A_e \ge0.

Divide by pep^e and let e→∞e \to\infty to prove (6.11). This limit is taken for each fixed p,ip,i; there is no interchange of Frobenius-iteration and characteristic limits.

Since Au−j(V)A_{u-j}(V) is a quotient of V⊗(u−j)V^{\otimes(u-j)}, the perfect pairing (6.9) yields

μmax⁡(Aj(V))=(p−1)deg⁡det⁡V−μmin⁡(Au−j(V))≤(p−1)KW⋅C+(u−j)cp−1≤(p−1)KW⋅C+nc.\begin{aligned} \mu_{\max}(A_j(V)) &= (p-1)\deg\det V - \mu_{\min}(A_{u-j}(V)) \\ &\le(p-1)K_W \cdot C + \frac{(u-j)c}{p-1} \\ &\le(p-1)K_W \cdot C + nc. \end{aligned}

The divisors Bp−pD=T0−(p−k0Np)DB_p-pD=T_0-(p-k_0N_p)D range over a fixed finite list. Combining (24), (6.3), and Lemma 6.4 therefore gives, uniformly for 0≤j≤u0 \le j \le u,

μmax⁡(Gj∣C)≤p(4+2/r)ΛHn+O(1)≤Mp:=7pΛHn+c0,(30)\begin{aligned} \mu_{\max}(G_j|_C) \le p(4+2/r)\Lambda H^n + O(1) \\ &\le M_p := 7p\Lambda H^n+c_0, \tag*{(30)} \end{aligned}

where c0≥0c_0 \ge0 is fixed. The coefficient 77 provides harmless room in this common bound.

Lemma 6.5. For all sufficiently large pp,

h0(ΔF,Lp)≤R(7nHn+O(1/p))<R/4.h^0(\Delta_F,L_p) \le R(7^nH^n+O(1/p)) < R/4.

The error constant is independent of the filtration index jj.

Proof. Write the fixed flag as

W=Wn⊃Wn−1⊃⋯⊃W1=C,Wn−k∈∣hk∣Wn−k+1(1≤k≤n−1).W=W_n\supset W_{n-1}\supset\cdots\supset W_1=C,\qquad W_{n-k}\in|h_k|_{W_{n-k+1}}\quad(1\leq k\leq n-1).

At step kk, fix the preceding nonnegative integers b1,…,bk−1b_1,\ldots,b_{k-1} and put

Fk=Gj∣Wn−k+1(−∑i<kbihi).\mathcal{F}_k=\mathcal{G}_j|_{W_{n-k+1}}\left(-\sum_{i<k}b_i h_i\right).

For each bk≥0b_k\geq0, the divisor restriction sequence is

0⟶Fk(−(bk+1)hk)⟶Fk(−bkhk)⟶Fk(−bkhk)∣Wn−k⟶0.0\longrightarrow\mathcal{F}_k\left(-(b_k+1)h_k\right)\longrightarrow\mathcal{F}_k(-b_kh_k)\longrightarrow\mathcal{F}_k(-b_kh_k)|_{W_{n-k}}\longrightarrow0.

Iterating it for bk=0,1,…b_k=0,1,\ldots and then proceeding to the next member of the flag bounds the section space by

h0(W,Gj)≤∑b1,…,bn−1≥0h0(C,Gj∣C(−∑ibihi∣C)).(31)h^0(W,\mathcal{G}_j)\leq\sum_{b_1,\ldots,b_{n-1}\geq0}h^0\left(C,\mathcal{G}_j|_C\left(-\sum_i b_i h_i|_C\right)\right). \tag*{(31)}

At each stage the remainder is zero after sufficiently negative ample twisting. Its stopping index need not be uniform in jj, pp or in the preceding twists: enlarging the nonnegative finite sums to the displayed lattice sum preserves the inequality.

A summand in (31) vanishes when ∑ibi(hi⋅C)>Mp\sum_i b_i(h_i\cdot C)>M_p, because then its maximum slope is negative. Each nonzero summand has at most ej(Mp+1)e_j(M_p+1) sections. Indeed, evaluation at ⌊Mp⌋+1\lfloor M_p\rfloor+1 distinct points is injective; the kernel has negative maximum slope after subtracting those points. By (6.3) it follows that

h0(W,Gj)≤ej(Mp+1)∏i=1n−1(1+MpliΛHn)=ejpn(7nHn+O(1/p)).(32)\begin{aligned} h^0(W,\mathcal{G}_j)\leq e_j(M_p+1)\prod_{i=1}^{n-1}\left(1+\frac{M_p}{l_i\Lambda H^n}\right) \\ &=e_jp^n\left(7^nH^n+O(1/p)\right). \tag*{(32)} \end{aligned}

The leading coefficient follows from Λ=∏ili\Lambda=\prod_i l_i. More importantly, the whole scalar polynomial on the first line is the same for every jj.

Sum over the filtration in (28). The ranks satisfy ∑jej=pn\sum_j e_j=p^n, so (32) gives the asserted bound with R=p2nR=p^{2n}. There is no extra factor for the number of graded pieces. Finally

7nHn≤(14ϵ)n<1/47^nH^n\leq(14\epsilon)^n<1/4

by (24), proving the strict inequality for all large pp.

The two orders of the determinant

Choose RR generically independent columns of (25) from bases of its source vector spaces. Their determinant is a nonzero section

0≠σ∈H0(W′×W′,Q1⊠Q2)0\neq\sigma\in H^0(W'\times W',Q_1\boxtimes Q_2)

of an actual external-product line bundle. To specify its factors, let mim_i be the sum of the weights of the RR chosen columns in slot ii. The target determinant is (det⁡E)s⊠(det⁡E)s(\det\mathcal{E})^s\boxtimes(\det\mathcal{E})^s, and the chosen source determinant is O(−m1S′)⊠O(−m2S′)\mathcal{O}(-m_1S')\boxtimes\mathcal{O}(-m_2S'). Thus

Qi=(det⁡E)⊗s⊗OW′(miS′),λi=mi/R.Q_i=(\det\mathcal{E})^{\otimes s}\otimes\mathcal{O}_{W'}(m_iS'),\qquad\lambda_i=m_i/R.

Every column weight lies between 00 and qq, so 0≤λi≤q0\leq\lambda_i\leq q independently of the columns chosen.

Under the numerical identification with the base-field twist,

c1(Qi)R=c1(E)s+λiS=Bpp+p−12pKW+λiS,0≤λi≤q.(33)\frac{c_1(Q_i)}{R}=\frac{c_1(\mathcal{E})}{s}+\lambda_iS=\frac{B_p}{p}+\frac{p-1}{2p}K_W+\lambda_iS,\qquad0\leq\lambda_i\leq q. \tag*{(33)}

The Frobenius first-Chern-class identity is also [30]; it is an identity of rational divisor classes. For the second equality, use (29). Complementary degrees in (6.9) have total first Chern class ej(p−1)KWe_j(p-1)K_W. Summing gives

∑jc1(Aj(ΩW1))=s(p−1)2KW.\sum_j c_1\left(A_j\left(\Omega_W^1\right)\right)=\frac{s(p-1)}{2}K_W.

Thus c1(F∗E)=sBp+s(p−1)KW/2c_1(F^*E)=sB_p+s(p-1)K_W/2, and Frobenius pullback of twisted divisor classes multiplies by pp, as required.

For 0≤λ≤q0\leq\lambda\leq q, the fixed movable inequality gives

(D+KW2+λS)⋅γ≤40ϵJ⋅γ.\left(D+\frac{K_W}{2}+\lambda S\right)\cdot\gamma\leq40\epsilon J\cdot\gamma.

where pullback by πx\pi_x is understood. This concerns only intersections of fixed divisors and the fixed complete-intersection witness, so it remains true on the reduction. The class in (33) differs from its left-hand divisor at λ=λi\lambda=\lambda_i by

1p(Bp−pD−KW2).\frac{1}{p}\left(B_p-pD-\frac{K_W}{2}\right).

Its numerator belongs to the fixed finite list T0−aD−KW/2T_0-aD-K_W/2, a∈{0,…,k0−1}a\in\{0,\ldots,k_0-1\}. The resulting error after intersection with γ\gamma is therefore O(p−1)O(p^{-1}), uniformly over the selected determinant columns.

Let x′x' be the twisted point and let 0≠τi∈H0(W′,Qi)0\ne\tau_i\in H^0(W',Q_i). The strict transform of its effective divisor on the blowup at x′x' pairs nonnegatively with the twist of γ\gamma. Since J⋅γ>0J\cdot\gamma>0, it follows that

ord⁡x′(τi)R≤40ϵ+O(1/p).(34)\frac{\operatorname{ord}_{x'}(\tau_i)}{R}\leq40\epsilon+O(1/p). \tag*{(34)}

The constant is uniform in the columns and in τi\tau_i. This argument tests sections on the reduction itself; it does not require them to lift to characteristic zero.

Künneth identifies the space containing σ\sigma with H0(W′,Q1)⊗H0(W′,Q2)H^0(W',Q_1)\otimes H^0(W',Q_2). Choose bases adapted to the orders of vanishing at x′x' in each factor. In each degree their leading terms are linearly independent. Tensor products of these leading terms remain independent in each bidegree of the two disjoint sets of parameters; terms of different bidegrees cannot cancel. Every nonzero tensor consequently has order at most the sum of the two maximum basis orders. Applying (34), we obtain

ord⁡(x′,x′)σ≤R(80ϵ+O(1/p)).(35)\operatorname{ord}_{(x',x')}^\sigma\leq R(80\epsilon+O(1/p)). \tag*{(35)}

On the other hand, (27) and Lemma 6.5 bound the matrix rank at (x′,x′)(x',x') by a number strictly smaller than R/4R/4. Trivialize its line bundles near that point. Invertible constant row operations make more than 3R/43R/4 rows vanish at the point. Each entry of those rows belongs to the maximal ideal, so every term of the determinant has order at least 3R/43R/4. Therefore

ord⁡(x′,x′)σ≥3R/4.(36)\operatorname{ord}_{(x',x')}^\sigma\geq3R/4. \tag*{(36)}

Equations (35) and (36) contradict 80ϵ<3/480\epsilon<3/4 for sufficiently large pp.

This contradiction proves Theorem 6.1. The full-rank calculation used z∗z_*, while the diagonal estimate holds at every point and was tested at the separately chosen xx. The errors were controlled by one fixed finite list of divisor classes and one fixed flag polynomial. Thus their constants do not depend on pp, the filtration index, or the chosen columns.

Application to the terminal case

We return to Theorem 5.1. Thus XX is a projective terminal Q\mathbb{Q}-factorial variety of dimension n≥2n \ge2 with KX∼0K_X \sim0, and LL is a nef Cartier divisor of full nef dimension. Assume that LL is not big. Recall the ample rational divisors P=r(L+tA)P = r(L + tA), where AA is a fixed ample Cartier divisor and t>0t > 0 tends to zero, with

r⟶∞,Pn⟶ϵn,ρ=(Pn)1/n.r \longrightarrow\infty,\qquad P^n \longrightarrow\epsilon^n,\qquad\rho= (P^n)^{1/n}.

The positive rational number ϵ\epsilon was chosen so that (14ϵ)n<1/4(14\epsilon)^n < 1/4 and 80ϵ<3/480\epsilon< 3/4. Choose the integer qq supplied by Proposition 5.3, and then choose tt sufficiently small that this proposition and Lemma 5.2 apply, that r>q+1r > q + 1, and that Pn<(2ϵ)nP^n < (2\epsilon)^n. We now fix tt, and therefore also PP, rr, ρ\rho and the projective bundle in (5.6). Every remaining choice is made over C\mathbb{C} before reducing to positive characteristic.

The divisors and the flag. Choose a smooth projective resolution w:W→Xw : W \to X and set

D=w∗P,S=w∗L,H0=w∗P.D = w^*P,\qquad S = w^*L,\qquad H_0 = w^*P.

The divisor SS is integral Cartier, and H0H_0 is nef and big. Since XX is terminal and KX∼0K_X \sim0, there is an integral effective ww-exceptional divisor EE with KW∼EK_W \sim E. The projection formula and the nefness of P−rLP - rL give

KWH0n−1=0,(2D+qS)H0n−1≤(2+q/r)H0n.K_W H_0^{n-1} = 0,\qquad(2D + qS)H_0^{n-1} \le(2 + q/r)H_0^n.

At H0H_0, the inequalities KWH0n−1<2H0n/rK_W H_0^{n-1} < 2H_0^n/r and (2D+qS)H0n−1<4H0n(2D + qS)H_0^{n-1} < 4H_0^n are strict. Thus, by continuity of intersection products, a sufficiently small rational ample perturbation H=H0+ηAWH = H_0 + \eta A_W, with AWA_W an ample Cartier divisor on WW and η>0\eta> 0, satisfies

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

This gives (24).

The canonical divisor of WW is pseudo-effective. Generic semipositivity of the cotangent bundle, originating in [25] and used here in the form [7], Theorem 2.1, together with restriction to sufficiently general complete-intersection curves [24], Theorem 6.1, gives a smooth integral flag with successive divisor classes liHl_iH, for sufficiently large divisible integers lil_i, such that

μmin⁡(ΩW1∣C)≥0.\mu_{\min}(\Omega_W^1|C) \ge0.

This is the flag in Hypothesis (i) of Theorem 6.1.

The finite jet system. On the bundle of (5.6), write R=P1+P2+qξR = P_1 + P_2 + q\xi. The divisor RR is ample: ξ\xi is nef and relatively ample, and P1+P2P_1 + P_2 is the pullback of an ample divisor on X×XX \times X. Proposition 5.3 supplies a smooth point z∗z_* in the complement of the two axes with

ϵ(R;z∗)>2n+2.\epsilon(R; z_*) > 2n + 2.

The point can be chosen over the open set where ww is an isomorphism. Choose a rational number aa strictly between 2n+22n + 2 and ϵ(R;z∗)\epsilon(R; z_*). On the blowup b:Z~→Zb : \widetilde{Z} \to Z at z∗z_*, with exceptional divisor GG, the rational divisor b∗R−aGb^*R - aG is ample. For sufficiently large divisible k0k_0, Serre vanishing gives

H1(Z~,OZ~(k0b∗R−k0aG))=0.H^1(\widetilde{Z},\mathcal{O}_{\widetilde{Z}}(k_0b^*R-k_0aG))=0.

Since z∗z_* is smooth, the sections on the thickened exceptional divisor k0aGk_0aG identify with the jet quotient at z∗z_* modulo mz∗k0a\mathfrak{m}_{z_*}^{k_0a}, in a local frame for k0Rk_0R. The restriction sequence therefore shows that sections of k0Rk_0R generate jets through order k0a−1k_0a-1, and hence through order (2n+2)k0(2n+2)k_0. Increase the divisibility of k0k_0 to make k0Pk_0P Cartier. Pulling these sections to

ZW=P(OW(S)1⊕OW(S)2)⟶W×WZ_W = \mathbb{P}(\mathcal{O}_W(S)_1 \oplus\mathcal{O}_W(S)_2) \longrightarrow W \times W

preserves the jets at the corresponding point, because the induced map ZW→ZZ_W \to Z is an isomorphism near that point. The pulled-back divisor is D1+D2+qξD_1 + D_2 + q\xi. We have obtained the finite system required in Hypothesis (ii).

The movable curve class. Choose a very general point x∈Wx \in W outside the exceptional locus, with image in the locus where Lemma 5.2 holds. Let πx:W^→W\pi_x:\widehat{W}\to W be its blowup and JJ its exceptional divisor. The rational divisor

D+=2D+ED^{+}=2D+E

is big. For every sufficiently divisible positive integer mm, normality of XX and exceptionality of EE give w∗OW(mE)=OXw_*\mathcal{O}_W(mE)=\mathcal{O}_X. Thus every section of mD+mD^{+} comes from a section of 2mP2mP, multiplied by the section of the fixed divisor mEmE. Since x∉Supp⁡Ex\notin\operatorname{Supp}E, Lemma 5.2 implies

ord⁡x(s)/m≤8ρ<16ϵ(0≠s∈H0(W,OW(mD+))).(37)\operatorname{ord}_x(s)/m\leq8\rho<16\epsilon\qquad(0\neq s\in H^0(W,\mathcal{O}_W(mD^{+}))). \tag*{(37)}

It follows that

πx∗D+−40ϵJ is not pseudo-effective.(38)\pi_x^*D^{+}-40\epsilon J\ \text{is not pseudo-effective.} \tag*{(38)}

Indeed, if it were pseudo-effective, a convex combination with the big divisor πx∗D+\pi_x^*D^{+} would make πx∗D+−cJ\pi_x^*D^{+}-cJ big for any rational cc with 16ϵ<c<40ϵ16\epsilon<c<40\epsilon. A nonzero section of a sufficiently divisible multiple would then give a section violating (6.19).

By the duality between pseudo-effective divisors and strongly movable curves [6], the strict separation in (6.20) is detected by a class

γ=f∗(A1⋯An−1),f:V⟶W^,\gamma=f_*(A_1\cdots A_{n-1}),\qquad f:V\longrightarrow\widehat{W},

where VV is smooth projective, ff is birational, and the AiA_i are ample integral Cartier divisors. To obtain this form, first choose a generating strongly movable class with negative pairing, then approximate its ample real classes by rational ones and clear denominators. We have

(πx∗D+)⋅γ<40ϵJ⋅γ.(\pi_x^*D^{+})\cdot\gamma<40\epsilon J\cdot\gamma.

The left side is nonnegative, because πx∗D+\pi_x^*D^{+} is pseudo-effective, so J⋅γ>0J\cdot\gamma>0.

For every 0≤λ≤q0\leq\lambda\leq q,

D+−(D+KW/2+λS)∼Rw∗(P−λL)+E/2D^{+}-(D+K_W/2+\lambda S)\sim_{\mathbb{R}}w^*(P-\lambda L)+E/2

is pseudo-effective: P−λL=(P−rL)+(r−λ)LP-\lambda L=(P-rL)+(r-\lambda)L is nef and EE is effective. Pulling back to W^\widehat{W} and pairing with γ\gamma therefore gives

πx∗(D+KW/2+λS)⋅γ≤(πx∗D+)⋅γ<40ϵJ⋅γ.\pi_x^*(D+K_W/2+\lambda S)\cdot\gamma\leq(\pi_x^*D^{+})\cdot\gamma<40\epsilon J\cdot\gamma.

This proves Hypothesis (iii). All the hypotheses of Theorem 6.1 now hold for one fixed collection of complex data, a contradiction. Hence LL is big, completing the proof of Theorem 5.1.

Completion of the full-dimension induction

Theorem 5.1 treats varieties with terminal singularities and linearly trivial canonical divisor. We now pass to klt Calabi–Yau pairs and complete the full-dimension assertion. The boundary perturbation below follows the reduction in [22], Section 7: an effective representative of a small boundary perturbation plus the nef divisor allows ordinary log abundance to be applied to a multiple of that nef divisor.

Proposition 7.1. Let n≥2n\geq2, and assume (Pj)(P_j) for every j<nj<n, together with Theorems 2.2 and 2.3. Let (X,B)(X,B) be a projective klt Q\mathbb{Q}-pair over C\mathbb{C} of dimension nn, and let MM be a nef Q\mathbb{Q}-Cartier divisor on XX. Suppose that T=KX+BT=K_X+B is pseudo-effective and that, for some rational a>0a>0,

(T+aM)⋅C>0(T+aM)\cdot C>0

for every integral curve CC through a very general point of XX. Then T+cMT+cM is big for every rational c>0c>0. Proof. Proposition 3.3 proves the assertion when κ(T)>0\kappa(T)>0. Proposition 3.4 reduces the remaining case to the following claim in dimension nn:

(X,B) projective klt,KX+B≡0,M nef and Q-Cartier of full nef dimension⟹M big.(39)\begin{aligned} &(X,B)\text{ projective klt},\qquad K_X+B\equiv0,\\ &M\text{ nef and $\mathbb{Q}$-Cartier of full nef dimension}\quad\Longrightarrow\quad M\text{ big}. \tag*{(39)} \end{aligned}

We prove this claim first with B=0B=0 and then with arbitrary boundary. We may take a small projective Q\mathbb{Q}-factorialization throughout: the adjoint and MM pull back, full nef dimension is preserved on the isomorphism locus, and bigness of the pullback implies bigness downstairs.

The case of zero boundary. Suppose that XX is klt and KX≡0K_X\equiv0. Theorem 2.2 makes KXK_X semiample, hence KX∼Q0K_X\sim_{\mathbb Q}0. Indeed, a semiample numerically trivial divisor defines a morphism with zero-dimensional image, so a sufficiently divisible multiple is linearly trivial. Take the global index-one cover

π:Xind⟶X\pi:X^{\mathrm{ind}}\longrightarrow X

associated with a trivialization of the smallest positive multiple of KXK_X that is linearly trivial. This is a finite quasi-étale cover, and

KXind=π∗KX∼0.K_{X^{\mathrm{ind}}}=\pi^*K_X\sim0.

The cover is klt. Since its canonical divisor is Cartier, its log discrepancies are positive integers, hence at least one; it therefore has canonical singularities. These are the standard index-one cover properties for klt varieties; see [19], Definition 5.19 and Proposition 5.20. By the crepant terminalization theorem [3], Corollary 1.4.3, there is a projective birational morphism

h:X~⟶Xindh:\widetilde X\longrightarrow X^{\mathrm{ind}}

with X~\widetilde X terminal and Q\mathbb{Q}-factorial and KX~=h∗KXindK_{\widetilde X}=h^*K_{X^{\mathrm{ind}}}. In particular, KX~K_{\widetilde X} is Cartier and linearly trivial, as required by Theorem 5.1.

Set M~=(π∘h)∗M\widetilde M=(\pi\circ h)^*M. This divisor is nef and has full nef dimension. To verify the latter assertion, choose a very general point upstairs outside the exceptional locus of hh and above the very general locus used for MM. Every curve through this point has a curve as its image in XX, and the projection formula gives strictly positive M~\widetilde M-degree. A positive Cartier multiple of M~\widetilde M is therefore big by Theorem 5.1. Bigness is detected by a dominant generically finite pullback, so MM is big on XX.

Introducing the boundary. Now let (X,B)(X,B) satisfy the hypotheses of (7.1), with B≠0B\ne0. Theorem 2.2 gives

KX+B∼Q0.K_X+B\sim_{\mathbb Q}0.

Choose a rational α>0\alpha>0 sufficiently small that (X,(1+α)B)(X,(1+\alpha)B) remains klt, and put

T∗=KX+(1+α)B∼QαB.T_* = K_X+(1+\alpha)B\sim_{\mathbb Q}\alpha B.

Thus T∗T_* is pseudo-effective and κ(T∗)≥0\kappa(T_*)\ge0. The full condition holds for T∗T_* and MM: for a curve CC through a point outside Supp⁡B\operatorname{Supp}B, we have T∗⋅C=αB⋅C≥0T_*\cdot C=\alpha B\cdot C\ge0, whereas M⋅C>0M\cdot C>0 if that point is very general. We will show that T∗+MT_*+M is big without using the conclusion of the present proposition.

If κ(T∗)>0\kappa(T_*)>0, this follows from Proposition 3.3. Suppose instead that κ(T∗)=0\kappa(T_*)=0, and apply Lemma 3.2 to (X,(1+α)B)(X,(1+\alpha)B) and MM. Write YY for its final model, BYB_Y and NN for the transforms of BB and MM, and

U=KY+(1+α)BY.U=K_Y+(1+\alpha)B_Y.

The output has U∼Q0U\sim_{\mathbb Q}0 and, for some rational s>0s>0, the divisor U+sNU+sN is nef of full nef dimension. The maps in the construction extract no divisors, so pushing forward the rational linear equivalence KX+B∼Q0K_X+B\sim_{\mathbb Q}0 also gives

KY+BY∼Q0.K_Y+B_Y\sim_{\mathbb Q}0.

Subtracting these two equivalences shows that αBY∼Q0\alpha B_Y \sim_{\mathbb{Q}} 0. Since BYB_Y is effective on a projective variety, intersection with a sufficiently ample complete-intersection curve forces BY=0B_Y = 0. The ordinary pair on YY is therefore klt with zero boundary and KY∼Q0K_Y \sim_{\mathbb{Q}} 0. Moreover, NN is nef of full nef dimension, because U+sN≡sNU + sN \equiv sN. The zero-boundary case just proved makes NN, and hence U+sNU + sN, big.

On a common smooth resolution, with maps pp to XX and qq to YY, the effective exceptional comparison from the reduction is

p∗(T∗+sM)=q∗(U+sN)+E,E≥0.p^*(T_* + sM) = q^*(U + sN) + E,\qquad E \ge0.

It follows that T∗+sMT_* + sM is big. Choose a positive rational λ\lambda with λ<min⁡{1,1/s}\lambda< \min\{1,1/s\}. Then

T∗+M=λ(T∗+sM)+(1−λ)T∗+(1−λs)MT_* + M = \lambda(T_* + sM) + (1 - \lambda)T_* + (1 - \lambda s)M

is big, since the first summand is big and the other two are pseudo-effective. We have thus established bigness of T∗+MT_* + M in both cases.

Choose an effective Q\mathbb{Q}-divisor GG with

G∼QT∗+M∼QαB+M.G \sim_{\mathbb{Q}} T_* + M \sim_{\mathbb{Q}} \alpha B + M.

For a sufficiently small rational u>0u > 0, the divisor

Δu=(1−uα)B+uG\Delta_u = (1 - u\alpha)B + uG

is effective and (X,Δu)(X,\Delta_u) is klt. To see this explicitly, take uα<1u\alpha< 1 and choose uu small enough that (X,B+uG)(X,B + uG) is klt on a fixed log resolution; then Δu≤B+uG\Delta_u \le B + uG. Its adjoint satisfies

KX+Δu∼QKX+B+u(G−αB)∼QuM.K_X + \Delta_u \sim_{\mathbb{Q}} K_X + B + u(G - \alpha B) \sim_{\mathbb{Q}} uM.

This adjoint is nef, so Theorem 2.2 makes it semiample. Consequently MM itself is semiample. The morphism given by a free multiple of MM has zero-dimensional general fiber: a positive-dimensional fiber through a very general point would contain a curve of MM-degree zero, contrary to full nef dimension. That morphism is therefore generically finite onto its image, and MM is big. This proves (7.1) for all klt Calabi–Yau pairs. Proposition 3.4 now supplies the case κ(T)=0\kappa(T) = 0, while Proposition 3.3 supplies κ(T)>0\kappa(T) > 0. These exhaust the possibilities furnished by the minimal-model and abundance inputs for a pseudo-effective klt adjoint, and establish the proposition. □

Positive parts and numerical semiampleness

We complete the simultaneous induction by proving the following positive-part statement.

Proposition 8.1. For every projective klt Q\mathbb{Q}-pair (X,B)(X,B) over C\mathbb{C} with KX+BK_X + B pseudo-effective and every nef Q\mathbb{Q}-Cartier divisor MM on XX, there is a smooth projective birational model w:W→Xw: W \to X such that

Pσ(w∗(KX+B+M))P_\sigma\bigl(w^*(K_X + B + M)\bigr)

is rational and numerically equivalent to a semiample Q\mathbb{Q}-divisor.

For the inductive step, fix such (X,B)(X,B) and MM with dim⁡X=n≥2\dim X = n \ge2, and put T=KX+BT = K_X + B. We assume (Zj)(Z_j) for j<nj < n and use (Pn)(P_n) from Proposition 7.1. Following the positive-part method of Lazić–Peternell [22], we first make a sufficiently large adjoint nef. Full nef dimension then gives bigness by (Pn)(P_n); otherwise its nef reduction permits the nef summand to descend to a lower-dimensional base.

Positive parts under the required comparisons

We will repeatedly use the following properties of Nakayama’s divisorial Zariski decomposition [27].

Lemma 8.2. The following assertions hold.

(1) Let p:V→Xp: V \to X be a projective birational morphism from a smooth projective variety to a normal projective variety. If DD is a pseudo-effective Q\mathbb{Q}-Cartier divisor on XX and EE is an effective pp-exceptional rational divisor, then

Pσ(p∗D+E)=Pσ(p∗D).P_{\sigma}(p^*D+E)=P_{\sigma}(p^*D).

(2) Let f:V→Sf: V \to S be a surjective morphism of smooth projective varieties, and let DD be a pseudo-effective rational divisor on SS. If Pσ(D)P_{\sigma}(D) is nef, then

Pσ(f∗D)=f∗Pσ(D).P_{\sigma}(f^*D)=f^*P_{\sigma}(D).

(3) For rational divisors on a fixed smooth projective variety, rationality and numerical semi ampleness of the positive part depend only on the numerical class of the divisor.

Proof. The first two statements are [22], Lemmas 2.4 and 2.5; the first allows the target XX to be normal. For the third, each asymptotic divisorial order σΓ(D)\sigma_{\Gamma}(D) depends only on the numerical class. Thus numerically equivalent divisors have the same negative part as an actual real divisor. For rational D,D′D,D' with D≡D′D \equiv D',

Pσ(D′)−Pσ(D)=D′−D.P_{\sigma}(D')-P_{\sigma}(D)=D'-D.

Consequently one positive part is rational if and only if the other is, and the two positive parts are numerically equivalent.

In particular, a positive part that is rational and numerically semiample is nef, so these properties persist on higher smooth models. Suppose that on a common smooth resolution of a birational contraction one has

p∗D≡q∗D′+E,p^*D \equiv q^*D' + E,

where D,D′D,D' are pseudo-effective rational Cartier divisors and EE is effective and qq-exceptional. If a smooth model over the target has rational numerically semiample positive part for D′D', take a higher common resolution dominating that model. The second part of Lemma 8.2 pulls that positive part to the common resolution. Its first and third parts, applied to (8.1), give the same conclusion for DD. This is the comparison that will be used at each birational step.

An MMP trivial on the nef divisor

Lemma 8.3. Let (X,B)(X,B) be a projective Q\mathbb{Q}-factorial klt Q\mathbb{Q}-pair of dimension nn, with T=KX+BT=K_X+B pseudo-effective, and let LL be a nef Cartier divisor on XX. If mm is an integer greater than 2n2n, there is a terminating (T+mL)(T+mL)-MMP whose every step is LL-trivial and is an ordinary TT-negative step. On its output, the transform of LL is Cartier and nef, and the transform of T+mLT+mL is nef.

Proof. Use Theorem 2.3 for the generalized klt pair whose nef data are mLmL on XX. Its adjoint T+mLT+mL is pseudo-effective. Suppose inductively that on the current model the ordinary pair is klt and the transform, still denoted by LL, is Cartier and nef. Every (T+mL)(T+mL)-negative extremal ray is TT-negative. By the ordinary length bound, it has a rational curve generator CC with 0<−T⋅C≤2n0<-T\cdot C\le2n. If L⋅C>0L\cdot C>0, integrality gives

(T+mL)⋅C≥−2n+m>0,(T+mL)\cdot C\ge-2n+m>0,

which is impossible. Hence L⋅C=0L\cdot C=0.

The Cartier descent statement in the ordinary cone and contraction theorem gives a Cartier divisor on the contraction base whose pullback is LL. It is nef: lift any curve on the base to a curve dominating it and use the projection formula. In a flip its pullback to the flipped variety is therefore again Cartier and nef. The relative signs of T+mLT + mL are those of TT, so the flip is also an ordinary flip for the klt pair. Thus the inductive hypotheses persist. The terminating program supplied by Theorem 2.3 has all the stated properties. □\square

Apply the lemma after a small Q\mathbb{Q}-factorialization, with L=m0ML = m_0M for an integer m0>0m_0 > 0 making LL Cartier. The program is MM-trivial, so on a common resolution its ordinary adjoint comparison also gives

p∗(T+M)=q∗(T′+M′)+E,p^*(T + M) = q^*(T' + M') + E,

where EE is effective and exceptional over the output. The transformed ordinary adjoint T′T' remains pseudo-effective, and M′M' is nef. By (8.1), it suffices to prove (Zn)(Z_n) on that output. We may consequently retain the notation XX, BB, TT, MM, LL and assume in addition that

T+mL is nef.T + mL \text{ is nef}.

The case of full nef dimension

Suppose first that T+mLT + mL has full nef dimension. Then (1) holds, and (Pn)(P_n) shows that T+MT + M is big. Write, by Kodaira’s lemma,

T+M∼QA1+G1,T + M \sim_{\mathbb{Q}} A_1 + G_1,

where A1A_1 is ample and G1≥0G_1 \ge0 is rational. Choose a rational v>0v > 0 sufficiently small that (X,B+vG1)(X, B + vG_1) is klt. Since M+vA1M + vA_1 is ample, a general effective rational representative A′A' of this divisor can be chosen with sufficiently small coefficients that (X,B+vG1+A′)(X, B + vG_1 + A') is klt. Its adjoint satisfies

KX+B+vG1+A′∼Q(1+v)(T+M).(40)K_X + B + vG_1 + A' \sim_{\mathbb{Q}} (1 + v)(T + M). \tag*{(40)}

It is big and has a good minimal model: one may use the big-case theorem of [3], or combine Theorems 2.3 and 2.2. On a common resolution, the left side of (40) is the pullback of a semiample divisor plus an effective exceptional divisor. Its positive part is therefore the semiample pullback. Dividing by 1+v1 + v proves (Zn)(Z_n) in this case.

Descent along a nef reduction

We treat the remaining case, where the nef dimension of T+mLT + mL is strictly smaller than nn. Let

X⇢ZX \dashrightarrow Z

be its nef reduction, with ZZ normal and projective. A very general compact fibre FF is contained in the morphism locus and has positive dimension. On this fibre,

(T+mL)∣F≡0.(T + mL)|_F \equiv0.

The restriction T∣FT|_F is pseudo-effective. To see this, choose effective rational approximations to TT after adding positive ample perturbations tending to zero, and choose FF outside the countably many exceptional choices for these approximations. Their restrictions are effective, and their classes approach T∣FT|_F. After a resolution of FF the same argument applies to the pullbacks. As L∣FL|_F is nef and T∣F≡−mL∣FT|_F \equiv-mL|_F, both divisors are numerically trivial. Indeed, intersect this equality with an ample complete-intersection curve on a smooth resolution of FF. Pseudo-effectivity makes the left side nonnegative and nefness makes the right side nonpositive. Their common value is zero, and a nef divisor with zero intersection against an ample complete-intersection curve is numerically trivial.

Restriction to a sufficiently general fibre gives a klt pair (F,B∣F)(F,B|_F) with adjoint T∣FT|_F. By Theorem 2.2, its numerically trivial adjoint is semiample, hence

KF+B∣F∼Q0.(41)K_F + B|_F \sim_{\mathbb{Q}} 0. \tag*{(41)}

These restrictions are made where the almost holomorphic nef reduction is a morphism. Normality and the klt restriction statement hold after shrinking the base; alternatively they follow by restricting a log resolution over a general smooth open. Numerical triviality, initially obtained for very general fibres, also follows on a general fibre by the constancy of the relevant intersection numbers in this family.

We next use the birational descent of nef divisors [22]. After resolving the nef reduction and modifying its base birationally, it supplies a diagram

X←pX1→fZ1X \xleftarrow{p} X_1 \xrightarrow{f} Z_1

in which X1,Z1X_1,Z_1 are smooth and projective, pp is birational, ff is a contraction, and there is a rational divisor M1M_1 on Z1Z_1 with

p∗M≡f∗M1.p^*M \equiv f^*M_1.

The divisor M1M_1 is nef, since its pullback is numerically equivalent to the nef divisor p∗Mp^*M and nefness descends under a surjective morphism. We may take a further log resolution of the pair on top without affecting (8.5).

Write the crepant boundary as B1+−B1−B_1^+ - B_1^-, with effective rational divisors of disjoint support, so that

KX1+B1+−B1−=p∗(KX+B).K_{X_1}+B_1^+-B_1^-=p^*(K_X+B).

Set B1=B1+B_1=B_1^+ and E=B1−E=B_1^-. Since the original boundary is effective, EE is pp-exceptional. Klt singularities make all coefficients of B1B_1 less than one, and its support is simple normal crossings. Thus (X1,B1)(X_1,B_1) is klt and

KX1+B1=p∗T+E,E≥0.K_{X_1}+B_1=p^*T+E,\qquad E\geq0.

In particular its adjoint is pseudo-effective.

If F1F_1 is a general fibre of ff, it maps birationally onto the corresponding compact fibre FF of the nef reduction. Every component of EE that meets F1F_1 restricts to an exceptional divisor over FF: for a centre dominating the base, codimension at least two is preserved on the general fibre, and the other centres are avoided. Equations (41) and (8.6) therefore show that

κ(F1,(KX1+B1)∣F1)=0.\kappa\left(F_1,(K_{X_1}+B_1)|_{F_1}\right)=0.

The restriction is an effective exceptional divisor up to rational linear equivalence. Equivalently, its section spaces are those of the trivial divisor on the normal fibre FF. In particular the general fibre pair has pseudo-effective adjoint and has a good minimal model by Theorems 2.3 and 2.2.

A relative good model and a lower-dimensional adjoint

At this point the nef summand comes from Z1Z_1, while the ordinary adjoint has Iitaka dimension zero on its general fibres. We use a relative good model to express that ordinary adjoint as a pullback from a variety of dimension less than nn.

The relative log canonical ring of the rational klt pair (X1,B1)(X_1,B_1) over Z1Z_1 is finitely generated. More precisely, for a positive integer rr making r(KX1+B1)r(K_{X_1}+B_1) Cartier, its Veronese algebra

⨁ℓ≥0f∗OX1(ℓr(KX1+B1))\bigoplus_{\ell\geq0} f_*\mathcal{O}_{X_1}\bigl(\ell r(K_{X_1}+B_1)\bigr)

is a finitely generated OZ1\mathcal{O}_{Z_1}-algebra. This is the relative finite-generation theorem for rational klt pairs, in the form [11], obtained from the finite-generation theorem of [3] and the canonical-bundle reduction of Fujino–Mori [14]. Together with the good minimal models of the very general closed fibres established above, this verifies both hypotheses of [16]. That theorem gives a good minimal model over Z1Z_1; the termination statement for an MMP with scaling once a good model exists, [16], supplies a relative program

(X1,B1)⇢(X2,B2).(X_1,B_1)\dashrightarrow(X_2,B_2).

Thus X2X_2 is projective and Q\mathbb{Q}-factorial, (X2,B2)(X_2,B_2) is klt, and KX2+B2K_{X_2}+B_2 is semiample over Z1Z_1. This application uses very general closed fibres over C\mathbb{C} and requires no change of the ground field to a geometric generic field.

By (8.5), we may replace the nef term numerically by f∗M1f^*M_1 before making the positive-part comparisons. This pullback is trivial on every step of the relative program and is carried unchanged from the base. The ordinary adjoint remains pseudo-effective by numerical pushforward.

Let

X2→gZ2→jZ1X_2 \xrightarrow{g} Z_2 \xrightarrow{j} Z_1

be the relative semiample fibration of KX2+B2K_{X_2}+B_2, with gg a contraction. Its construction gives a jj-ample Q\mathbb{Q}-Cartier divisor A2A_2 on Z2Z_2 such that

KX2+B2∼Qg∗A2.(42)K_{X_2}+B_2 \sim_{\mathbb{Q}} g^*A_2. \tag*{(42)}

The relative program preserves Iitaka dimension on the general fibres, by its effective exceptional pullback comparisons. From (8.7), the relative Iitaka dimension is zero. Hence

dim⁡Z2=dim⁡Z1<n.\dim Z_2=\dim Z_1<n.

Apply Ambro’s canonical bundle formula consequence [1] to (8.8). Its hypotheses hold: (X2,B2)(X_2,B_2) is a projective klt pair with effective rational boundary, gg is a contraction to a normal projective variety, and the ordinary adjoint is rationally linearly pulled back from a Q\mathbb{Q}-Cartier divisor. It gives an effective rational boundary BZ2B_{Z_2} such that (Z2,BZ2)(Z_2,B_{Z_2}) is klt and

KX2+B2∼Qg∗(KZ2+BZ2).(43)K_{X_2}+B_2\sim_{\mathbb{Q}}g^*(K_{Z_2}+B_{Z_2}). \tag*{(43)}

The base adjoint is pseudo-effective. One direct verification, using only the inputs already in force, is as follows. The pseudo-effective ordinary adjoint on X2X_2 has a good minimal model by Theorems 2.3 and 2.2; it therefore has a nonzero section in a sufficiently divisible positive multiple. Since g∗OX2=OZ2g_*\mathcal{O}_{X_2}=\mathcal{O}_{Z_2}, the projection formula and (8.9) identify this section space with the corresponding section space on Z2Z_2. Thus KZ2+BZ2K_{Z_2}+B_{Z_2} even has an effective rationally linearly equivalent divisor.

We are now in the setting of (Zdim⁡Z2)(Z_{\dim Z_2}): the pair on the base is klt with pseudo-effective adjoint, and j∗M1j^*M_1 is a nef rational Cartier divisor. There is consequently a smooth projective birational model w2:W2→Z2w_2:W_2\to Z_2 on which

Pσ(w2∗(KZ2+BZ2+j∗M1))P_{\sigma}\bigl(w_2^*(K_{Z_2}+B_{Z_2}+j^*M_1)\bigr)

is rational and numerically semiample. Resolve the main component of X2×Z2W2X_2\times_{Z_2}W_2 to obtain a smooth projective variety VV mapping birationally to X2X_2 and surjectively to $W_2. Since the displayed positive part is nef, the pullback formula of Lemma 8.2, together with (8.9), proves the same positive-part assertion on VV for

KX2+B2+g∗j∗M1.K_{X_2}+B_2+g^*j^*M_1.

Take a common resolution dominating both VV and X1X_1. The relative MMP compares KX1+B1K_{X_1}+B_1 with KX2+B2K_{X_2}+B_2 by adding an effective divisor exceptional over X2X_2. The M1M_1 terms have equal pullbacks, since they come from the relative base. The comparison (8.1) therefore proves the positive-part assertion on a smooth model over X1X_1 for KX1+B1+f∗M1K_{X_1}+B_1+f^*M_1. Finally, (8.5) and (8.6) give

KX1+B1+f∗M1=p∗(T+M)+E,K_{X_1}+B_1+f^*M_1=p^*(T+M)+E,

where EE is effective and pp-exceptional. Another application of Lemma 8.2 proves (Zn)(Z_n) on a smooth model over the original XX.

Completion of the proof of Proposition 8.1. The preceding argument proves (Zn)(Z_n) from (Pn)(P_n) and the lower-dimensional assertions. Together with Proposition 7.1 and the dimension-zero and dimension-one cases, it completes the simultaneous induction. ∺ես

Descent to the original variety

The positive-part statement is birational, whereas the main theorem requires a semiample representative on the original variety. The following descent uses the rational singularities of klt pairs; it is the numerical semiampleness statement of [22].

Lemma 8.4. Let p:W→Xp: W \to X be a projective birational morphism from a smooth projective variety to a normal projective variety with rational singularities, over C\mathbb{C}. Let DD be a Q\mathbb{Q}-Cartier divisor on XX. If p∗Dp^{*}D is numerically equivalent to a semiample Q\mathbb{Q}-divisor on WW, then DD is numerically equivalent to a semiample Q\mathbb{Q}-Cartier divisor on XX.

Proof. Choose a semiample rational divisor AWA_W with AW≡p∗DA_W \equiv p^{*}D. After clearing denominators, the difference of the corresponding line bundles is numerically trivial. Numerically trivial line bundles modulo Pic⁡0(W)\operatorname{Pic}^{0}(W) are torsion. Thus, after increasing a positive integer rr, we have

OW(rAW)≃p∗OX(rD)⊗PWwith PW∈Pic⁡0(W).\mathcal{O}_W(rA_W) \simeq p^{*}\mathcal{O}_X(rD) \otimes P_W \quad\text{with } P_W \in\operatorname{Pic}^{0}(W).

Rational singularities identify Pic⁡0(X)\operatorname{Pic}^{0}(X) with Pic⁡0(W)\operatorname{Pic}^{0}(W) by pullback. Write PW=p∗PXP_W = p^{*}P_X and set AX=OX(rD)⊗PXA_X = \mathcal{O}_X(rD) \otimes P_X. Then p∗AX≃OW(rAW)p^{*}A_X \simeq\mathcal{O}_W(rA_W).

A positive power of the line bundle on the right is globally generated. Since p∗OW=OXp_{*}\mathcal{O}_W = \mathcal{O}_X, the projection formula identifies its sections with those of the same power of AXA_X. These sections generate downstairs: a failure at any point of XX would remain a failure at every point above it. Hence AXA_X is semiample. A Cartier divisor representing AXA_X, divided by rr, is semiample and numerically equivalent to DD, because PXP_X is algebraically trivial. □\square

We can now prove Theorem 1.1 over C\mathbb{C}. Its divisor D=KX+B+MD = K_X + B + M is nef, so

Pσ(w∗D)=w∗DP_{\sigma}(w^{*}D) = w^{*}D

on every smooth birational model. Proposition 8.1 makes this pullback numerically semiample. A klt variety has rational singularities, so Lemma 8.4 gives the required semiample rational Cartier divisor on XX.

Algebraically closed fields of characteristic zero

We finish by transferring the result to the ground fields in the statement of Theorem 1.1. The very general points used in the proof were needed only over C\mathbb{C}; numerical semiampleness itself descends by a finite-type parameter argument.

Lemma 8.5. Let k0⊂Kk_0 \subset K be an extension of algebraically closed fields of characteristic zero. Let X0X_0 be a normal projective variety over k0k_0, and let D0D_0 be a Q\mathbb{Q}-Cartier divisor. If its pullback DKD_K to XKX_K is numerically equivalent to a semiample Q\mathbb{Q}-Cartier divisor, then D0D_0 has that property over k0k_0.

Proof. Clear denominators in D0D_0 and in a semiample representative over KK, and take a further multiple which is globally generated. Its difference from the corresponding multiple of DKD_K is numerically trivial. After another positive multiple this difference belongs to Pic⁡0(XK)\operatorname{Pic}^{0}(X_K), since numerical triviality modulo Pic⁡0\operatorname{Pic}^{0} is torsion. We have therefore fixed an integer r>0r > 0 and a line bundle PK∈Pic⁡0(XK)P_K \in\operatorname{Pic}^{0}(X_K) such that

OXK(rDK)⊗PK\mathcal{O}_{X_K}(rD_K) \otimes P_K

is globally generated.

Choose a k0k_0-point of X0X_0 and rigidify line bundles there. The finite-type scheme Pic⁡0(X0)\operatorname{Pic}^{0}(X_0) then has a Poincaré family. Tensor this family by the fixed line bundle OX0(rD0)\mathcal{O}_{X_0}(rD_0). The set of parameters for which the resulting line bundle is globally generated is constructible. Indeed, stratify the parameter scheme so that the zeroth direct image is locally free and cohomology and base change hold. On each stratum use the evaluation map; the image in the parameter space of the support of its cokernel is closed, because projection from X0X_0 is proper. Its complement is the globally generated locus on that stratum. Formation of the Picard scheme and of this constructible condition commutes with the field extension. The locus is nonempty after extension to KK, by the chosen PKP_K, and is consequently nonempty over k0k_0. As k0k_0 is algebraically closed, it has a k0k_0-point. The corresponding globally generated line bundle, represented by a Cartier divisor and divided by rr, is the desired semiample rational divisor numerically equivalent to D0D_0. □

Completion of the proof of Theorem 1.1. Let kk be the given algebraically closed field of characteristic zero. Descend XX, BB, MM, the required rational Cartier structures, and a projective embedding to a finitely generated subfield of kk. Let k0⊂kk_0 \subset k be its algebraic closure inside kk, and choose an embedding k0↪Ck_0 \hookrightarrow\mathbb{C}.

The hypotheses persist under the resulting algebraically closed field extensions. For klt singularities this follows from a log resolution, which can be included among the descended data. Nefness is invariant under field extension, since it can be tested by ampleness after arbitrarily small rational ample perturbations. Pseudo-effectivity is invariant for the same reason with bigness in place of ampleness: a rational divisor is pseudo-effective exactly when all its positive rational ample perturbations are big, and bigness is preserved and reflected by extension of the section spaces. These tests show both that the descended data satisfy the hypotheses and that their complex extension does.

The result over C\mathbb{C} supplies a semiample numerical representative of KX+B+MK_X + B + M after this extension. Lemma 8.5 descends it to k0k_0. Extending that representative to kk preserves global generation of a suitable multiple and numerical equivalence. It is the required semiample Q\mathbb{Q}-Cartier divisor on the original variety. □

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