Contents

1 Introduction 2

2 Forms, birational maps, and uniform inputs 4

3 The Hodge structure generated by the top forms 7

4 A diagonal estimate for the Hodge rank 9

5 A uniform bound for the top-form Hodge structure 16

6 Uniform exponents for klt pluricanonical characters 29

7 Residues and descent across the conductor 34

Introduction

The index of a log Calabi–Yau pair measures the degree in which its rationally trivial log canonical class becomes an actual trivial line bundle. A uniform index theorem asks whether that degree can be chosen from the dimension and the boundary coefficients alone. For a nonnormal pair, this question includes a descent problem: trivializations on the components of the normalization need not agree along the double locus.

We work over an algebraically closed field kk of characteristic zero. A scheme is demi-normal if it is reduced, satisfies Serre’s condition S2S_2, is seminormal, and has only nodes in codimension one. Let XX be a projective equidimensional demi-normal scheme, and let B≥0B \ge0 be a rational Weil divisor with no component in the nonnormal locus. Write ν ⁣:Xˉ→X\nu\colon\bar{X} \to X for the normalization and Cˉ\bar{C} for its conductor divisor. The pair (X,B)(X, B) is semi-log-canonical, abbreviated slc, if KX+BK_X + B is rational Cartier and

(Xˉ,Cˉ+ν∗−1B)(\bar{X}, \bar{C} + \nu_*^{-1}B)

is log canonical. These are the singularities that allow normal components to meet along a double locus while retaining adjunction and pluricanonical descent [28]. We call (X,B)(X, B) a log Calabi–Yau pair when, in addition, KX+B∼Q0K_X + B \sim_{\mathbb{Q}} 0: some positive Cartier multiple has trivial associated line bundle. The index of the pair is the least such positive integer.

Theorem 1.1. For every integer d≥4d \ge4 and every finite set Φ⊂[0,1]∩Q\Phi\subset[0,1] \cap\mathbb{Q}, there is an integer a(d,Φ)>0a(d,\Phi) > 0 with the following property. Let (X,B)(X,B) be a connected projective equidimensional semi-log-canonical log Calabi–Yau pair of dimension dd over kk, with every nonzero coefficient of BB in Φ\Phi. Then

a(d,Φ)(KX+B) is Cartier,OX(a(d,Φ)(KX+B))≃OX.a(d,\Phi)(K_X+B)\text{ is Cartier}, \qquad\mathcal{O}_X\bigl(a(d,\Phi)(K_X+B)\bigr) \simeq\mathcal{O}_X.

The bound is independent of the number of irreducible components of XX and of the number of log canonical strata on their birational models. It is a common trivializing multiple, so it clears the local Cartier indices and kills the remaining global torsion at the same time. Together with the theorem in dimensions at most three of Jiang and Liu [26 Corollary 1.6], this proves the finite-rational-coefficient slc index conjecture [26 Conjecture 1.5].

History and relation to earlier work

The distinction between existence of an index and a uniform index is already visible in numerical-dimension-zero abundance. Gongyo proved that a numerically trivial log canonical divisor on a projective slc pair is rationally linearly trivial [16 Theorem 1.5]; the resulting trivializing multiple may depend on the pair. The index conjecture asks for a common multiple after fixing the dimension and the boundary coefficients. Its finite-rational-coefficient slc formulation is stated, for example, in Jiang and Liu [26 Conjecture 1.5]. The nonnormal setting is important because slc pairs occur as limits in moduli problems; see Kollár [28] and the boundedness theory for polarized slc Calabi–Yau pairs in Birkar [1].

Pluricanonical representations have long connected index problems to descent. Fujino developed admissible sections in his abundance theorem for slc threefolds [13], and formulated uniform boundedness of canonical representations for canonical varieties with trivial canonical divisor [14 Conjecture 3.2]. His local-index results and Ishii’s global-index theorem for non-klt log canonical threefold pairs with standard coefficients made this connection explicit [14, 24]. Here the standard coefficients are 11 and 1−1/q1 - 1/q for positive integers qq. Fujino–Gongyo subsequently proved finiteness of the log pluricanonical representation for every projective lc pair with semiample log canonical divisor [15 Theorem 1.1]. Uniform boundedness of these finite images is the additional issue in the index problem.

Xu organized reductions among the normal index conjecture, its slc version, and boundedness of pluricanonical representations [42]. In particular, his Theorem 1.11 gives the implication from normal indices in dimension dd and bounded representations in dimension d−1d-1 to slc indices in dimension dd. Jiang proved the global index bound for boundary-free klt threefolds [25 Corollary 1.7]. Jiang–Liu bounded the representations of lc surfaces with a fixed trivializing multiple, obtaining the slc index theorem in dimensions at most three and the non-klt lc case in dimension four [26 Theorem 1.4 and Corollaries 1.6–1.7]. Xu also treated klt fourfold pairs with nonzero boundary [42 Theorem 1.14].

Several more recent results give bounds under different geometric hypotheses. Birkar proved the index conjecture for rationally connected klt pairs in every dimension, allowing a fixed rational DCC coefficient set [2 Corollary 1.8]. Filipazzi–Mauri–Moraga obtained sharp bounds for coregularity-zero pairs, including slc pairs [12]; here coregularity zero means that a dlt model of the normalization with its induced boundary has a zero-dimensional minimal lc stratum. Figueroa–Filipazzi–Moraga–Peng developed corresponding index and complement results in low coregularity [11]. Masamura proved boundedness of the indices of smooth Calabi–Yau fourfolds [30 Corollary 1.6]. Uniform bounds need not be numerically small: Singh constructed smooth Calabi–Yau varieties whose indices grow doubly exponentially with dimension [37].

The proof here follows the established normal-to-slc strategy. It uses the uniform normal log canonical index theorem of the companion Uniform Pluricanonical Iitaka Fibrations [36 Theorem 1.2], together with the all-dimensional good-model theorem of Log abundance in characteristic zero [33 Theorem 11.1]. These are substantial inputs. Integral cohomology already bounds pluricanonical characters in terms of middle Betti numbers of suitable covers [26 Lemma 2.7]. The additional uniformity comes from a rank bound for the rational Hodge structure generated by a holomorphic top form and the resulting character bound for arbitrary integral klt pairs with fixed index. The latter is the klt case of the bounded-representation problem formulated in Jiang and Liu [26 Conjecture 1.1]. The final comparison of conductor residues uses Kollár’s linking theorem and its even-degree residue compatibility [29 Theorem 10 and Proposition 14].

The rank argument combines local positivity, moving subvarieties, and section counts. Its order propagation belongs to the Ein–Küchle–Lazarsfeld method [10]; we use the precise chain and scalar constructions of OpenAI [35 Sections 5–6] and OpenAI [36 Section 6]. Cotangent semipositivity [6, 18], divisorial Zariski decomposition [4, 5, 32], and effective birationality [1] supply the positivity estimates. The character argument builds on Matsumura–Wang’s decomposition of klt log Calabi–Yau pairs [31] and the singular Beauville–Bogomolov theory [9, 18, 19, 22]. For rationally connected factors we use Han–Jiang’s boundedness theorem and Jiang–Liu’s bounded-family representation theorem [21, 26]. The proofs below isolate the new uniform estimates and explain the adaptations of these earlier constructions.

The character obstruction and the proof

We first describe the descent problem that dictates the proof. The uniform normal index theorem of OpenAI [36 Theorem 1.2] supplies one even integer mm, depending only on dd and Φ\Phi, for all the normalization components. On the iith component its trivialization can be written as a rational mm-canonical form θi\theta_i with the prescribed logarithmic poles. On a crepant divisorial log terminal model, logarithmic residue restricts this form to the conductor strata. At a generic node, the two residues differ by a nonzero scalar rer_e; the existence of some global trivializing multiple ensures that the ratio is constant. Make a finite graph whose vertices are normalization components and whose edges are the generic nodes. Rescaling θi\theta_i changes its incident edge ratios. Thus simultaneous matching amounts to making every product of ratios around a closed walk equal to one. A uniform power of all the forms will accomplish this if the orders of these products are uniformly bounded.

Minimal log canonical strata supply the necessary interpretation of a closed walk. Their adjoint pairs are klt. Inside one normalization component, P1\mathbb{P}^{1}-linking identifies any two minimal strata by a crepant birational map that preserves the even-degree residue. Across an edge, we prove a corresponding birational residue comparison with multiplier rer_e. A closed walk therefore induces a crepant birational self-map of one minimal klt stratum, whose action on its trivializing form is exactly the product of the edge ratios. Section 7 carries out these comparisons, including nonsplit nodes and the final S2S_2 extension.

The main uniformity problem is consequently the following one. For a projective integral klt pair (V,Δ)(V,\Delta) satisfying m(KV+Δ)∼0m(K_V+\Delta)\sim0, bound, in terms of dim⁡V\dim V and mm, the order of the scalar by which a crepant birational self-map acts on a trivializing mm-canonical form. We prove this in Theorem 6.1. The structural decomposition of such pairs separates a rationally connected factor, an abelian factor, and irreducible Calabi–Yau or symplectic factors. The rationally connected factor is controlled by boundedness and log pluricanonical representations. For the other factors, the character appears in integral middle cohomology.

The relevant cohomology is the smallest rational Hodge substructure T(U)⊂Hn(U,Q)T(U)\subset H^{n}(U,\mathbb{Q}) containing the holomorphic top forms of a smooth projective resolution UU. It is birationally invariant and carries a polarized integral lattice. A bound for its rank therefore bounds the degree of the cyclotomic polynomial of a top-form character. Theorem 5.1 provides that rank bound under the rational-image hypotheses satisfied by the irreducible factors.

Two parts of the rank argument are useful independently. First, a dimension-dependent estimate for the variation of a Hodge norm gives a strict improvement over the largest possible metric growth whenever a specified top cup product vanishes. Applied to a class on the blowup of the diagonal, it bounds dim⁡T(U)\dim T(U) from a normalized volume and a lower Seshadri bound. These arguments occupy Sections 3 and 4. Second, Section 5 removes the Seshadri hypothesis. Small-order moving subvarieties determine rational fibrations; a maximal such fibration reduces the issue to vertical jets and horizontal section counts. A calibrated big divisor keeps the two counts on the same scale, and a finite power-map argument makes the horizontal estimate linear in the sheaf rank.

Section 6 converts this rank bound into the required uniform character exponent. Section 7 then proves Theorem 1.1. The substantial companion inputs—the normal index theorem, good minimal models, and the scalar and structural results used in these reductions—are stated with their precise roles in Section 2 and at their points of use.

Forms, birational maps, and uniform inputs

The analytic and Hodge-theoretic arguments are over C\mathbb{C}. We return to an arbitrary algebraically closed characteristic-zero field at the end of the proof. Varieties in the intervening sections are normal, integral, and projective unless otherwise specified. We use the standard discrepancy conventions for klt, dlt, and lc pairs [28]. For normal varieties, m(KX+Δ)∼0m(K_X+\Delta)\sim0 means that this is an integral principal divisor. In particular it is Cartier. This convention is stronger than rational linear triviality of the same multiple.

Trivializations as rational forms

Let F=C(X)F = \mathbb{C}(X) for an nn-fold XX. A rational mm-canonical form is a nonzero element of (⋀nΩF/C)⊗m(\bigwedge^{n} \Omega_{F/\mathbb{C}})^{\otimes m}. If η\eta is a rational top form and θ=uη⊗m\theta= u\eta^{\otimes m}, put

Div⁡(θ)=Div⁡(u)+mDiv⁡(η).\operatorname{Div}(\theta) = \operatorname{Div}(u) + m\operatorname{Div}(\eta).

The divisor on the right is independent of the expression for θ\theta. The equality m(KX+Δ)∼0m(K_X + \Delta) \sim0 is equivalent to the existence of such a form with

Div⁡(θ)=−mΔ.\operatorname{Div}(\theta) = -m\Delta.

All forms satisfying this identity differ by a nonzero constant. The identity also implies that mΔm\Delta is integral.

A birational map between pairs is BB-birational, or crepant birational, if the log canonical pullbacks agree on a common resolution, with canonical divisors chosen compatibly. We write Bir⁡(X,Δ)\operatorname{Bir}(X,\Delta) for the group of these self-maps. A pseudo-automorphism is a birational self-map which is an isomorphism on open subsets with complements of codimension at least two.

Lemma 2.1. Let (X,Δ)(X,\Delta) and (Y,ΔY)(Y,\Delta_Y) be normal projective pairs, and let θX,θY\theta_X,\theta_Y be degree-mm rational forms satisfying (2.1) for the respective boundaries. A birational map f:X⇢Yf : X \dashrightarrow Y is BB-birational if and only if

f∗θY=cθXfor some c∈C∗.f^*\theta_Y = c\theta_X \qquad\text{for some } c \in\mathbb{C}^*.

Proof. Choose a common smooth projective resolution WW, and use one rational top form to represent KWK_W. Write the two pulled-back forms as uXη⊗mu_X\eta^{\otimes m} and uYη⊗mu_Y\eta^{\otimes m}. If KW+ΔWXK_W + \Delta_W^X and KW+ΔWYK_W + \Delta_W^Y are the corresponding crepant pullbacks, then

m(KW+ΔWX)=−Div⁡(uX),m(KW+ΔWY)=−Div⁡(uY).m(K_W + \Delta_W^X) = -\operatorname{Div}(u_X), \qquad m(K_W + \Delta_W^Y) = -\operatorname{Div}(u_Y).

Their equality is equivalent to Div⁡(uY/uX)=0\operatorname{Div}(u_Y/u_X) = 0. A rational function with zero divisor on the normal projective integral variety WW is a nonzero constant.

Thus a BB-birational self-map acts on the one-dimensional space of trivializing forms by a scalar. Theorem 6.1 will bound its order uniformly. No finiteness assumption on the order of the birational map itself is made.

The normal index and good-model inputs

We isolate two substantial companion results. This makes clear which uniformity is already available on normal varieties and which must be proved for descent across the conductor.

Theorem 2.2 (Normal index theorem [36 Theorem 1.2]). For every integer d≥0d \ge0 and every rational set I⊂[0,1]I \subset[0,1] satisfying the descending chain condition, there is an integer alc(d,I)>0a_{\mathrm{lc}}(d,I)>0 such that every normal projective integral lc pair (X,Δ)(X,\Delta) of dimension dd, with coefficients in II and KX+Δ∼Q0K_X + \Delta\sim_{\mathbb{Q}} 0, satisfies

alc(d,I)(KX+Δ)∼0.a_{\mathrm{lc}}(d,I)(K_X + \Delta) \sim0.

Theorem 2.3 (Good minimal models [33 Theorem 11.1]). A projective lc pair over C\mathbb{C} with effective rational boundary and pseudo-effective log canonical divisor has a good log minimal model. In particular its adjoint is nonvanishing and its transform on the good model is semiample.

For a klt pair with a good minimal model, an MMP with scaling may be chosen to terminate at such a model. We use this consequence together with the extraction, small Q\mathbb{Q}-factorialization, and big-adjoint finite-generation results of [3]. When the adjoint is merely pseudo-effective, the good-model theorem above is the nonvanishing and semi-ampleness input.

We also use the uniform pluricanonical degree theorem [36 Theorem 1.1]: for smooth projective varieties of each fixed dimension and nonnegative Kodaira dimension, one complete pluricanonical system defines the Iitaka fibration. Section 5 states the chain and tracking consequences in the precise forms needed there.

Bounded comparison models for rationally connected bases

The rank argument uses a boundedness consequence of the canonical bundle formula. Recall that a contraction h ⁣:V→Yh \colon V \to Y is a projective surjective morphism of normal varieties with h∗OV=OYh_{*}\mathcal{O}_{V} = \mathcal{O}_{Y}. Two normal varieties are isomorphic in codimension one if they have isomorphic open subsets whose complements have codimension at least two.

Proposition 2.4. Fix nn. Let h ⁣:V→Yh \colon V \to Y be a contraction over C\mathbb{C}, where VV is klt of dimension nn, KV∼Q0K_{V} \sim_{\mathbb{Q}} 0, and 0<b=dim⁡Y<n0 < b = \dim Y < n. Suppose that a smooth projective resolution of YY is rationally connected. Then YY is isomorphic in codimension one to a normal projective variety Y^\widehat{Y} in a bounded family depending only on nn. In particular Y^\widehat{Y} has a very ample Cartier divisor HH for which

Hb≤Cn,∣KY^⋅Hb−1∣≤Cn.H^{b} \le C_{n}, \qquad\lvert K_{\widehat{Y}} \cdot H^{b-1} \rvert\le C_{n}.

The canonical intersection is the degree of the canonical Weil divisor on a general complete-intersection curve in the smooth locus.

Proof. The bounded moduli denominator proposition of OpenAI [36 Proposition 4.1] applies to hh. Its lower-dimensional normal-index hypotheses are supplied by Theorem 2.2. It gives a generalized klt pair (Y,BY+MY)(Y, B_{Y} + M_{Y}) with effective boundary in a dimension-dependent rational DCC set, b-nef moduli data with a uniformly bounded b-Cartier denominator, and

KY+BY+MY∼Q0.K_{Y} + B_{Y} + M_{Y} \sim_{\mathbb{Q}} 0.

Here the last equivalence follows from the exact canonical bundle formula and h∗OV=OYh_{*}\mathcal{O}_{V} = \mathcal{O}_{Y}. The proof of the rationally connected generalized torsion result [36 Proposition 4.5] shows that these bases are uniformly generalized ϵ\epsilon-lc and applies Birkar [2 Theorem 1.7] to obtain boundedness up to isomorphism in codimension one. Its normal bounded comparison models give Y^\widehat{Y}.

Choose very ample divisors from bounded projective embeddings of this family. Their top degrees are bounded. A general curve cut out by b−1b-1 such divisors is smooth and avoids the singular locus, and its degree and genus are bounded. Adjunction gives

KY^⋅Hb−1=2g(C)−2−(b−1)Hb,K_{\widehat{Y}} \cdot H^{b-1} = 2g(C) - 2 - (b-1)H^{b},

which proves the second bound. For b=1b = 1 use the normal curve itself.

Generic data and section orders

All finite collections of varieties, divisors, maps, and forms can be defined over a finitely generated subfield of C\mathbb{C}. Geometric generic fibres and moving subvarieties may be studied after algebraically closed field extension; sections commute with that extension, and the singularity conditions can be checked on a descended log resolution. We use very general points when countably many section-order conditions must hold simultaneously. Equivalently, the points may be taken geometric generic over a countable field containing the data. Dominant extensions of parameter spaces used to define models preserve this genericity.

For a big rational divisor DD on an nn-fold, write vol⁡(D)=lim sup⁡m→∞n!h0(mD)mn\operatorname{vol}(D)=\limsup_{m\to\infty}\frac{n!h^0(mD)}{m^n}, with degrees divisible enough to make the divisor integral. Divisors compared by an effective rationally linearly equivalent difference give inclusions of these complete section spaces. Section 5 will use such inclusions on resolutions, where orders are measured at smooth generic points. Object-dependent divisibility and asymptotic thresholds are permitted; the asserted final bounds depend only on the parameters specified in the corresponding statements.

The Hodge structure generated by the top forms

We will bound the order of a birational map on a one-dimensional space of pluricanonical forms by realizing its scalar as an eigenvalue of an integral Hodge structure of bounded rank. The relevant Hodge structure is usually much smaller than the full middle cohomology. We first recall its basic properties and prove the metric estimate that will make its rank accessible in Section 4.

For a smooth projective complex nn-fold UU, let

T(U)⊂Hn(U,Q)T(U) \subset H^n(U,\mathbb{Q})

be the smallest rational Hodge substructure whose complexification contains Hn,0(U)H^{n,0}(U), and put r(U)=dim⁡QT(U)r(U)=\dim_{\mathbb{Q}} T(U). Such a smallest substructure exists: intersections are Hodge substructures, and finite dimensionality reduces an arbitrary intersection to a finite one.

Lemma 3.1. The Hodge structure T(U)T(U) is birationally invariant. Cup product with any rational divisor class annihilates T(U)T(U); in particular, T(U)T(U) is primitive for every rational ample class. Moreover, if f:Z→Uf: Z \to U is a morphism from a smooth projective variety with dim⁡f(Z)<n\dim f(Z)<n, then f∗T(U)=0f^*T(U)=0.

Proof. For a birational morphism p:W→Up: W \to U between smooth projective varieties, p∗:Hn(U,Q)→Hn(W,Q)p^*: H^n(U,\mathbb{Q}) \to H^n(W,\mathbb{Q}) is an injective Hodge morphism, with left inverse p∗p_*. Birational invariance of holomorphic top forms gives Hn,0(W)=p∗Hn,0(U)H^{n,0}(W)=p^*H^{n,0}(U). The image p∗T(U)p^*T(U) therefore contains T(W)T(W) by minimality. Its inverse image of T(W)T(W) is a Hodge substructure containing Hn,0(U)H^{n,0}(U), and hence equals T(U)T(U). Thus T(W)=p∗T(U)T(W)=p^*T(U). Common resolutions give the assertion for birational maps.

The kernel of cup product with a rational divisor class is a rational Hodge substructure, with the usual Tate twist in the target. It contains Hn,0(U)H^{n,0}(U) because Hn+1,1(U)=0H^{n+1,1}(U)=0, so it contains T(U)T(U). Finally, f∗f^* vanishes on holomorphic top forms when its image has dimension less than nn. Its kernel is again a rational Hodge substructure, which proves the last assertion.

For a normal projective variety VV, we also write r(V)=r(U)r(V)=r(U), where UU is any smooth projective resolution. Lemma 3.1 makes this independent of the choice of UU.

We use the Hodge norm ∥z∥ω\|z\|_\omega of a cohomology class on a compact Kähler manifold: this is the L2L^2-norm of its ω\omega-harmonic representative. It is also the minimum L2L^2-norm among closed representatives of the class. We use the usual Lefschetz decomposition, Hodge–Riemann bilinear relations, and commutation of the Kähler Lefschetz operator with the Laplacian; see, for example, Voisin [40].

The next estimate concerns a Kähler metric stretched in at most half of the complex tangent directions. Without its cohomological hypothesis, a middle-degree norm can grow like Rn/2R^{n/2}. The cohomological hypothesis forces a uniform loss in this growth rate. The proof combines pointwise variation of the norm with orthogonality of harmonic and exact top-degree forms.

Lemma 3.2 (A quantitative Hodge norm gap). Let MM be a compact Kähler manifold of complex dimension 2n2n, where n≥1n \ge1, let DD be a Kähler form, and let HH be a smooth closed semipositive (1,1)(1,1)-form of pointwise rank at most nn. If z∈Hn,n(M)z \in H^{n,n}(M) satisfies [H]nz=0[H]^n z = 0, then, for every R≥1R \ge1,

∥z∥D+RH≤R(n−δn)/2∥z∥D+H,δn=1(2nn)+2.\|z\|_{D+RH} \le R^{(n-\delta_n)/2}\|z\|_{D+H}, \qquad\delta_n = \frac{1}{\binom{2n}{n}+2}.

Proof. Fix RR and write ω=D+RH\omega= D + RH, Q=RHQ = RH. Let γ\gamma be the ω\omega-harmonic representative of zz. In an ω\omega-unitary coframe diagonalizing QQ, write its eigenvalues as bi∈[0,1]b_i \in[0,1] and set bI=∑i∈Ibib_I = \sum_{i\in I} b_i for an nn-element subset II of {1,…,2n}\{1,\ldots,2n\}. Keeping γ\gamma fixed while differentiating its squared norm with respect to log⁡R\log R gives, relative to the present volume form,

∑∣I∣=∣J∣=n(Tr⁡Q−bI−bJ)∣γIJ‾∣2.\sum_{\lvert I\rvert=\lvert J\rvert=n} \left(\operatorname{Tr} Q-b_I-b_J\right)\lvert\gamma_{I\overline{J}}\rvert^2.

Indeed the volume contributes Tr⁡Q\operatorname{Tr} Q, while the covariant holomorphic and antiholomorphic factors contribute −bI-b_I and −bJ-b_J. Define the nonnegative pointwise deficit

e=n∣γ∣2−∑I,J(Tr⁡Q−bI−bJ)∣γIJ‾∣2.e=n\lvert\gamma\rvert^2-\sum_{I,J}\left(\operatorname{Tr} Q-b_I-b_J\right)\lvert\gamma_{I\overline{J}}\rvert^2.

We will prove

∫Me dVω≥δn∥γ∥ω2.\int_M e\,dV_\omega\ge\delta_n\|\gamma\|_\omega^2.

Put Nn=(2nn)N_n=\binom{2n}{n}. If rank⁡Q<n\operatorname{rank} Q<n, then Tr⁡Q≤n−1\operatorname{Tr} Q\le n-1 and e≥∣γ∣2e\ge\lvert\gamma\rvert^2. If rank⁡Q=n\operatorname{rank} Q=n, denote its nn-dimensional kernel by KK, the coefficient γKK‾\gamma_{K\overline{K}} by aa, and put

d0=n−Tr⁡Q,p=∏bi>0bi.d_0=n-\operatorname{Tr} Q,\qquad p=\prod_{b_i>0}b_i.

Every coefficient other than aa involves a positive eigenvalue in at least one index set. Subtracting that eigenvalue from Tr⁡Q\operatorname{Tr} Q leaves a sum of at most n−1n-1 numbers at most one. Consequently

e≥d0∣a∣2+∑(I,J)≠(K,K)∣γIJ‾∣2.e\ge d_0\lvert a\rvert^2+\sum_{(I,J)\ne(K,K)}\lvert\gamma_{I\overline{J}}\rvert^2.

Since 0≤bi≤10\le b_i\le1, we also have

(1−p)2≤d0,1−p2≤2d0.(1-p)^2\le d_0,\qquad1-p^2\le2d_0.

Consider the top-degree forms

A=ωnn!∧γ,B=Qnn!∧γ.A=\frac{\omega^n}{n!}\wedge\gamma,\qquad B=\frac{Q^n}{n!}\wedge\gamma.

In normalized exterior bases, the coefficient of AA is a signed sum of the NnN_n diagonal coefficients of γ\gamma. The coefficient of BB is papa, with the same sign as the aa term in AA. Thus Cauchy–Schwarz and (3.4) give

∣A−B∣2≤Nne,∣B∣2≥∣γ∣2−2e.\lvert A-B\rvert^2\le N_ne,\qquad\lvert B\rvert^2\ge\lvert\gamma\rvert^2-2e.

The same inequalities hold when rank⁡Q<n\operatorname{rank} Q<n: then B=0B=0 and e≥∣γ∣2e\ge\lvert\gamma\rvert^2. The form AA is harmonic, because multiplication by ω\omega commutes with the Laplacian. The form BB is exact, because QQ is closed and

[B]=Rnn![H]nz=0.[B] = \frac{R^n}{n!}[H]^n z = 0.

They are therefore L2L^2-orthogonal. Integrating (3.5) yields

Nn∫Me dVω≥∥A−B∥ω2≥∥B∥ω2≥∥γ∥ω2−2∫Me dVω,N_n \int_M e\,\mathrm{d}V_\omega\ge\lVert A-B\rVert_\omega^2 \ge\lVert B\rVert_\omega^2 \ge\lVert\gamma\rVert_\omega^2 - 2\int_M e\,\mathrm{d}V_\omega,

which is (3.3).

For completeness, varying the metric does not require differentiating the harmonic representative. At the current value of RR, keeping it fixed supplies an upper derivative for the minimum defining ∥z∥D+RH2\lVert z\rVert^2_{D+RH}. These minimum norms are locally Lipschitz in log⁡R\log R, by comparison of nearby metrics. Equations (3.2) and (3.3) therefore imply almost everywhere

ddlog⁡R∥z∥D+RH2≤(n−δn)∥z∥D+RH2.\frac{\mathrm{d}}{\mathrm{d}\log R}\lVert z\rVert^2_{D+RH} \le(n-\delta_n)\lVert z\rVert^2_{D+RH}.

Integration from 11 to RR proves (3.1).

A diagonal estimate for the Hodge rank

We now show that a lower bound for local positivity of a normalized polarization bounds r(U)r(U). The geometric part of the proof constructs a Kähler class on a modification of the blown-up diagonal, with all uncontrolled corrections supported on subvarieties that fail to dominate one factor. Lemma 3.1 makes these corrections invisible to T(U)T(U). The resulting diagonal class has a fixed nonzero intersection but a norm that decreases with r(U)r(U); Lemma 3.2 converts this comparison into the required bound.

For an ample rational divisor hh on a projective variety and a smooth point xx, its Seshadri constant is

ϵ(h;x)=inf⁡C∋xh⋅Cmult⁡xC,\epsilon(h;x)=\inf_{C\ni x}\frac{h\cdot C}{\operatorname{mult}_x C},

where the infimum runs over integral curves through xx. Equivalently, it is the largest ss for which σ∗h−sEx\sigma^*h-sE_x is nef on the blowup σ\sigma of xx.

Lemma 4.1 (Diagonal estimate). Fix an integer n≥2n\ge2 and a real number c>0c>0. Let XX be a normal projective complex nn-fold with canonical singularities and KX∼0K_X\sim0 as an integral principal divisor. Suppose hh is an ample rational divisor such that

1≤hn≤2,ϵ(h;x)>cat very general smooth points x∈X.1\le h^n\le2,\qquad\epsilon(h;x)>c\quad\text{at very general smooth points }x\in X.

Then r(U)=dim⁡QT(U)r(U)=\dim_{\mathbb{Q}}T(U), for any smooth projective resolution UU of XX, is bounded by a constant depending only on nn and cc.

Proof. Choose a resolution ρ:U→X\rho:U\to X, isomorphic over the smooth locus, obtained by blowups, and an effective exceptional divisor NN such that −N-N is ρ\rho-ample. The canonical form trivializing KXK_X gives

KU≥0,KU exceptional over X.K_U\ge0,\qquad K_U\text{ exceptional over }X.

Put H=ρ∗hH=\rho^*h and l=Hn∈[1,2]l=H^n\in[1,2]. We also denote by HH a smooth closed semipositive representative, obtained by pulling back a Fubini–Study form from an embedding given by a multiple of hh. Let

Y=U×U,π:P=Bl⁡ΔY⟶YY=U\times U,\qquad\pi:P=\operatorname{Bl}_{\Delta}Y\longrightarrow Y

be the blowup of the diagonal, with exceptional divisor EE. Subscripts 1,21,2 indicate pullback from the two factors, on every subsequent model. A subvariety of any such model will be called double dominant if its maps to both copies of UU are dominant.

Diagonal conditions and the number of sections

Fix rational numbers

t=14,τ=n−1+t,L=10n2.t=\frac{1}{4},\qquad\tau=n-1+t,\qquad L=10n^2.

and choose a rational a2a_2 depending only on n,cn,c, sufficiently large that a2>L/ca_2>L/c and a2>τ(1+1/(10n))a_2>\tau(1+1/(10n)). Set a1=10na2a_1=10na_2 and A=a1H1+a2H2A=a_1H_1+a_2H_2. These choices give the strict inequalities

a2>τ(1+a2/a1),n1+n/L>τ(1+a2/a1).a_2>\tau(1+a_2/a_1),\qquad\frac{n}{1+n/L}>\tau(1+a_2/a_1).

They remain true after sufficiently small rational perturbations of a1,a2,ta_1,a_2,t. We first prove that

G=A−τE is big,B(A−tE) has no double-dominant component,G=A-\tau E\text{ is big},\qquad\mathbf{B}(A-tE)\text{ has no double-dominant component},

where B\mathbf{B} denotes the stable base locus.

For sufficiently divisible positive integers mm, put

Qm=H0(Y,mA),Vm=H0(P,mG)=H0(Y,mA⊗IΔmτ)⊂Qm.Q_m=H^0(Y,mA),\qquad V_m=H^0(P,mG)=H^0(Y,mA\otimes\mathcal{I}_{\Delta}^{m\tau})\subset Q_m.

The conormal bundle of the diagonal is ΩU1\Omega_U^1. Its infinitesimal layers therefore give

dim⁡(Qm/Vm)≤∑0≤j<mτh0(U,OU(m(a1+a2)H)⊗Sym⁡jΩU1).\dim(Q_m/V_m)\leq\sum_{0\leq j<m\tau}h^0\left(U,\mathcal{O}_U\left(m(a_1+a_2)H\right)\otimes\operatorname{Sym}^j\Omega_U^1\right).

We need an estimate uniform in jj, because jj grows with mm.

The reflexive cotangent sheaf of XX is slope semistable of degree zero with respect to hh. This follows from generic semipositivity for the cotangent bundle and KX≡0K_X\equiv0; the precise singular-variety semistability and restriction statements we use are [18 Theorem 5.3 and Proposition 5.4]; see also [6 Theorem 1.3]. Choose a fixed sufficiently positive general complete-intersection flag on UU, cut by pullbacks of hypersurfaces on XX, terminating in a smooth curve CC avoiding the exceptional locus. Its members are smooth and integral. The bundle ΩU1∣C\Omega_U^1|_C is semistable of degree zero, as is every symmetric power in characteristic zero.

Write D0=m0HD_0=m_0H, with m0hm_0h very ample, and rj=(j+n−1n−1)r_j=\binom{j+n-1}{n-1}. On CC, a negative twist of Sym⁡jΩU1∣C\operatorname{Sym}^j\Omega_U^1|_C has no sections. For k≥0k\geq0, subtracting kdeg⁡CD0+1k\deg_C D_0+1 points gives

h0(C,OC(kD0)⊗Sym⁡jΩU1∣C)≤rj(kdeg⁡CD0+1).h^0\left(C,\mathcal{O}_C(kD_0)\otimes\operatorname{Sym}^j\Omega_U^1|_C\right)\leq r_j(k\deg_C D_0+1).

Negative twists also have no sections on higher flag members: general curves of this kind sweep out a dense subset, and their restrictions have negative slope. If a hypersurface cut in the flag has degree ee with respect to D0D_0, write bZ,j(k)b_{Z,j}(k) for the section dimension on the member ZZ. The restriction sequences and negative-twist vanishing give

bZ,j(k)≤∑a=0⌊k/e⌋bZ′,j(k−ae),Z′∈∣eD0∣Z.b_{Z,j}(k)\leq\sum_{a=0}^{\lfloor k/e\rfloor}b_{Z',j}(k-ae),\qquad Z'\in|eD_0|_Z.

Since D0i−1⋅Z′=e(D0i⋅Z)D_0^{i-1}\cdot Z'=e(D_0^i\cdot Z), summing the degree-(i−1)(i-1) leading term on Z′Z' divides its coefficient by eiei. Induction gives, on an ii-dimensional flag member ZZ,

h0(Z,OZ(kD0)⊗Sym⁡jΩU1∣Z)≤rj((D0i⋅Z)kii!+O((k+1)i−1)),h^0\left(Z,\mathcal{O}_Z(kD_0)\otimes\operatorname{Sym}^j\Omega_U^1|_Z\right)\le r_j\left(\frac{(D_0^i\cdot Z)k^i}{i!}+O((k+1)^{i-1})\right),

with the implied constant independent of jj. Since ∑j<qrj=qn/n!+O(qn−1)\sum_{j<q}r_j=q^n/n!+O(q^{n-1}), (4.3) becomes

dim⁡(Qm/Vm)≤l(a1+a2)nτn(n!)2m2n+o(m2n).\dim(Q_m/V_m)\le\frac{l(a_1+a_2)^n\tau^n}{(n!)^2}m^{2n}+o(m^{2n}).

All asymptotic errors in this proof concern the fixed variety and fixed divisors; their thresholds need not be uniform in XX. On the other hand,

dim⁡Qm=l2a1na2n(n!)2m2n+o(m2n).\dim Q_m=\frac{l^2a_1^na_2^n}{(n!)^2}m^{2n}+o(m^{2n}).

The first inequality in (4.1), together with l≥1l\ge1, makes the difference of the leading coefficients positive. Thus GG is big.

We next show that, for all sufficiently large divisible mm, there is no divisorial valuation vv over YY whose centre is double dominant and satisfies

v(Vm)≥mAY(v).v(V_m)\ge mA_Y(v).

Here v(Vm)v(V_m) is the order of the base ideal of Vm⊂H0(Y,mA)V_m\subset H^0(Y,mA), and AY(v)A_Y(v) is the log discrepancy. The Seshadri assumption and a2c>La_2c>L imply that ma2Hma_2H separates jets modulo the LmLm-th power of the maximal ideal on a dense open subset of UU, for all sufficiently large divisible mm. Indeed, at a smooth point satisfying the Seshadri bound the divisor a2h−LExa_2h-LE_x on its blowup is ample. Serre vanishing supplies the jet separation, and surjectivity of evaluation is open.

If (4.5) held, localize a resolution carrying vv over the generic point of the first factor and extend to C(U)‾\overline{\mathbb{C}(U)}. The divisor remains horizontal; its discrepancy and its base-ideal order become the corresponding quantities on this smooth geometric generic fibre. Double dominance ensures that its centre meets the second-factor jet-separation open. At a closed point yy of that intersection, the restricted base ideal II would satisfy lct⁡y(I)≤1/m\operatorname{lct}_y(I)\le1/m. For J=I+myLmJ=I+\mathfrak{m}_y^{Lm}, the sum-of-ideals inequality gives

lct⁡y(J)≤lct⁡y(I)+nLm≤1+n/Lm.\operatorname{lct}_y(J)\le\operatorname{lct}_y(I)+\frac{n}{Lm}\le\frac{1+n/L}{m}.

[8 Lemma 2.18]. The threshold–colength inequality [7 Theorem 1.1] then gives

s:=length⁡(Oy/J)≥mnn!(n1+n/L)n.s:=\operatorname{length}(\mathcal{O}_y/J)\ge\frac{m^n}{n!}\left(\frac{n}{1+n/L}\right)^n.

Jet separation allows us to choose ss sections g1,…,gsg_1,\ldots,g_s of ma2Hma_2H, defined over C\mathbb{C}, whose images modulo JJ are linearly independent over C(U)‾\overline{\mathbb{C}(U)}. Namely, after scalar extension the images of any complex basis span the quotient, so one can select a basis among them. If f1,…,fqf_1,\ldots,f_q is a complex basis of H0(U,ma1H)H^0(U,ma_1H), their qsqs products figjf_i g_j are linearly independent modulo VmV_m. To see this, restrict a complex linear relation to the geometric generic fibre and reduce modulo JJ. Independence of the gjg_j there makes each coefficient ∑icijfi\sum_i c_{ij}f_i zero at the generic point. These are complex linear relations among the fif_i, so all cijc_{ij} vanish.

Consequently (4.6) gives the lower leading coefficient

la1n(n!)2(n1+n/L)n\frac{l a_1^n}{(n!)^2}\left(\frac{n}{1+n/L}\right)^n

for m−2ndim⁡(Qm/Vm)m^{-2n}\dim(Q_m/V_m). By the second inequality in (4.1), this exceeds the upper coefficient in (4.4), a contradiction. The numerical bounds are uniform over the chosen jet-separation open, so the sufficiently large mm can be fixed independently of the hypothetical valuation.

This exclusion controls the discrepancies of a general divisor with the prescribed diagonal vanishing along every double-dominant centre. We now turn that discrepancy control into the second assertion of (4.2), by comparing an adjoint ample model with the diagonal blowup near such centres.

Removing base components that dominate both factors

Fix such an mm, also large enough that ∣mG∣|mG| has generically finite map. First choose a log resolution p0:W→Pp_0 : W \to P of its base ideal, together with EE and NK=π∗KYN_K = \pi^*K_Y. Then choose ΔP∈1m∣mG∣\Delta_P \in\frac{1}{m}|mG| general. Bertini makes its free part smooth and transverse to the fixed normal crossings divisor, so the resulting boundary on WW is log smooth. Write

KW+ΔW=p0∗(KP+ΔP).K_W+\Delta_W=p_0^*(K_P+\Delta_P).

Every double-dominant divisor on WW has coefficient less than one in ΔW\Delta_W. To verify this, use

KP+ΔP=π∗(KY+π∗ΔP)−tE.K_P+\Delta_P=\pi^*(K_Y+\pi_*\Delta_P)-tE.

For the finitely many exceptional or fixed divisors on this resolution, a general member has valuation v(Vm)/mv(V_m)/m after pushforward to YY. Its coefficient in ΔW\Delta_W is therefore

1−AY(v)+v(Vm)m−tv(E)<11-A_Y(v)+\frac{v(V_m)}{m}-tv(E)<1

when its centre is double dominant, by the exclusion of (4.5). Components of the general free part have coefficient 1/m<11/m<1. Formula (4.7) remains valid if EE occurs in the fixed part of ∣mG∣|mG|: pulling back the pushforward restores exactly the prescribed multiplicity mτEm\tau E.

Replace negative coefficients of ΔW\Delta_W by zero, and decrease all coefficients at least one to rational numbers strictly below one. The resulting boundary BWB_W is klt. Set LW=KW+BWL_W=K_W+B_W; then

KW+BW=p0∗(D′+NK)+Ge−FN,D′=KP+ΔP−NK∼QA−tE,K_W+B_W=p_0^*(D'+N_K)+G_e-F_N,\qquad D'=K_P+\Delta_P-N_K\sim_{\mathbb{Q}} A-tE,

where NK≥0N_K\geq0, Ge≥0G_e\geq0 is p0p_0-exceptional, and every component of FN≥0F_N\geq0 fails to be double dominant. The assertion about GeG_e follows because ΔP\Delta_P is effective: negative coefficients can occur only on p0p_0-exceptional divisors. The assertion about FNF_N is the preceding coefficient bound.

The divisor KW+BWK_W+B_W is big. Indeed, KWK_W is effective, and BWB_W contains with positive coefficient the big free part of ∣mG∣|mG|. The existence of ample models for big klt adjoints [3] gives a projective klt pair (V,BV)(V,B_V), the ample rational adjoint divisor DV=KV+BVD_V=K_V+B_V, and a common smooth resolution

r0:S→W,q:S→V,p=p0r0:S→Pr_0:S\to W,\qquad q:S\to V,\qquad p=p_0r_0:S\to P

such that

r0∗(KW+BW)=q∗DV+EV,EV≥0 is q-exceptional.r_0^*(K_W+B_W)=q^*D_V+E_V,\qquad E_V\geq0\text{ is }q\text{-exceptional}.

We choose divisor representatives compatibly throughout these formulas.

Suppose that B(A−tE)\mathbf{B}(A-tE) has a double-dominant component. Its image in YY contains a point z=(x,y)z=(x,y) satisfying two conditions: neither xx nor yy lies on the image of a nonconstant rational curve in UU, and zz avoids the images of NKN_K and FNF_N. Such a point exists. The effective canonical divisor makes UU non-uniruled, so images of rational curves are contained in a countable union of proper closed subsets. Double dominance, and uncountability of C\mathbb{C}, allow us to avoid their inverse images and the finitely many other indicated subsets.

Every fibre of qq is rationally chain connected because (V,BV)(V,B_V) is klt, by [20 Corollary 1.6]. If a fibre meets (πp)−1(z)(\pi p)^{-1}(z), all its rational chains have constant image in both copies of UU: a nonconstant image would be a rational curve through xx or yy. Thus that entire fibre maps to zz. This uses the all-fibres statement; chains through special points may equivalently be obtained by proper specialization.

It follows that VV maps to YY near the points lying over zz. Here is the precise local argument. Let Γ⊂V×Y\Gamma\subset V\times Y be the closure of the graph of the birational map V⇢YV\dashrightarrow Y. Every fibre of Γ→V\Gamma\to V meeting V×{z}V\times\{z\} is a singleton, by the preceding paragraph and the map S→ΓS\to\Gamma. Properness makes this projection finite near each such fibre, and finite birationality over normal VV makes it an isomorphism there. The image in YY of its non-isomorphism locus is closed and avoids zz. Removing it, and the images of NK,FNN_K,F_N, gives an open Y0∋zY^0\ni z for which the graph is an open V0⊂VV^0\subset V, proper over Y0Y^0, and SY0=q−1(V0)S_{Y^0}=q^{-1}(V^0).

Over Y0Y^0, Equations (4.8) and (4.9) reduce to

p∗D′+r0∗Ge=q∗DV+EV.p^*D' + r_0^*G_e = q^*D_V + E_V.

The divisors D′D' on PY0P_{Y^0} and DVD_V on V0V^0 are relatively ample over Y0Y^0: the first has relative class −tE-tE, and the second is the restriction of an ample divisor. Adding an effective exceptional divisor to a birational pullback does not change its pushforward section algebra, by normality. The relative Proj of the two sides of (4.10) therefore identifies PY0≃V0P_{Y^0}\simeq V^0. On this common model, pushforward gives D′=DVD'=D_V, and (4.10) gives EV=r0∗GeE_V=r_0^*G_e.

For divisible kk, the model formulas give the following map of complete section spaces:

H0(V,kDV)≃H0(W,kLW)→ ⋅skFN H0(W,k(LW+FN))≃H0(P,k(D′+NK)).\begin{aligned} H^0(V,kD_V)&\simeq H^0(W,kL_W) \xrightarrow{\ \cdot s_{kF_N}\ } H^0(W,k(L_W+F_N))\\ &\simeq H^0(P,k(D'+N_K)). \end{aligned}

The first isomorphism pulls sections to SS, multiplies by the canonical section of kEVkE_V, and descends to WW. The last uses LW+FN=p0∗(D′+NK)+GeL_W+F_N=p_0^*(D'+N_K)+G_e and removes the effective exceptional divisor GeG_e by pushforward. Large divisible multiples of DVD_V are globally generated. Their images in (4.11) generate above zz: there FN=NK=0F_N=N_K=0, and EV=r0∗GeE_V=r_0^*G_e shows that multiplication and removal of the exceptional factors cancel. Thus under PY0≃V0P_{Y^0}\simeq V^0 the transported section is exactly the original section of kDVkD_V. Finally NKN_K is a fixed divisor and can be removed. Indeed, under Y→X×XY\to X\times X, KYK_Y is effective exceptional and AA is pulled back from X×XX\times X, so

H0(Y,k(A+KY))=skKYH0(Y,kA)H^0(Y,k(A+K_Y))=s_{kK_Y}H^0(Y,kA)

for divisible kk. Its pullback NKN_K has zero coefficient along EE; dividing by its canonical section therefore preserves the vanishing condition imposed by −ktE-ktE. Hence

H0(P,k(A−tE+NK))=skNKH0(P,k(A−tE)).H^0(P,k(A-tE+N_K))=s_{kN_K}H^0(P,k(A-tE)).

Generation above zz contradicts the assumed base component. This proves (4.2).

An ample class with controlled corrections

The preceding argument controls where base conditions occur, rather than their number or multiplicity. This is enough: on each correction, Lemma 3.1 annihilates the pullback of T(U)T(U) from at least one factor.

Choose an ample rational divisor on PP of the form

J=m′(H1+H2)−N1−N2−λE,J = m'(H_1 + H_2) - N_1 - N_2 - \lambda E,

with m′m' large and λ>0\lambda> 0 small. For sufficiently small rational ε>0\varepsilon> 0, the stable base locus of A−tE−εJA - tE - \varepsilon J still has no double-dominant component. In fact

A−tE−εJ=(a1−εm′)H1+(a2−εm′)H2−(t−ελ)E+ε(N1+N2).A - tE - \varepsilon J = (a_1 - \varepsilon m')H_1 + (a_2 - \varepsilon m')H_2 - (t - \varepsilon\lambda)E + \varepsilon(N_1 + N_2).

The first three terms satisfy (4.2) by the strict margins in (4.1); adding the last effective term can introduce base components only in its non-double-dominant support.

Take a divisible multiple whose base locus is the stable base locus, and principalize its base ideal on a smooth w:P~→Pw:\widetilde{P} \to P, with normal crossings support also including EE. This can be done without changing the complement of the base locus. Write

w∗(A−tE−εJ)=M+Ffix,w^*(A - tE - \varepsilon J) = M + F_{\mathrm{fix}},

where MM is semiample and Ffix≥0F_{\mathrm{fix}} \ge0 has only non-double-dominant components. Choose an effective ww-exceptional TT with −T-T relatively ample. For sufficiently small rational u>0u > 0, εw∗J−uT\varepsilon w^*J - uT is ample. Consequently

D=w∗(A−tE)−Ffix−uT+H1+H2D = w^*(A - tE) - F_{\mathrm{fix}} - uT + H_1 + H_2

is ample and has a Kähler representative with D≥H1+H2D \ge H_1 + H_2. If FF is the strict transform of EE, then

D=(a1+1)H1+(a2+1)H2−tF−Z,Z=t(w∗E−F)+Ffix+uT≥0.D = (a_1 + 1)H_1 + (a_2 + 1)H_2 - tF - Z,\qquad Z = t(w^*E - F) + F_{\mathrm{fix}} + uT \ge0.

Its components are smooth and fail to be double dominant. All further constants CC depend only on nn, cc, and may increase from line to line. Volume monotonicity in (4.12) gives

∫P~D2n≤(2nn)(a1+1)n(a2+1)nl2≤C.\int_{\widetilde{P}} D^{2n} \le\binom{2n}{n}(a_1 + 1)^n(a_2 + 1)^n l^2 \le C.

For general x∈Ux \in U, the fibre P~x\widetilde{P}_x over the first projection is smooth and birational to UU. All the correction components avoid the fibre above the diagonal point (x,x)(x,x): for each one, at least one projection has proper image. Thus the original exceptional space there is unchanged and

Fx≃Pn−1,O(Fx)∣Fx=OPn−1(−1),D∣Fx=tc1(OPn−1(1)),Dxn≥l,F_x \simeq\mathbb{P}^{n-1},\qquad\mathcal{O}(F_x)|_{F_x} = \mathcal{O}_{\mathbb{P}^{n-1}}(-1),\qquad D|_{F_x} = t c_1(\mathcal{O}_{\mathbb{P}^{n-1}}(1)),\qquad D_x^n \ge l,

where Dx=D∣P~xD_x = D|_{\widetilde{P}_x}. The last inequality follows from Dx≥H2∣P~xD_x \ge H_2|_{\widetilde{P}_x}.

The diagonal class and its norm

We will construct a middle-degree class vv whose intersection with DnD^n is fixed, but whose norm is small when r(U)r(U) is large. A test class with the same intersection and the improved growth of Lemma 3.2 will then force an upper bound for r(U)r(U).

Put r=r(U)>0r=r(U)>0; positivity follows from the canonical generator, since Hn,0(U)H^{n,0}(U) is one-dimensional. By Lemma 3.1, T(U)T(U) is primitive. Choose a Hodge-homogeneous basis α1,…,αr\alpha_1,\ldots,\alpha_r of T(U)CT(U)_{\mathbb{C}}, orthonormal for its Hodge–Riemann Hermitian form, so that

∫Uαiαj‾=ciδij,∣ci∣=1.\int_U \alpha_i\overline{\alpha_j}=c_i\delta_{ij},\qquad|c_i|=1.

Put βi=αi‾/ci\beta_i=\overline{\alpha_i}/c_i and, on P~\widetilde{P}, set

v=lr∑i=1rαi⊗βi∈Hn,n(P~),v=\frac{l}{r}\sum_{i=1}^{r}\alpha_i\otimes\beta_i\in H^{n,n}(\widetilde{P}),

using pullback from YY. The graded product rule and the dual-basis normalization give

(−1)n∫P~vv‾=l2r,H1v=H2v=0.(-1)^n\int_{\widetilde{P}}v\overline{v}=\frac{l^2}{r},\qquad H_1v=H_2v=0.

On the diagonal, the class vv has integral ll; hence its restriction to FF is H1n∣FH_1^n|_F. On every component of ZZ, one projection has image of dimension less than nn, so Lemma 3.1 kills the corresponding factor in vv. The projection formula and (4.12) now give

Dv=−t[F]H1n,∫P~vDn=−tnl.Dv=-t[F]H_1^n,\qquad\int_{\widetilde{P}}vD^n=-t^nl.

For the second identity, integrate over the first factor and use ∫FxDxn−1=tn−1\int_{F_x}D_x^{n-1}=t^{n-1} from (4.14).

For R≥1R\geq1, consider ω=D+RH1\omega=D+RH_1. We claim that

∥[F]H1n∥ω≤CR−n/2.\|[F]H_1^n\|_\omega\leq CR^{-n/2}.

By Hodge-star duality, it suffices to pair with harmonic (n−1,n−1)(n-1,n-1)-forms gg. On the general fibre, Lefschetz decomposition of the (1,1)(1,1)-class [Fx][F_x] bounds its squared Hodge norm by a dimensional constant times

∣Fx2Dxn−2∣+(FxDxn−1)2Dxn.|F_x^2D_x^{n-2}|+\frac{(F_xD_x^{n-1})^2}{D_x^n}.

This is bounded by (4.14), since the two numerators are tn−2t^{n-2} and t2n−2t^{2n-2}. Consequently

∣∫P~x[Fx]g∣P~x∣≤C∥g∣P~x∥L2(Dx).\left|\int_{\widetilde{P}_x}[F_x]g|_{\widetilde{P}_x}\right|\leq C\|g|_{\widetilde{P}_x}\|_{L^2(D_x)}.

Here replacing a closed restricted form by its harmonic representative can only decrease its norm. Integrate against HnH^n on UU and apply Cauchy–Schwarz. Pointwise restriction to the vertical tangent space does not increase the norm, while

H1n∧ωn≤CR−nω2n.H_1^n\wedge\omega^n\leq CR^{-n}\omega^{2n}.

Fibre integration outside the measure-zero exceptional sets therefore gives

∫U∥g∣P~x∥L2(Dx)2Hn(x)≤CR−n∥g∥ω2.\int_U\|g|_{\widetilde{P}_x}\|_{L^2(D_x)}^2H^n(x)\leq CR^{-n}\|g\|_\omega^2.

Since ∫UHn=l≤2\int_UH^n=l\leq2, this proves (4.17).

Decompose v=v0+v1v=v_0+v_1 into its primitive and nonprimitive parts for ω\omega. Lefschetz linear algebra has a dimension-only inverse bound on the nonprimitive middle-degree part. Equations (4.15), (4.16), and (4.17) imply

∥v1∥ω≤C∥ωv∥ω≤CR−n/2.\|v_1\|_\omega\leq C\|\omega v\|_\omega\leq CR^{-n/2}.

Hodge–Riemann positivity on v0v_0, and orthogonality of Lefschetz summands for both the Hodge norm and the middle intersection pairing, then give

∥v∥ω≤C(r−1/2+R−n/2).\lVert v\rVert_{\omega} \le C(r^{-1/2}+R^{-n/2}).

Indeed, the signed self-pairing of v0v_0 is its squared norm, whereas the absolute self-pairing of v1v_1 is bounded by its squared norm; (4.15) supplies the remaining term l2/rl^2/r. To test the fixed intersection in (4.16), set

z′=Dn−c′H2n,c′=∫H1nDn∫H1nH2n=∫H1nDnl2.z' = D^n-c'H_2^n,\qquad c'=\frac{\int H_1^nD^n}{\int H_1^nH_2^n}=\frac{\int H_1^nD^n}{l^2}.

Thus H1nz′=0H_1^nz'=0, and ∣c′∣≤C|c'|\le C by Hi≤DH_i\le D and (4.13). The same inequalities give ∥z′∥D+H1≤C\lVert z'\rVert_{D+H_1}\le C: the indicated smooth representatives have bounded pointwise norm for D+H1D+H_1, whose volume is bounded. The form H1H_1 has rank at most nn, so Lemma 3.2 yields

∥z′∥D+RH1≤CR(n−δn)/2.\lVert z'\rVert_{D+RH_1}\le CR^{(n-\delta_n)/2}.

Since vH2=0vH_2=0, cup-product Cauchy–Schwarz and (4.18) now imply

tn≤tnl=∣∫vz′∣≤C(r−1/2+R−n/2)R(n−δn)/2.t^n\le t^nl=\left|\int vz'\right|\le C(r^{-1/2}+R^{-n/2})R^{(n-\delta_n)/2}.

Choose RR depending only on n,cn,c so large that the term CR−δn/2CR^{-\delta_n/2} is at most tn/2t^n/2. The remaining inequality bounds rr in terms of n,cn,c, as required. □

A uniform bound for the top-form Hodge structure

The diagonal estimate bounds the top-form Hodge rank from a uniform positive lower bound for the Seshadri constant of a normalized polarization. Here we remove that additional hypothesis for varieties whose smaller rational images are rationally connected.

Theorem 5.1. For every integer n≥2n\ge2 there is a constant RnR_n with the following property. Let TT be a projective Q\mathbb{Q}-factorial terminal complex nn-fold with KT∼0K_T\sim0. Suppose that a smooth projective resolution UU has h1(U,OU)=0h^1(U,\mathcal{O}_U)=0, and that every positive-dimensional rational image of TT of dimension less than nn has a rationally connected smooth projective resolution. Then

r(T)=dim⁡QT(U)≤Rn.r(T)=\dim_{\mathbb{Q}}T(U)\le R_n.

The proof proceeds by contradiction. Large r(T)r(T) produces covering subvarieties of Kodaira dimension zero on which complete systems of the restricted polarization have small orders. The rational functions constant on these members define fields that can be realized by contractions on small terminal models. We choose a contraction with maximal proper base dimension and use a bounded comparison model for its base. A suitable big divisor then lets us compare two section counts: vertical jets bound the number of independent restrictions to a fibre, while slopes on the base bound the number of global sections these restrictions can produce. Their product is too small to account for the divisor’s volume.

Unless another dependence is displayed, constants depend only on the dimension. Thresholds for taking a sufficiently divisible multiple of a divisor may depend on that divisor and its variety. We write D1⪯D2D_1\preceq D_2 when D2−D1D_2-D_1 is rationally linearly equivalent to an effective rational divisor; such a comparison is restricted only to subvarieties not contained in the chosen effective difference.

Section orders and the covering-family inputs

Let PP be a big, nef, semiample rational Cartier divisor on an integral projective variety VV. At a smooth point xx, set

γ(P;V,x)=sup⁡m>0 sufficiently divisible0≠s∈H0(V~,mμ∗P)ord⁡x(s)m.\gamma(P;V,x)=\sup_{\substack{m>0\ \text{sufficiently divisible}\\0\ne s\in H^0(\widetilde{V},m\mu^*P)}}\frac{\operatorname{ord}_x(s)}{m}.

where μ:V~→V\mu:\widetilde{V}\to V is a smooth projective resolution that is an isomorphism near xx. Birational pushforward makes this independent of the resolution. We always use these complete section spaces, even when VV occurs as a subvariety of another variety. Write γ(P;V)\gamma(P;V) for the very general value. In dimension dd, counting sections and jet conditions gives

γ(P;V)≥(Pd)1/d.\gamma(P;V)\ge(P^d)^{1/d}.

Indeed, the two leading counts are Pdmd/d!P^d m^d/d! and kd/d!k^d/d! for sections and conditions of order at least kk, respectively.

We use three results from the scalar-order construction of OpenAI [36 Section “Scalar order and curve estimates”]. We state exactly the parts needed below. A marked covering family consists of an integral parameter space SS, a dominant mark map u:S→Vu:S\to V, and an incidence I⊂S×V\mathcal{I}\subset S\times V whose geometric generic fibre CbC_b is integral, positive-dimensional, and contains u(b)u(b). A generic movement from a generic mark chooses a generic parameter over that mark and then a generic point of its member. Each new choice is generic over all preceding data. Dominant extensions of parameter spaces are allowed to specify geometric components and models.

Input 5.2 (Generic chains). A finite nonempty collection of marked covering families determines a rational fibration ξ:V⇢M\xi:V\dashrightarrow M with geometrically integral generic fibre. If its generic fibre, called a leaf, has dimension hh, then 1≤h≤dim⁡V1\le h\le\dim V, every generic member lies in a leaf, and at most hh generic movements reach a point generic in the leaf over the algebraic closure of the field of its starting mark. Suppose that, for each family, either

γ(P∣Cb;Cb,u(b))≤B,ordim⁡Cb=1,P⋅Cbmult⁡u(b)Cb≤B.\gamma(P|_{C_b};C_b,u(b))\le B,\qquad\text{or}\qquad\dim C_b=1,\qquad\frac{P\cdot C_b}{\operatorname{mult}_{u(b)}C_b}\le B.

For a smooth model FF of the geometric generic leaf, with PP pulled back, one then has

γ(P∣F;F)≤hB,(P∣F)h≤(hB)h.\gamma(P|_F;F)\le hB,\qquad(P|_F)^h\le(hB)^h.

This is [36 Lemma 6.2]. The assertion about endpoints also identifies its function field: C(M)\mathbb{C}(M) consists exactly of the rational functions constant on the geometric generic members. In fact, enlarge the field of definition to contain the function being tested. Constancy along successive movements then gives constancy at a generic endpoint of the leaf, hence constancy on that geometric generic leaf.

Input 5.3 (Tracking and canonical degrees). Let ZZ be projective, Q\mathbb{Q}-factorial and klt of dimension d≥2d\ge2, and let NN be big, nef and semiample. If d+1d+1 equally spaced positive rational levels, with spacing Δ>0\Delta>0, lie strictly between (Nd)1/d(N^d)^{1/d} and γ(N;Z)\gamma(N;Z), there is a covering family of subvarieties W⊂ZW\subset Z, of dimension 0<e<d0<e<d, such that a smooth geometric generic model W∗W^* satisfies

NeW≤(2/Δ)d−eNd,N^eW\le(2/\Delta)^{d-e}N^d,
KW∗(N∣W∗)e−1≤(KZ+(2d/Δ)N)∣W(N∣W)e−1.K_{W^*}(N|_{W^*})^{e-1}\le(K_Z+(2d/\Delta)N)|_{W}(N|_W)^{e-1}.

If a smooth model of ZZ has nonnegative Kodaira dimension, so does W∗W^*. The same inheritance statement holds for arbitrary covering families.

This is [36 Lemma 6.3]; its section order argument uses the parameter differentiation of Ein et al. [10 Proposition 2.3]. For the inheritance statement, cut the parameter space until incidence evaluation is generically finite and dominant, resolve, and restrict the ramification formula to a geometric generic parameter fibre. The cuts can be chosen with independent generic coefficients, so the construction still tests the original geometric generic member.

Input 5.4 (Small volumes on Iitaka fibres). Fix e≥1e \ge1 and C′>0C' > 0. Let WiW_i be smooth projective ee-folds with κ(Wi)≥0\kappa(W_i) \ge0, and let LiL_i be big, nef, semiample rational divisors such that

Lie⟶0,KWiLie−1≤C′Lie.L_i^e \longrightarrow0,\qquad K_{W_i}L_i^{e-1} \le C'L_i^e.

After passing to a subsequence and resolving their Iitaka fibrations, the smooth geometric generic fibres UiU_i have a fixed positive dimension, satisfy κ(Ui)=0\kappa(U_i) = 0, and obey

vol⁡(KUi+Li∣Ui)⟶0.\operatorname{vol}(K_{U_i}+L_i|_{U_i}) \longrightarrow0.

The restrictions Li∣UiL_i|_{U_i} remain big, nef and semiample. When the Iitaka base is a point, UiU_i is the entire smooth model.

This is [36 Lemma 6.4]. Its uniform Iitaka hypothesis is supplied by that paper’s uniform pluricanonical Iitaka theorem. We use the conclusion in arbitrary lower dimensions, including a zero-dimensional Iitaka base. All three inputs hold at geometric generic data: their finite constructions spread after dominant parameter extensions. A countable field of definition includes the section-order conditions in all sufficiently divisible degrees. Thus the analytic and model-theoretic inputs over C\mathbb{C} apply to these data without specializing a previously generic parameter.

Large rank produces subvarieties of small order

The transition is indirect: small Seshadri constants force large ambient section orders, and the tracking input turns these orders into subvarieties of small polarized degree. Passing to Iitaka fibres and repeating in decreasing dimension eventually produces small complete-system orders on Kodaira-dimension-zero members.

Lemma 5.5. Fix n≥2n \ge2 and η>0\eta> 0. There is a number R(n,η)R(n,\eta) such that if TT is as in Theorem 5.1 and r(T)>R(n,η)r(T) > R(n,\eta), the following holds. For every normal projective canonical VV birational to TT with KV∼0K_V \sim0, and every ample rational Cartier divisor PP on VV, there is a marked covering family of subvarieties CbC_b with 0<dim⁡Cb<n0 < \dim C_b < n, whose smooth geometric generic models satisfy

κ(Cb∗)=0,γ(P∣Cb;Cb,u(b))≤η(Pn)1/n,\kappa(C_b^*) = 0,\qquad\gamma(P|_{C_b};C_b,u(b)) \le\eta(P^n)^{1/n},

where the mark is smooth on the member.

Proof. We explain the two scalar-order arguments from [36] used here, since the additional fibration hypothesis in its full scalar-estimate Proposition 6.1 is unnecessary for this conclusion.

From small Seshadri constants to large ambient orders. Suppose that 1≤Pin≤21 \le P_i^n \le2 and that the very general Seshadri constants ϵ(Pi)\epsilon(P_i) tend to zero. Then

γ(Pi;Vi)⟶∞\gamma(P_i;V_i) \longrightarrow\infty

after passing to a subsequence. Otherwise the orders are bounded by some D0D_0. Curves realizing arbitrarily small Seshadri ratios spread into marked covering curve families. Input 5.2 produces leaves of a fixed dimension hh with (Pi∣Fi)h⟶0(P_i|_{F_i})^h \longrightarrow0. Since Pin≥1P_i^n \ge1, eventually 0<h<n0 < h < n. Resolve the leaf fibration and choose a very general smooth fibre FiF_i; put q=n−hq=n-h. Its normal bundle is trivial. Therefore restriction to its uuth infinitesimal neighbourhood has rank at most

(u+q−1q)h0(Fi,mPi∣Fi).\binom{u+q-1}{q}h^0(F_i,mP_i|_{F_i}).

Set u=⌈Dm⌉u=\lceil Dm\rceil for a fixed D>D0D>D_0. For each fixed fibration the leading coefficient of this expression in mnm^n is

Dqq!h!(Pi∣Fi)h,\frac{D^q}{q!h!}(P_i|_{F_i})^h,

whereas the ambient section count has coefficient at least 1/n!1/n!. First take ii large, then mm sufficiently divisible and large. A nonzero ambient section vanishes on that neighbourhood, so has order at least uu at a very general point of FiF_i. This contradicts the bound D0D_0. This argument is the proof of the second scalar inequality in [36], with its order bound as an explicit hypothesis.

From large ambient orders to small orders on moving members. If the lemma were false, choose counterexamples with r(Ti)→∞r(T_i)\to\infty and rescale PiP_i rationally to have 1≤Pin≤21\le P_i^n\le2. Lemma 4.1 forces ε(Pi)→0\varepsilon(P_i)\to0, and hence (5.6) holds. Take small projective Q\mathbb{Q}-factorializations and pull back PiP_i. They are klt, have principal canonical divisor, and preserve the complete section spaces. Choose n+1n+1 order levels with spacing Δi→∞\Delta_i\to\infty between (Pin)1/n(P_i^n)^{1/n} and γ(Pi;Vi)\gamma(P_i;V_i). Input 5.3 produces members of a fixed dimension e<ne<n on a subsequence. With WiW_i their smooth models and Li=Pi∣WiL_i=P_i|_{W_i},

κ(Wi)≥0,Lie⟶0,KWiLie−1≤C′Lie.\kappa(W_i)\ge0,\qquad L_i^e\longrightarrow0,\qquad K_{W_i}L_i^{e-1}\le C'L_i^e.

Here KVi∼0K_{V_i}\sim0, so C′C' can be fixed. Input 5.4 gives positive-dimensional Iitaka fibres UiU_i with κ(Ui)=0\kappa(U_i)=0 and adjoint volume tending to zero.

Represent Li∣UiL_i|_{U_i} by a divided general free member Γi\Gamma_i for which (Ui,Γi)(U_i,\Gamma_i) is klt. A Q\mathbb{Q}-factorial good model Zi′Z'_i of this big adjoint exists by [3]; write Ni′N'_i for its big semiample adjoint. Then

(Ni′)dim⁡Zi′⟶0,KZi′⪯Ni′,κ(Zi′)=0.(N'_i)^{\dim Z'_i}\longrightarrow0,\qquad K_{Z'_i}\preceq N'_i,\qquad\kappa(Z'_i)=0.

On a common resolution, with maps xix_i to UiU_i and yiy_i to Zi′Z'_i, there is also the effective comparison

xi∗(Li∣Ui)⪯yi∗Ni′.x_i^*(L_i|_{U_i})\preceq y_i^*N'_i.

To prove it, write xi∗(KUi+Γi)∼Qyi∗Ni′+Fix_i^*(K_{U_i}+\Gamma_i)\sim_{\mathbb{Q}}y_i^*N'_i+F_i with Fi≥0F_i\ge0 exceptional over Zi′Z'_i. Since κ(Ui)=0\kappa(U_i)=0, choose an effective Di∼QKUiD_i\sim_{\mathbb{Q}}K_{U_i}. In divisible degrees, the pullback of DiD_i plus a general member of the free polarization system contains the fixed part FiF_i. The latter general member contains none of the finitely many components of FiF_i, hence Fi≤xi∗DiF_i\le x_i^*D_i. Subtracting proves (5.7).

If γ(Ni′;Zi′)→0\gamma(N'_i;Z'_i)\to0 along a subsequence, stop. Otherwise take a subsequence on which it has a positive lower bound. More generally, the data at this stage have fixed dimension dd, are Q\mathbb{Q}-factorial klt, and satisfy

Nid⟶0,κ(Zi)≥0,KZi⪯a0Ni,γ(Ni;Zi)≥a1>0N_i^d\longrightarrow0,\qquad\kappa(Z_i)\ge0,\qquad K_{Z_i}\preceq a_0N_i,\qquad\gamma(N_i;Z_i)\ge a_1>0

for fixed positive a0,a1a_0,a_1. Choose d+1d+1 equally spaced fixed levels below a1a_1; they eventually exceed (Nid)1/d(N_i^d)^{1/d}. The tracking and Iitaka-fibre inputs apply again, since their canonical-degree bound is at most (a0+2d/Δ)Lie(a_0+2d/\Delta)L_i^e. They produce another good model of strictly smaller positive dimension, with polarization volume tending to zero, Kodaira dimension zero, canonical class bounded above by the new polarization, and comparison (5.7). At this new stage we make the same dichotomy: either the orders tend to zero along a subsequence and we stop, or they have a positive lower bound on a subsequence and the construction repeats. Every repetition decreases dimension. In dimension one the order is bounded by the degree, which tends to zero, so the construction must terminate with order tending to zero.

Trace these members through the successive covering families and Iitaka fibres to the original ViV_i. Fibres sweep the preceding member; the birational comparisons are isomorphisms on opens met by the next geometric generic members. Thus the composite members map birationally to their images and have Kodaira dimension zero. Each effective comparison restricts to the next member, which is not contained in its extra divisor. Restricting successively and pulling back to a common smooth model of the final descendant compares the original restricted polarization with the final polarization by an effective difference. Multiplication by that difference injects their complete section spaces. At a generic mark outside the difference it preserves order. Thus the resulting members satisfy γ(Pi∣Cb;Cb,u(b))→0\gamma(P_i|_{C_b}; C_b, u(b)) \to0. They eventually satisfy (5.5), a contradiction. This is the dimension-decreasing part of the first scalar-estimate proof in [36], stopped before its separate fibration contradiction.

We will also apply this lemma to a big rational divisor DD on a Q\mathbb{Q}-factorial canonical model XX birational to TT, with KX∼0K_X \sim0. Choose a small effective klt boundary proportional to DD and run its MMP. Its ample model XDX_D is canonical with KXD∼0K_{X_D} \sim0: the canonical generator remains principal on every model, and all these birational steps are crepant for the zero boundary. Let PDP_D be the ample polarization induced by DD. On a common resolution,

p∗D∼Qq∗PD+E,E≥0 exceptional over XD,v(D):=vol⁡(D)1/n=(PDn)1/n.p^*D \sim_{\mathbb{Q}} q^*P_D + E,\qquad E \ge0\ \text{exceptional over }X_D,\qquad v(D) := \operatorname{vol}(D)^{1/n} = (P_D^n)^{1/n}.

Multiplication by the fixed part identifies sufficiently divisible section spaces. The low-order lemma applies to (XD,PD)(X_D, P_D) because r(T)r(T) is birationally invariant.

Realizing chain fields by contractions

The chain fibration just constructed is initially rational. Its realization as a morphism on a small terminal model will make its base accessible to the boundedness input. Call a subfield of C(T)\mathbb{C}(T) attained if it is the field of a contraction T′→YT' \to Y, where T′T' is Q\mathbb{Q}-factorial terminal and is equipped with a crepant birational map to TT that is an isomorphism in codimension one.

Lemma 5.6. If 0<η<1/n0 < \eta< 1/n, every chain field obtained from a family in Lemma 5.5 is attained and has transcendence degree strictly between 00 and nn.

Proof. Its leaves have positive dimension. A leaf cannot fill VV, since (5.2) and (5.5) would give γ(P;V)≤nη(Pn)1/n\gamma(P; V) \le n\eta(P^n)^{1/n}, contradicting (5.1). Its function field is relatively algebraically closed in C(T)\mathbb{C}(T) by the geometric integrality of its leaves.

Choose a smooth projective base model MM for this field. For ϕ:T⇢M\phi:T\dashrightarrow M, let JJ be the closure on TT of the inverse image of a general member HMH_M of a very ample system on MM. The map is defined in codimension one, and these divisors form a movable system. On a smooth resolution p:T~→Tp:\widetilde{T}\to T resolving ϕ\phi,

p∗J=ϕ~∗HM+EM,EM≥0 exceptional over T.p^*J = \widetilde{\phi}^*H_M + E_M,\qquad E_M \ge0\ \text{exceptional over }T.

Choose HMH_M general for this resolution as well. With the canonical generator used to represent KT~K_{\widetilde{T}}, terminality gives

KT~≥aEMK_{\widetilde{T}} \ge aE_M

for some positive rational aa. We claim that all ratios of sections of divisible multiples of JJ are constant on the generic members of the covering family, transferred to T~\widetilde{T}. Here is why (5.10) may be used on a member. Cut the parameter space by the dimension of a generic evaluation fibre, choosing hyperplanes with independent generic coefficients. The resulting incidence evaluates generically finitely and dominantly to T~\widetilde{T}. Nonempty zero-dimensional cuts of the generic evaluation fibre avoid the added boundary in a projective closure. The universal choices of hyperplanes still dominate the original parameter space. After a geometric component and a resolution are chosen, the ramification formula on this total space, restricted to its smooth geometric generic parameter fibre C∗C^*, gives

KC∗⪰aEM∣C∗.K_{C^*} \succeq aE_M|_{C^*}.

The map ϕ~\widetilde{\phi} is constant on C∗C^*, so (5.9) identifies the restricted polarization with EM∣C∗E_M|_{C^*}. Two independent restricted sections in any common degree, followed by a suitable power and multiplication by the effective canonical difference, would give two independent sections of a pluricanonical system on C∗C^*. That would contradict κ(C∗)=0\kappa(C^*) = 0. Ambient nonzero sections remain nonzero at these generic data. The claim follows.

By the function-field characterization after Input 5.2, the section-ratio field of JJ is contained in C(M)\mathbb{C}(M). The reverse inclusion follows from ratios of hyperplane pullbacks, since HMH_M is very ample. Thus this section-ratio field is exactly C(M)\mathbb{C}(M).

For a small positive rational ϵ\epsilon, the pair (T,ϵJ)(T,\epsilon J) is klt and its adjoint is pseudo-effective. Theorem 2.3 gives a terminating MMP to a good model. There are no divisorial steps: the divisor is movable, whereas the exceptional divisor of a negative divisorial contraction is contained in its fixed part. Movability persists through the flips. These steps are crepant for the zero boundary; the resulting T′T' is again terminal and isomorphic to TT in codimension one. The semiample contraction, with Stein factorization, realizes the section-ratio field C(M)\mathbb{C}(M), which is already relatively algebraically closed. This proves attainment.

Assume now that r(T)>R(n,η)r(T) > R(n,\eta), where η\eta will be chosen uniformly at the end. There is an attained field of transcendence degree between 0 and nn. Among all attained fields of transcendence degree less than nn, choose one whose transcendence degree bb is maximal, and write its contraction as

h:T′⟶Y,s=n−b>0.h:T' \longrightarrow Y,\qquad s=n-b>0.

The rational-image hypothesis in Theorem 5.1 makes a smooth resolution of YY rationally connected. Proposition 2.4 therefore provides a normal comparison model Y^\widehat Y, isomorphic to YY in codimension one, and a very ample Cartier divisor HH with

N:=Hb≤C(n),∣KY^Hb−1∣≤C(n).N:=H^b\leq C(n),\qquad\lvert K_{\widehat{Y}}H^{b-1}\rvert\leq C(n).

We make one further modification so that divisors pulled back from the common big opens of these bases extend without ambiguity upstairs. Let F0F_0 be the sum of the prime divisors of T′T' whose image in YY has codimension at least two. There are finitely many: they are among the components of the closed locus where the fibre dimension is larger than ss. Choose a very ample H0H_0 on YY and a rational number a>2na>2n. Run a terminating MMP for a klt boundary rationally equivalent to

ϵF0+ah∗H0,\epsilon F_0+ah^*H_0,

with ϵ>0\epsilon>0 small; the latter summand is represented by divided general members. The length bound 2n2n for negative extremal rays, applied to the pair omitting this summand, forces every step to be over YY. Indeed a horizontal extremal curve has h∗H0h^*H_0-degree at least one, so the added summand makes its total degree positive. This argument repeats after each step, and the morphism to YY descends through contractions and flips.

Every component of F0F_0 is contracted. To see this, over the complement of their images the sections of the displayed adjoint come from aH0aH_0: the fibres are connected and the adjoint restricts trivially there. These base sections extend across the omitted codimension-two set by normality. Thus every surviving component of F0F_0 would be a fixed component in all sufficiently divisible systems, contradicting semiampleness on the good model. Write that model as

h ⁣:X⟶Y.h \colon X \longrightarrow Y.

It is Q\mathbb{Q}-factorial canonical, has KX∼0K_X \sim0, and defines the same field as before. Its resolution still has irregularity zero. Crucially, no prime divisor of XX maps to a subset of codimension at least two in YY. Terminality is no longer required for this working model; any later chain field is attained by applying Lemma 5.6 on the original terminal TT.

A big divisor calibrated by the degree on the base

To compare orders on fibres with slopes on the base, we need a linear functional on divisor classes of XX that agrees with base degree on pullbacks and is nonnegative on effective divisors. We construct this functional together with a big divisor whose volume root and functional value are controlled by one parameter. The base polarization alone has zero volume on XX, whereas an arbitrary ample divisor need not satisfy the required degree bound.

Lemma 5.7 (Calibration). Let h ⁣:X→Yh \colon X \to Y be a contraction of normal projective complex varieties, where XX is a Q\mathbb{Q}-factorial canonical nn-fold with KX∼0K_X \sim0 and irregularity zero on a resolution. Suppose that 0<b:=dim⁡Y<n0 < b := \dim Y < n and that no prime divisor of XX maps into a subset of codimension at least two in YY. Let Y^\widehat{Y} be a normal projective variety isomorphic to YY in codimension one, and let HH be a very ample divisor on Y^\widehat{Y} satisfying

Hb≤N0,∣KY^⋅Hb−1∣≤N0.H^b \le N_0,\qquad\left|K_{\widehat{Y}}\cdot H^{b-1}\right| \le N_0.

Pullback from the common smooth open subsets of the bases defines

W=h∗Cl⁡(Y)R=h∗Cl⁡(Y^)R⊂N1(X)R,ℓ(h∗L)=L⋅Hb−1.W = h^* \operatorname{Cl}(Y)_{\mathbb{R}} = h^* \operatorname{Cl}(\widehat{Y})_{\mathbb{R}} \subset N^1(X)_{\mathbb{R}},\qquad\ell(h^*L) = L\cdot H^{b-1}.

Let A=h∗HA=h^*H, represented by an effective integral Weil divisor. There is a linear extension ℓX ⁣:N1(X)R→R\ell_X \colon N^1(X)_{\mathbb{R}}\to\mathbb{R} of ℓ\ell, nonnegative on the pseudo-effective cone, and there are a rational number δ>0\delta>0 and a big rational divisor DD such that

cδ≤v(D)≤Cδ,D−δ3A is big,ℓX(D)≤Cδ.c\delta\le v(D) \le C\delta,\qquad D-\frac{\delta}{3}A\text{ is big},\qquad\ell_X(D)\le C\delta.

Here v(D)=vol⁡(D)1/nv(D)=\operatorname{vol}(D)^{1/n}, c>0c>0 depends only on nn, and CC depends only on n,N0n,N_0.

The two conditions beyond v(D)≍δv(D)\asymp\delta have distinct roles. The bigness of D−δA/3D-\delta A/3 will force the low-order families to be vertical. The bound on ℓX(D)\ell_X(D) will convert cotangent semipositivity into a slope bound on the base.

Proof. We first construct a supporting functional for the pseudo-effective cone and then choose a point on which volume has the required scale. The hypothesis on irregularity, together with Q\mathbb{Q}-factoriality, gives

Cl⁡(X)R=Pic⁡(X)R=N1(X)R.\operatorname{Cl}(X)_{\mathbb{R}}=\operatorname{Pic}(X)_{\mathbb{R}}=N^1(X)_{\mathbb{R}}.

Indeed pullback to a resolution detects numerically trivial line bundles, whose classes are torsion when the Picard variety is zero. We can therefore pass between real linear equivalence and numerical classes throughout the proof.

Choose common smooth big open subsets of YY and Y^\widehat{Y}. Their inverse image in XX has complement of codimension at least two, so Cartier pullbacks there extend uniquely as Weil divisors on XX. This defines the indicated pullback on class groups. It is injective: if s=n−bs=n-b and QQ is an ample Cartier divisor on XX, the operation

B⟼h∗(B⋅Qs)B \longmapsto h_*(B \cdot Q^s)

on divisor classes is a left inverse to pullback, up to multiplication by the positive degree of QsQ^s on the generic fibre. The same operation sends effective classes to effective classes or zero, by using general representatives of sufficiently divisible multiples of QQ.

The degree ℓ\ell is strictly positive on W∩Eff⁡‾(X)∖{0}W \cap\overline{\operatorname{Eff}}(X) \setminus\{0\}. To see the point requiring care, choose a finite linear projection f:Y^→Pbf:\widehat{Y} \to\mathbb{P}^b with f∗OPb(1)=OY^(H)f^*\mathcal{O}_{\mathbb{P}^b}(1)=\mathcal{O}_{\widehat{Y}}(H). For every effective real Weil divisor LL on Y^\widehat{Y},

ℓ(L)H−L has an effective representative.\ell(L)H-L \text{ has an effective representative.}

In fact f∗f∗L−L≥0f^*f_*L-L \ge0 and f∗L∼Rℓ(L)OPb(1)f_*L \sim_{\mathbb{R}} \ell(L)\mathcal{O}_{\mathbb{P}^b}(1). The intersect-and-push operation just described shows that if a pullback class is pseudo-effective on XX, its base class lies in the closure of effective base classes. Applying (5.14) to approximating classes and pulling back shows that a degree-zero such class and its negative are both pseudo-effective on XX. The pseudo-effective cone in N1(X)RN^1(X)_{\mathbb{R}} contains no line, so the class is zero. This also proves that the formula defining ℓ\ell is well defined on WW.

Fix an ample class P0P_0 on XX, and minimize ℓ(L)\ell(L) on the set

{L∈W:P0+L∈Eff⁡‾(X)}.\{L \in W : P_0+L \in\overline{\operatorname{Eff}}(X)\}.

The set is nonempty. Its subsets on which ℓ\ell is bounded above are bounded: otherwise, dividing an unbounded sequence by its norm and passing to a limit would give a nonzero pseudo-effective class in WW of nonpositive degree. Closedness therefore gives a minimum c0=ℓ(L0)c_0=\ell(L_0). Put d0=P0+L0d_0=P_0+L_0. The open big cone is disjoint from

P0+{L∈W:ℓ(L)≤c0}.P_0+\{L \in W:\ell(L)\le c_0\}.

Indeed a big point in this affine half-space would remain big after subtracting a sufficiently small positive multiple of AA, contradicting minimality. Separating these two convex sets gives a nonzero linear functional λ\lambda, nonnegative on the pseudo-effective cone, with λ(d0)=0\lambda(d_0)=0. Its restriction to WW is a nonnegative multiple of ℓ\ell: it vanishes on ker⁡ℓ\ker\ell, and the orientation follows from the half-space being separated. That multiple is positive, since otherwise λ(P0)=λ(d0)=0\lambda(P_0)=\lambda(d_0)=0, whereas a nonzero nonnegative functional is strictly positive at an interior point of the cone. Normalize λ\lambda to obtain ℓX\ell_X.

For t>0t>0, set dt=d0+tAd_t=d_0+tA. These classes are big. For large tt, L0+tAL_0+tA is pseudo-effective, since sufficiently large multiples of HH added to any fixed real Weil class on the base are effective; convexity with the pseudo-effective class d0d_0 then proves the assertion for every t>0t>0. On the other hand, AA is not big: its restriction to the positive-dimensional generic fibre is trivial. Continuity and homogeneity of volume give

v(dt)t=v(A+t−1d0)⟶0(t⟶∞),ℓX(dt)=tHb.\frac{v(d_t)}{t}=v(A+t^{-1}d_0)\longrightarrow0 \qquad(t\longrightarrow\infty), \qquad\ell_X(d_t)=tH^b.

It remains to bound this volume ratio from below for small tt. This is where the trivial canonical class enters the construction.

Let p:X~→Xp:\widetilde{X}\to X be a smooth projective resolution and write the divisorial Zariski decomposition of d~0=p∗d0\widetilde{d}_0=p^*d_0 as

d~0=Pσ(d~0)+Nσ(d~0).\widetilde{d}_0=P_\sigma(\widetilde{d}_0)+N_\sigma(\widetilde{d}_0).

We use its numerical formulation, as in [32 Chapter III] and [4]. Fix the dimension-dependent integer M=M(n)M=M(n) in Birkar’s Calabi–Yau effective birationality theorem [1 Corollary 1.4]. Suppose first that Pσ(d~0)P_\sigma(\widetilde{d}_0) is numerically nonzero. For an ample class JJ on X~\widetilde{X}, monotonicity of positive intersection products gives

vol⁡(d~0+uJ)=⟨(d~0+uJ)n⟩≥un−1Pσ(d~0+uJ)⋅Jn−1.\operatorname{vol}(\widetilde{d}_0+uJ)=\left\langle(\widetilde{d}_0+uJ)^n\right\rangle \geq u^{n-1}P_\sigma(\widetilde{d}_0+uJ)\cdot J^{n-1}.

Here the trace of the one-class positive product is the positive part of the divisorial Zariski decomposition; see [5 Definition 2.10, Proposition 2.13, Theorem 3.1, and Section 3.4]. As u↓0u\downarrow0, the intersection on the right tends to Pσ(d~0)⋅Jn−1>0P_\sigma(\widetilde{d}_0)\cdot J^{n-1}>0. Choose a>0a>0 such that p∗d1−aJp^*d_1-aJ is pseudo-effective. For 0<t<10<t<1, the identity dt=(1−t)d0+td1d_t=(1-t)d_0+td_1 and volume monotonicity yield

vol⁡(dt)≥(1−t)nvol⁡(d~0+at1−tJ).\operatorname{vol}(d_t)\geq(1-t)^n\operatorname{vol}\left(\widetilde{d}_0+\frac{at}{1-t}J\right).

Consequently v(dt)/t→∞v(d_t)/t\to\infty as t↓0t\downarrow0. The constants in this divergence may depend on XX; no uniform threshold in tt is needed.

Suppose instead that Pσ(d~0)P_\sigma(\widetilde{d}_0) is numerically zero. Then d0d_0 has a unique effective real representative N0′N'_0. For existence, push forward Nσ(d~0)N_\sigma(\widetilde{d}_0); numerical and real linear equivalence agree here. For uniqueness, the pullback of any effective representative of d0d_0 dominates Nσ(d~0)N_\sigma(\widetilde{d}_0). Their difference is effective and numerically zero, hence zero. Let E0E_0 be the reduced support of N0′N'_0. It has Kodaira dimension zero: if some multiple of E0E_0 had a different effective representative, replacing a sufficiently small positive multiple of E0E_0 inside N0′N'_0 would contradict uniqueness.

Choose a small positive rational ε\varepsilon for which (X,εE0)(X,\varepsilon E_0) is klt. Theorem 2.3 gives a terminating MMP for this pair and a good model X‾\overline{X}. Precisely the components of E0E_0 are contracted. Any divisorial step must contract a component of its transform, since K∼0K\sim0 and a curve outside the effective boundary has nonnegative intersection with it. Conversely, semiampleness on the good model and κ(E0)=0\kappa(E_0)=0 force the effective pushforward of E0E_0 to vanish. These steps are crepant for the zero boundary, so X‾\overline{X} is again Q\mathbb{Q}-factorial canonical with principal canonical divisor. The pushforward A‾\overline{A} of AA is an integral Weil divisor and is big: the big class dtd_t pushes forward to tA‾t\overline{A}. Birkar’s theorem now gives

vol⁡(A‾)≥M−n\operatorname{vol}(\overline{A})\geq M^{-n}

[1 Corollary 1.4]. Its hypotheses are exactly that X‾\overline{X} is projective klt, KX‾∼R0K_{\overline{X}}\sim_{\mathbb{R}}0, and A‾\overline{A} is big and integral; no Cartier-index bound is required.

A single rational number u≥0u\geq0 gives inclusions

H0(X‾,mA‾)⊆H0(X,m(A+uE0))H^0(\overline{X},m\overline{A})\subseteq H^0(X,m(A+uE_0))

for every sufficiently divisible mm. Indeed, on a common resolution pull back A‾\overline{A} and push forward to XX. The resulting rational divisor differs from AA only on E0E_0, and its difference is bounded above by uE0uE_0. Thus vol⁡(A+uE0)≥vol⁡(A‾)\operatorname{vol}(A+uE_0)\geq\operatorname{vol}(\overline{A}). For all sufficiently small t>0t>0 we have N0′≥tuE0N'_0\geq tuE_0, and hence

vol⁡(dt)=vol⁡(N0′+tA)≥tnvol⁡(A+uE0)≥tnM−n.\operatorname{vol}(d_t)=\operatorname{vol}(N'_0+tA)\geq t^n\operatorname{vol}(A+uE_0)\geq t^nM^{-n}.

The same conclusion includes E0=0E_0 = 0, with u=0u = 0.

In both cases the ratio v(dt)/tv(d_t)/t is at least M−1M^{-1} for all sufficiently small t>0t > 0. By (5.15) and continuity, it takes the value (2M)−1(2M)^{-1} at some t>0t > 0. At this parameter,

dt−t3A=d2t/3 is big,ℓX(dt)=tHb≤N0t.d_t-\frac{t}{3}A=d_{2t/3}\text{ is big},\qquad\ell_X(d_t)=tH^b\leq N_0t.

Approximate tt by a positive rational number δ\delta and dtd_t by a rational class DD. Openness of the big cone and continuity of volume and ℓX\ell_X preserve these assertions with, for example, lower constant 1/(4M)1/(4M) and suitable upper constant depending only on nn, N0N_0. Since XX is Q\mathbb{Q}-factorial, the rational class has a rational Cartier divisor representative. This proves (5.13).

Vertical orders and horizontal section counts

We now apply the low-order families to the divisor supplied by Lemma 5.7. Keep the contraction h ⁣:X→Yh\colon X\to Y, its bounded comparison model Y^\widehat{Y}, and the very ample divisor HH on Y^\widehat{Y}. Write b=dim⁡Yb=\dim Y, s=n−bs=n-b, A=h∗HA=h^*H, and N=HbN=H^b. Thus 0<b<n0<b<n, and both NN and ∣KY^⋅Hb−1∣\lvert K_{\widehat{Y}}\cdot H^{b-1}\rvert are bounded in terms of nn. There is no divisor of XX mapping into the codimension-two sets omitted when identifying YY with Y^\widehat{Y}. Let DD and δ>0\delta>0 be the calibrated divisor and parameter. In this subsection CC denotes constants depending only on nn, independently of 0<η≤10<\eta\leq1; the threshold for a sufficiently large divisible integer mm may depend on all the fixed geometric data.

For sufficiently large divisible mm, our target is the estimate

h0(X,OX(mD))≤C(mηv(D))s(mδ)b.h^0(X,\mathcal{O}_X(mD))\leq C(m\eta v(D))^s(m\delta)^b.

The first factor will bound, over the base function field, the number of independent restrictions to the generic fibre, using vertical jets. The second will bound their contribution to global sections, using slopes on the base and a section estimate linear in the sheaf rank. Since v(D)v(D) is comparable to δ\delta, this would contradict the volume asymptotic h0(X,mD)∼mnv(D)n/n!h^0(X,mD)\sim m^n v(D)^n/n! when η\eta is sufficiently small.

The families are vertical. Apply Lemma 5.5 to the ample model XDX_D of DD. If a geometric generic member CtC_t has nonconstant image in Y^\widehat{Y}, choose a hyperplane in ∣H∣\lvert H\rvert through the image of its marked point xtx_t without containing the image of CtC_t. Since D−δA/3D-\delta A/3 is big, choose a section of a sufficiently divisible multiple of this divisor whose divisor avoids the generic mark. This section, multiplied by the corresponding power of the hyperplane section, gives

γ(PD∣Ct;Ct,xt)≥δ/3.\gamma(P_D|_{C_t};C_t,x_t)\geq\delta/3.

Here one works on a common resolution and uses (5.8). The mark lies in the birational isomorphism locus and avoids the fixed divisor; the chosen section remains nonzero on the member. Hyperplane pullbacks extend in codimension one on XX because no divisor maps into the omitted base sets. The same construction is valid over the geometric generic coefficient field. The low-order bound is at most ηv(D)≤Cηδ\eta v(D)\le C\eta\delta, contradicting this inequality when η\eta is sufficiently small in terms of nn.

The family is therefore vertical for hh. Its chain field contains C(Y)\mathbb{C}(Y) and is attained. Both fields are relatively algebraically closed in C(X)\mathbb{C}(X); maximality of dim⁡Y\dim Y among proper attained fields forces them to coincide. Indeed the chain field is proper by Input 5.2 and the choice η<1/n\eta<1/n, and an inclusion of equal transcendence degree would be algebraic. On a smooth model FF of the geometric generic fibre of hh, also resolving the ample-model map, the chain estimate (5.2) now gives

γ(PD∣F;F)≤sηv(D).\gamma(P_D|_F;F)\leq s\eta v(D).

For sufficiently divisible mm, put Vm=H0(X,OX(mD))V_m = H^0(X, \mathcal{O}_X(mD)) and let rmr_m be the dimension over C(Y)\mathbb{C}(Y) of its span in the generic fibre of h∗OX(mD)h_*\mathcal{O}_X(mD). After extending to the geometric generic field, this span identifies with a subspace of H0(F,mPD∣F)H^0(F,mP_D|_F) multiplied by the fixed part in (5.8). At a general mark that fixed part is a unit. Thus (5.18) bounds the order of every nonzero element of the span, including arbitrary scalar combinations over that field. Its vertical kk-jet map is injective for

k=⌈msηv(D)⌉.k = \lceil ms\eta v(D)\rceil.

Consequently, for mm sufficiently large,

rm≤(s+ks)≤C(mηv(D))s.r_m \le\binom{s+k}{s} \le C(m\eta v(D))^s.

Saturate the subsheaf generically spanned by VmV_m in h∗OX(mD)h_*\mathcal{O}_X(mD), transfer it across the common big open of YY and Y^\widehat{Y}, and extend reflexively. This gives a reflexive sheaf Em\mathcal{E}_m on Y^\widehat{Y} of rank rmr_m, with

dim⁡Vm≤h0(Y^,Em).\dim V_m \le h^0(\widehat{Y},\mathcal{E}_m).

We must bound the number of these sections without losing a further power of rmr_m.

A slope bound from jets along the fibres. For a torsion-free sheaf S\mathcal{S} on Y^\widehat{Y} write

μH(S)=c1(S)⋅Hb−1rank⁡S.\mu_H(\mathcal{S}) = \frac{c_1(\mathcal{S}) \cdot H^{b-1}}{\operatorname{rank}\mathcal{S}}.

Let S⊂Em\mathcal{S} \subset\mathcal{E}_m be saturated of rank d>0d>0. On a smooth big open of XX, the saturated relative tangent sheaf T=ker⁡(dh)\mathcal{T}=\ker(dh) and its quotient in TX\mathcal T_X are vector bundles. We remove their codimension-two defects, while retaining the generic points of divisors where the differential of hh drops rank. The evaluation map from h∗Sh^*\mathcal{S} to L=OX(mD)L=\mathcal{O}_X(mD) is defined there. Since T\mathcal{T} is integrable, the bundles of jets along T\mathcal{T} have a filtration with quotients

L⊗Sym⁡i(T∗),0≤i≤k.L \otimes\operatorname{Sym}^i(\mathcal{T}^*), \qquad0 \le i \le k.

For completeness, these bundles can be constructed by taking ordered derivatives in local frames of T\mathcal{T}. The product rule makes changes of frames triangular in the order; integrability identifies the degree-ii symbol with Sym⁡i(T∗)\operatorname{Sym}^i(\mathcal{T}^*). The cocycle identities agree with ordinary fibrewise jets on the dense smooth locus of hh and hence hold throughout this open.

Functions from the base have zero derivative along T\mathcal{T}. Taking jets of the evaluation map therefore gives an OX\mathcal{O}_X-linear map

h∗S⟶JTk(L),h^*\mathcal{S} \longrightarrow J^k_{\mathcal{T}}(L),

generically injective by (5.18). Take its top exterior power and a nonzero component in the induced graded filtration. In characteristic zero, the symmetric and exterior powers occurring there embed in direct sums of tensor powers. Selecting a nonzero summand gives

h∗det⁡S⟶(T∗)⊗j⊗Ld,0≤j≤kd.h^*\det\mathcal{S} \longrightarrow(\mathcal{T}^*)^{\otimes j} \otimes L^d,\qquad0 \le j \le kd.

Wedge with the pulled-back base differentials defines a regular map

T∗⟶⋀b+1ΩX1⊗OX(−h∗KY^).\mathcal{T}^* \longrightarrow\bigwedge^{b+1}\Omega_X^1 \otimes\mathcal{O}_X(-h^*K_{\widehat{Y}}).

which is generically injective. To check regularity, extend a local leafwise covector to an ordinary covector and wedge it with the pulled-back base volume form. Two extensions differ by a conormal covector, whose wedge is zero. This also proves regularity along multiple-fibre divisors: the pulled-back volume form may vanish there but has no pole.

Combining (5.21) and (5.22), and moving the twists to the source, gives a nonzero map from a line bundle of class

h∗det⁡S−dmD+jh∗KY^h^* \det\mathcal{S} - dmD + jh^*K_{\widehat{Y}}

to a tensor power of ΩX1\Omega_X^1. We test this map by the functional ℓX\ell_X from Lemma 5.7. On a smooth resolution p:Z→Xp: Z \to X, define Λ(M)=ℓX(p∗M)\Lambda(M) = \ell_X(p_*M). This is nonnegative on pseudo-effective divisor classes and vanishes on exceptional classes. The canonical class of ZZ is effective and exceptional, since XX is canonical and KX∼0K_X \sim0, so Λ(KZ)=0\Lambda(K_Z) = 0.

Saturate the line defined by the map on ZZ. Campana–Păun’s cotangent theorem [6 Theorem 1.3] says that every torsion-free quotient of a cotangent tensor power on ZZ has pseudo-effective determinant. The determinant of the tensor power itself is a multiple of KZK_Z. It follows that the saturated line has Λ\Lambda-degree at most zero. Its pushforward differs from (5.23) by an effective divisor, because the original map is regular in codimension one. Thus

ℓ(det⁡S)≤dmℓX(D)−jℓ(KY^)≤Cdmδ.\begin{aligned} \ell(\det\mathcal{S}) \le dm\ell_X(D) - j\ell(K_{\widehat{Y}}) \\ &\le Cdm\delta. \end{aligned}

The last inequality uses j≤kdj \le kd, η≤1\eta\le1, the bounded canonical degree of Y^\widehat{Y}, and v(D)≤Cδv(D) \le C\delta; the ceiling in kk is absorbed once mδ≥1m\delta\ge1. If j=0j = 0, the same conclusion follows directly from the effective divisor of the map to OX\mathcal{O}_X. Since S\mathcal{S} was arbitrary, this proves μmax⁡,H(Em)≤Cmδ\mu_{\max,H}(\mathcal{E}_m) \le Cm\delta.

Counting sections without a rank loss. The following elementary consequence of the Grauert–Mülich–Spindler theorem removes the rank from inside the polynomial section bound.

Lemma 5.8. Let b≥1b \ge1. A torsion-free slope-semistable sheaf G\mathcal{G} on PCb\mathbb{P}^b_{\mathbb{C}}, of rank uu and slope μ\mu with respect to OPb(1)\mathcal{O}_{\mathbb{P}^b}(1), satisfies

h0(Pb,G)≤Cbu(1+max⁡{0,μ})b,h^0(\mathbb{P}^b,\mathcal{G}) \le C_bu\left(1+\max\{0,\mu\}\right)^b,

where CbC_b depends only on bb.

Proof. If μ<0\mu< 0, a nonzero section would yield a subsheaf of slope at least zero, contradicting semistability. Suppose μ≥0\mu\ge0. For b≥2b \ge2, the Grauert–Mülich–Spindler theorem [17, 38], in its torsion-free form [23 Corollary 3.1.6], bounds the highest degree aa of the splitting on a general line by a≤μ+(u−1)/2≤μ+ua \le\mu+ (u-1)/2 \le\mu+ u. For b=1b = 1, the splitting theorem on P1\mathbb{P}^1 and semistability give the stronger equality a=μa = \mu.

A general linear flag gives, for any torsion-free sheaf with highest general-line splitting degree aa,

h0(G)≤u(a+bb)(a≥0),h0(G)=0(a<0).h^0(\mathcal{G}) \le u\binom{a+b}{b}\quad(a \ge0), \qquad h^0(\mathcal{G}) = 0\quad(a < 0).

Indeed the successive restrictions can be chosen torsion-free: embed the sheaf in a vector bundle and choose the cuts general for the associated primes of the quotient as well. Testing general lines shows that twists by integers below −a-a have no sections. Starting with the bound u(a+1)u(a+1) on a line, the hyperplane restriction sequences and the identity ∑i=0a(i+b−1b−1)=(a+bb)\sum_{i=0}^{a}\binom{i+b-1}{b-1}=\binom{a+b}{b} prove (5.25) inductively. For an integer t≥1t \ge1, let

ft:Pb⟶Pb,[x0:⋯:xb]⟼[x0t:⋯:xbt].f_t:\mathbb{P}^b \longrightarrow\mathbb{P}^b,\qquad[x_0:\cdots:x_b]\longmapsto[x_0^t:\cdots:x_b^t].

Finite separable pullback preserves semistability [41 Lemma 2.1]. Since ftf_t is flat, Gt=ft∗G⊗OPb(b(t−1))\mathcal{G}_t=f_t^*\mathcal{G}\otimes\mathcal{O}_{\mathbb{P}^b}(b(t-1)) is torsion-free and semistable, of rank uu and slope tμ+b(t−1)t\mu+b(t-1). Moreover

h0(Gt)≥tbh0(G).h^0(\mathcal{G}_t)\geq t^b h^0(\mathcal{G}).

To see this, multiply the pulled-back sections by the tbt^b homogeneous monomials

x0b(t−1)−∑i=1bei∏i=1bxiei,0≤ei<t.x_0^{b(t-1)-\sum_{i=1}^b e_i}\prod_{i=1}^b x_i^{e_i},\qquad0\leq e_i<t.

On x0≠0x_0\ne0, these monomials form a basis of the upper function field over the field generated by the tt-th powers of the affine coordinates. A linear relation among their products with pulled-back sections therefore separates into linear relations among the original sections, which proves (5.26).

Apply (5.25) to Gt\mathcal{G}_t, whose highest general-line degree is at most tμ+b(t−1)+ut\mu+b(t-1)+u. Divide the resulting bound by tbt^b and let t→∞t\to\infty, keeping G\mathcal{G} and uu fixed. This yields

h0(G)≤ub!(μ+b)b.h^0(\mathcal{G})\leq\frac{u}{b!}(\mu+b)^b.

and hence the asserted bound, for example with Cb=bb/b!C_b=b^b/b!. □

Completion of the proof of Theorem 5.1. Choose a finite linear projection f:Y^→Pbf:\widehat{Y}\to\mathbb{P}^b for the embedding defined by HH. It has degree N=HbN=H^b and f∗OPb(1)=OY^(H)f^*\mathcal{O}_{\mathbb{P}^b}(1)=\mathcal{O}_{\widehat{Y}}(H). The torsion-free sheaf f∗Emf_*\mathcal{E}_m has rank NrmNr_m and

μmax⁡(f∗Em)≤Cmδ/N.\mu_{\max}(f_*\mathcal{E}_m)\leq Cm\delta/N.

For this, let A\mathcal{A} be its first Harder–Narasimhan term. Adjunction gives a nonzero map f∗A→Emf^*\mathcal{A}\to\mathcal{E}_m. After removing torsion and extending across codimension two, it gives a map from the reflexive pullback f[∗]Af^{[*]}\mathcal{A} to the reflexive sheaf Em\mathcal{E}_m; denote its torsion-free image by Q\mathcal Q. Finite separable reflexive pullback preserves semistability and multiplies slopes for these polarizations by NN [41 Lemma 2.1]. Consequently

Nμ(A)≤μH(Q)≤μmax⁡,H(Em)≤Cmδ,N\mu(\mathcal{A})\leq\mu_H(\mathcal Q)\leq\mu_{\max,H}(\mathcal{E}_m)\leq Cm\delta,

proving (5.27). No injectivity of the adjunction map is required.

Apply Lemma 5.8 to the semistable Harder–Narasimhan factors of f∗Emf_*\mathcal{E}_m and sum their section bounds. Their ranks sum to NrmNr_m, and NN is bounded in terms of nn. For all sufficiently large divisible mm, this gives

dim⁡Vm≤h0(Y^,Em)≤Crm(mδ)b≤C(mηv(D))s(mδ)b.\dim V_m\leq h^0(\widehat{Y},\mathcal{E}_m)\leq Cr_m(m\delta)^b\leq C(m\eta v(D))^s(m\delta)^b.

This is the target estimate (5.17). Divide by mnm^n and use the volume asymptotic in divisible degrees. Since n=s+bn=s+b, we obtain

v(D)nn!≤Cηsv(D)sδb.\frac{v(D)^n}{n!}\leq C\eta^s v(D)^s\delta^b.

The lower calibration bound v(D)≥cδv(D)\geq c\delta then implies cb/n!≤Cηsc^b/n!\leq C\eta^s. This is impossible for a sufficiently small positive η\eta depending only on nn. There are only finitely many pairs b,s>0b,s>0 with b+s=nb+s=n, so choose η\eta for all of them at once, also satisfying the earlier verticality and chain requirements, and then impose the rank threshold in Lemma 5.5. The resulting contradiction bounds r(T)r(T) in terms of nn alone. □

Uniform exponents for klt pluricanonical characters

The rank bound now gives a uniform exponent for the scalar by which a crepant birational transformation acts on a log volume form. We work over C\mathbb{C} throughout this section. The transformation itself may have infinite order.

Theorem 6.1 (Uniform klt character exponent). For integers n≥0n \ge0 and m≥1m \ge1, there is an integer L(n,m)>0L(n,m) > 0 with the following property. Let (X,Δ)(X,\Delta) be an integral projective klt nn-fold pair, with Δ≥0\Delta\ge0 and m(KX+Δ)∼0m(K_X+\Delta) \sim0 as an integral principal divisor. Choose a rational mm-canonical form θ\theta with Div⁡(θ)=−mΔ\operatorname{Div}(\theta)=-m\Delta. For every BB-birational self-map ff of (X,Δ)(X,\Delta), write f∗θ=cθf^*\theta=c\theta, where c∈C∗c \in\mathbb{C}^*. Then cL(n,m)=1c^{L(n,m)}=1.

The proof separates the action into its rationally connected, abelian, and nonabelian boundary-free factors. The main issue is that an arbitrary birational transformation need not preserve a given product cover. We first construct a cover admitting a lift, and then recover the factor fields from their tangent directions. This costs only the exponent n!n!, independently of the degrees of the covers.

A terminal model for the action

Passing to a terminal pair makes the action an isomorphism in codimension one. We will then lift it through a finite cover of the smooth locus.

Lemma 6.2. In the setting of Theorem 6.1, there is a projective crepant birational morphism

(V,BV)⟶(X,Δ)(V,B_V) \longrightarrow(X,\Delta)

such that VV is Q\mathbb{Q}-factorial, BV≥0B_V \ge0, and the pair (V,BV)(V,B_V) is terminal. Every BB-birational self-map of (X,Δ)(X,\Delta) induces a pseudo-automorphism of VV preserving BVB_V.

Proof. The extraction and Q\mathbb{Q}-factorialization theorem for klt pairs [3 Corollary 1.4.3] extracts the exceptional divisors with discrepancy at most zero. There are only finitely many such divisors. To recall why, take a log resolution with crepant subboundary ∑jbjDj\sum_j b_jD_j, where every bj<1b_j < 1. For an exceptional divisorial valuation vv over this resolution,

A∑jbjDj(v)=A∑jDj(v)+∑j(1−bj)v(Dj).A_{\sum_j b_jD_j}(v)=A_{\sum_j D_j}(v)+\sum_j(1-b_j)v(D_j).

The first term is a nonnegative integer. If it is positive and the centre is contained in the support, the displayed sum is strictly greater than one. If the generic point of the centre lies outside the support, smoothness gives log discrepancy at least two. Thus valuations of log discrepancy at most one are lc places of the reduced simple normal crossings divisor. Such places are toroidal; their positive integral weights are bounded by ∑j(1−bj)v(Dj)≤1\sum_j(1-b_j)v(D_j) \le1. Together with the finitely many divisors on the resolution, this proves finiteness. Extracting these places gives the asserted terminal pair, and its boundary is effective because each extracted discrepancy is nonpositive.

Pull θ\theta back to VV. Its order at every prime divisor of VV is nonpositive, whereas its order at every exceptional divisor over VV is strictly positive by terminality. A transformation multiplying θ\theta by a nonzero constant cannot exchange these two kinds of divisorial valuations. Neither it nor its inverse therefore contracts a prime divisor. It is a pseudo-automorphism, and the orders of θ\theta show that it preserves the boundary coefficients.

Product covers and their factor fields

We state the structural input in the form needed here. A finite surjective morphism of normal varieties is quasi-étale if it is étale in codimension one. By purity it is étale over the smooth locus of its target. We write Ω[j]\Omega^{[j]} for the reflexive extension of jj-forms from the smooth locus.

Input 6.3 (Product cover). Let (V,BV)(V,B_V) be an integral projective klt pair with BV≥0B_V \ge0, KVK_V rational Cartier, and KV+BV∼Q0K_V+B_V \sim_{\mathbb{Q}} 0. There is a finite quasi-étale cover

P=∏i∈IPi⟶VP=\prod_{i\in I}P_i\longrightarrow V

whose positive-dimensional factors have the following properties. There is at most one abelian factor and at most one rationally connected factor (F,H)(F,H), where (F,H)(F,H) is klt, H≥0H\ge0, and KF+H∼Q0K_F+H\sim_{\mathbb{Q}}0; the entire pulled-back boundary is the pullback of HH, and is zero if that factor is absent. All factors are Q\mathbb{Q}-Gorenstein. All other factors are irreducible Calabi–Yau or irreducible holomorphic symplectic varieties. They, and every connected normal finite quasi-étale cover of them, have canonical singularities and Cartier trivial canonical class. Their reflexive form algebra is generated by a top form in the Calabi–Yau case and by a symplectic form in the symplectic case. In particular they have no reflexive one-forms or vector fields.

The cover can be chosen so that every connected normal finite quasi-étale cover of FF is rationally connected. On every such cover, reflexive one-forms and vector fields tangent to the pulled-back boundary vanish.

The product decomposition is proved in OpenAI [34 Proposition 5.1], using the decomposition theorem of Matsumura and Wang [31 Theorem 1.3] and the singular Beauville–Bogomolov theorem [22 Definition 1.4 and Theorem 1.5]. The statements about further covers and logarithmic vector fields are respectively Lemmas 5.3 and 5.2 of OpenAI [34]. The abelian factor includes all one-dimensional boundary-free factors. A connected normal finite quasi-étale cover of an abelian variety is étale, and is again abelian after choosing an origin.

The following argument adapts the factor-direction construction in OpenAI [34 Proposition 5.4]. That proposition treats finite regular actions; we give the argument needed for arbitrary pseudo-automorphisms.

Lemma 6.4 (Lifting and separating a birational action). Let (V,BV)(V,B_V) be as in Lemma 6.2, of dimension n>0n>0. Choose a product cover P=∏i∈IPi→VP=\prod_{i\in I}P_i\to V as in Input 6.3, and let ff be a BB-birational self-map with f∗θ=cθf^*\theta=c\theta. There are normal integral projective varieties RR, RiR_i, finite quasi-étale maps

R→ψ∏i∈IRi⟶∏i∈IPi⟶V,R\xrightarrow{\psi}\prod_{i\in I}R_i\longrightarrow\prod_{i\in I}P_i\longrightarrow V,

and birational self-maps hih_i of RiR_i with the following properties. Each Ri→PiR_i\to P_i is a finite quasi-étale cover. Write HiH_i for its boundary, zero except on the rationally connected factor, and put pi=mp_i=m on that factor and pi=1p_i=1 on the others. There are rational pip_i-canonical forms θi\theta_i with

Div⁡(θi)=−piHi,hi∗θi=diθi(di∈C∗),\operatorname{Div}(\theta_i)=-p_iH_i,\qquad h_i^*\theta_i=d_i\theta_i\quad(d_i\in\mathbb{C}^*),

and

cn!=∏i∈Idim/pi.c^{n!}=\prod_{i\in I}d_i^{m/p_i}.

In particular each hih_i is BB-birational for (Ri,Hi)(R_i,H_i).

Proof. A cover admitting a lift. Put U=VsmU = V_{\mathrm{sm}}. The connected étale cover PU→UP_U \to U corresponds to a finite-index subgroup of π1top(U)\pi_1^{\mathrm{top}}(U). This fundamental group is finitely generated, so it has only finitely many subgroups of any fixed index. Their intersection is a finite-index characteristic subgroup contained in the subgroup defining PUP_U. Riemann existence gives its connected algebraic étale cover. Normalize VV in its function field to obtain a finite quasi-étale cover R→VR \to V factoring through PP.

The pseudo-automorphism ff identifies two open subsets of UU with complements of codimension at least two. Removing such subsets does not change the fundamental group of a complex manifold, by transversality. Characteristicity therefore lifts this isomorphism to the chosen cover. Riemann existence makes the lift algebraic, and it induces a pseudo-automorphism gg of RR. If HRH_R and θR\theta_R denote the pulled-back boundary and form, then

g∗θR=cθR,g^*\theta_R = c\theta_R,

and gg preserves HRH_R in codimension one. No degree bound for R→VR \to V is required.

Preserving the factor directions. Over the product of the smooth loci of the PiP_i, the map R→PR \to P is étale. The tangent directions of the factors give a splitting there, whose reflexive extension is

TR=⨁i∈IEi.\mathcal{T}_R = \bigoplus_{i \in I} \mathcal{E}_i.

Let TR(−log⁡Supp⁡HR)\mathcal{T}_R(-\log\operatorname{Supp} H_R) be the reflexive sheaf of derivations preserving the reduced ideal of every boundary component, a condition tested at codimension-one points. Consider the finite-dimensional C\mathbb{C}-algebra

A={u∈H0(R,End⁡(TR)):u(TR(−log⁡Supp⁡HR))⊆TR(−log⁡Supp⁡HR)}.\mathcal{A} = \{u \in H^0(R,\operatorname{End}(\mathcal{T}_R)) : u(\mathcal{T}_R(-\log\operatorname{Supp} H_R)) \subseteq\mathcal{T}_R(-\log\operatorname{Supp} H_R)\}.

Conjugation by gg acts on A\mathcal{A}: both the tangent sheaf and the logarithmic condition are determined on a big open set.

Every member of A\mathcal{A} has zero entries between different Ei\mathcal{E}_i. To see this, fix general smooth points in the complementary factors and slice in one factor direction. Each connected component over that factor’s smooth locus extends by normalization to a connected normal finite quasi-étale cover of the factor. The omitted set has codimension at least two, since a divisorial point of a finite cover lies over a divisorial, hence smooth, point of the normal factor. The ambient cover is étale on this open slice, so restricted entries are regular and extend reflexively across its complement. On the slice its tangent directions are Ei\mathcal{E}_i, while complementary summands are trivial. An entry in either direction involving a nonabelian boundary-free factor therefore gives reflexive one-forms or vector fields on its cover, and these vanish by Input 6.3. For the only remaining case, an abelian and a rationally connected factor, slice in the rationally connected direction. An entry towards the abelian summand gives one-forms; an entry in the reverse direction gives vector fields tangent to the boundary: that boundary is pulled back from the rationally connected factor, so the ideal-preservation condition restricts at every divisorial point of the slice. These vanish as well. The slices cover a dense open of RR, proving the assertion.

Consequently every block projection is a central idempotent of A\mathcal{A}. The primitive central idempotents give nonzero direct summands of the rank-nn tangent sheaf, so there are at most nn of them. Conjugation by gg permutes these idempotents. Therefore

h=gn!h = g^{n!}

fixes every primitive central idempotent. Every central idempotent is a sum of primitive central idempotents, so hh fixes every block projection and preserves each factor direction.

Recovering the factor fields. Let KiK_i be the relative algebraic closure of C(Pi)\mathbb{C}(P_i) in C(R)\mathbb{C}(R), and let RiR_i be the normalization of PiP_i in KiK_i. Equivalently, R→Ri→PiR \to R_i \to P_i is the Stein factorization of the projection. At the generic point of RR, the directions complementary to ii span Der⁡C(Pi)C(R)\operatorname{Der}_{\mathbb{C}(P_i)}\mathbb{C}(R). In characteristic zero their common field of constants is exactly KiK_i. Preservation of these directions thus gives a birational self-map hih_i of RiR_i.

The map ψ:R→∏iRi\psi: R \to\prod_i R_i is proper and has finite fibres, because its composite to PP is finite. It is finite and, by dimension, surjective. The maps Ri→PiR_i \to P_i are quasi-étale. Indeed, since C(P)/C(Pi)\mathbb{C}(P)/\mathbb{C}(P_i) is a regular extension, the product Ri×∏j≠iPjR_i \times\prod_{j\ne i} P_j is an intermediate normal finite cover of PP. Ramification over a prime of PiP_i would persist in this product and then in a prolongation to RR, contradicting quasi-étaleness of R→PR \to P. The same ramification calculation in the tower proves that ψ\psi is quasi-étale. In particular the pulled-back pairs (Ri,Hi)(R_i,H_i) are klt. The relation between hh and the hih_i is rational equivariance of ψ\psi; no regularity assertion about the hih_i is needed.

Comparing the forms. On each boundary-free RiR_i, choose a generator θi\theta_i of its trivial canonical sheaf. For the rationally connected factor, restrict the degree-mm trivialization pulled back from VV to that factor of PP, using smooth complementary points and the external product of canonical lines. The resulting form has divisor −mH-mH on that factor; pull it back to RiR_i. This constructs the forms of degree pip_i in the statement. Their product, in any fixed order, satisfies

θR=aψ∗(⋀iθi⊗m/pi)(a∈C∗).\theta_R = a\psi^*\left(\bigwedge_i \theta_i^{\otimes m/p_i}\right) \qquad(a \in\mathbb{C}^*).

Here the wedge denotes external product of pluricanonical lines. Indeed both sides have divisor −mHR-mH_R, so their ratio is a global unit on the normal projective integral variety RR.

Write ui=hi∗θi/θi∈C(Ri)∗u_i=h_i^*\theta_i/\theta_i \in\mathbb{C}(R_i)^*. Pulling (6.2) back by hh shows that the pullback of ∏iuim/pi\prod_i u_i^{m/p_i} is the constant cn!c^{n!}. Since ψ\psi is dominant, the product is constant on ∏iRi\prod_i R_i. Fixing general points in all complementary factors shows that every uim/piu_i^{m/p_i}, and hence every uiu_i, is constant. Denote it by did_i. This proves (6.1); proportionality of the forms proves that each hih_i is B-birational. □

We have reduced the character on VV to characters on finite covers of the individual factors. Their dimensions are at most nn, and the integer mm has not changed. We next bound these factor characters, using bounded families on the rationally connected factor and the rank bound on the other nonabelian factors.

Characters on the factors

Lemma 6.5 (Rationally connected factors). For r,m≥1r,m \ge1 there is an integer Erc(r,m)>0E_{\mathrm{rc}}(r,m)>0 that kills the degree-mm B-birational character of every integral projective rationally connected klt pair (F,H)(F,H) of dimension rr with H≥0H \ge0 and m(KF+H)∼0m(K_F+H) \sim0 integral principal.

Proof. By Han and Jiang [21 Theorem 1.2], the underlying varieties are bounded modulo flops: they are isomorphic in codimension one to normal members YY of a bounded family. The theorem applies because −m(KF+H)-m(K_F+H) is Cartier and nef. In dimension one one can instead use F≃P1F \simeq\mathbb{P}^1 directly.

Let BYB_Y be the strict transform of HH. A degree-mm log trivializing form has divisor −mBY-mB_Y on YY, by the codimension-one identification. Thus m(KY+BY)∼0m(K_Y+B_Y) \sim0 is integral principal, and the map is B-birational by the form criterion. In particular the transformed pair is klt. Choose very ample divisors AA in bounded projective embeddings of these YY, with ArA^r uniformly bounded. Since mBYmB_Y is integral,

(Supp⁡BY)Ar−1≤mBYAr−1=−mKYAr−1≤m(2+(r−1)Ar).(\operatorname{Supp} B_Y)A^{r-1} \le mB_YA^{r-1} = -mK_YA^{r-1} \le m\left(2+(r-1)A^r\right).

For the last inequality, take a general complete-intersection curve of r−1r-1 members of ∣A∣|A|. It is smooth and avoids the singular locus of the normal variety YY, and adjunction gives −KYAr−1=2−2g+(r−1)Ar-K_YA^{r-1}=2-2g+(r-1)A^r.

Reduced subvarieties of bounded degree in bounded projective embeddings form a bounded family. Moreover, the nonzero coefficients of BYB_Y lie in {1/m,…,(m−1)/m}\{1/m,\ldots,(m-1)/m\}, since the pair is klt. Thus the pairs are log bounded modulo B-birational contractions. (A birational map that is an isomorphism in codimension one is a birational contraction in this terminology.)

Jiang and Liu [26 Theorem 3.2], which applies in every dimension, now gives integers k,N>0k,N>0 depending only on r,mr,m such that k(KF+H)∼0k(K_F+H)\sim0 and the image of the degree-kk B-representation has order at most NN. If a map acts by dd on a degree-mm generator and by ee on a degree-kk generator, then comparison in degree kmkm gives dk=emd^k=e^m. Since eN!=1e^{N!}=1, we obtain dkN!=1d^{kN!}=1. We may take Erc(r,m)=kN!E_{\mathrm{rc}}(r,m)=kN!.

Lemma 6.6 (Boundary-free factors). For each r≥1r\ge1 there is an integer E0(r)>0E_0(r)>0 with the following property. Let YY be a connected normal finite quasi-étale cover of an rr-dimensional abelian, irreducible Calabi–Yau, or irreducible holomorphic symplectic factor of Input 6.3. Every birational self-map of YY acts on its canonical volume form by a scalar killed by E0(r)E_0(r).

Proof. Let UU be a smooth projective resolution of YY. The canonical singularities and trivial canonical class give hr,0(U)=1h^{r,0}(U)=1. For a nonabelian factor, OpenAI [36 Lemma 5.2] shows that q(U)=0q(U)=0 and that every positive-dimensional rational image of smaller dimension has rationally connected smooth resolution. Its hypotheses hold for YY itself, using the identity cover, because the defining form-algebra properties persist under all further connected normal finite quasi-étale covers. Take a crepant projective Q\mathbb{Q}-factorial terminalization of YY. It still has principal canonical divisor, and the two properties just stated are birational invariants. Theorem 5.1 therefore bounds dim⁡QT(U)\dim_{\mathbb{Q}}T(U) in terms of rr. Nonabelian factors here have dimension at least two. For an abelian factor, take U=YU=Y and use instead

dim⁡QT(U)≤dim⁡QHr(U,Q)=(2rr).\dim_{\mathbb{Q}}T(U)\leq\dim_{\mathbb{Q}}H^r(U,\mathbb{Q})=\binom{2r}{r}.

Thus there is a common dimension bound b(r)b(r) in either case.

Let p,q:W→Up,q:W\to U be a smooth projective common resolution of the induced birational self-map of UU. By Lemma 3.1, birational invariance of the Hodge structure generated by the top form gives

T(W)=p∗T(U)=q∗T(U).T(W)=p^*T(U)=q^*T(U).

Consequently A=p∗q∗A=p_*q^* preserves T(U)T(U) and the cup-product pairing there; its inverse is q∗p∗q_*p^*. Pullback and pushforward are integral on cohomology modulo torsion, so AA preserves the full lattice

T(U)∩(Hr(U,Z)/torsion).T(U)\cap\left(H^r(U,\mathbb{Z})/\mathrm{torsion}\right).

Moreover, T(U)T(U) is primitive for every rational ample class: the kernel of cup product by that class is a rational Hodge substructure containing Hr,0(U)H^{r,0}(U). The Hodge–Riemann relations therefore turn the cup pairing and Hodge decomposition on T(U)T(U) into a positive-definite Hermitian form, preserved by AA.

The scalar dd on the canonical volume form is an eigenvalue of this integral operator. It is an algebraic integer, and all its conjugates occur among the eigenvalues of AA, hence have modulus one. Kronecker’s theorem makes dd a root of unity. If its order is ee, the degree of its cyclotomic polynomial is Euler’s totient φ(e)\varphi(e), so

φ(e)≤b(r).\varphi(e)\leq b(r).

There are only finitely many positive integers with this property. Their least common multiple is a permissible choice of E0(r)E_0(r).

Proof of Theorem 6.1. For n=0n=0 the pair is a point and the character is trivial, so take L(0,m)=1L(0,m)=1. Suppose n>0n>0. Lemmas 6.2 and 6.4 express cn!c^{n!} as in (6.1). The rationally connected factor satisfies the hypotheses of Lemma 6.5; in particular it remains rationally connected by the cover-stable choice in Input 6.3. Every other factor satisfies Lemma 6.6. Define

E(n,m)=lcm⁡1≤r≤n{Erc(r,m),E0(r)},L(n,m)=n!E(n,m).E(n,m)=\operatorname{lcm}_{1\le r\le n}\{E_{\mathrm{rc}}(r,m),E_0(r)\},\qquad L(n,m)=n!E(n,m).

Each diE(n,m)=1d_i^{E(n,m)}=1, and (6.1) gives cL(n,m)=1c^{L(n,m)}=1. Every bound depends only on the factor dimensions and mm, and therefore only on n,mn,m.

Residues and descent across the conductor

The normal index theorem gives a uniformly bounded trivializing degree on each component of the normalization. The remaining question is whether these trivializations can be chosen compatibly along the conductor. We will express each obstruction around a conductor cycle as the character of a birational self-map of a single klt pair. Theorem 6.1 then kills every obstruction with the same exponent, independently of the number of components and the length of the cycle. This follows the established reduction from normal indices and bounded pluricanonical representations to slc indices [42 Theorem 1.11]. We give the residue comparison explicitly, using Kollár’s compatibility theorem inside each normalization component and keeping the degree fixed throughout.

We first work over C\mathbb{C}. Throughout this section mm is a positive even integer. For a dlt pair (Y,Γ)(Y,\Gamma), a stratum means YY itself or an lc centre. A minimal stratum is minimal for inclusion; thus it is YY if the pair is klt. Dlt strata are normal, iterated adjunction gives effective dlt pairs (W,ΓW)(W,\Gamma_W) on them, and the strata of (W,ΓW)(W,\Gamma_W) are exactly the strata of (Y,Γ)(Y,\Gamma) contained in WW. In particular, minimal strata are klt; see [28 Chapter 4] and [29 Definition 4].

Residues in a fixed degree

Suppose that (Y,Γ)(Y,\Gamma) is a projective integral dlt pair and that a rational mm-canonical form θ\theta satisfies

Div⁡(θ)=−mΓ.\operatorname{Div}(\theta)=-m\Gamma.

At the generic point of a codimension-kk stratum WW, the pair is simple normal crossing. In local coordinates in which the coefficient-one components through WW are x1⋯xk=0x_1\cdots x_k=0, write

θ=f(dx1x1∧⋯∧dxkxk∧dy1∧⋯∧dydim⁡W)⊗m.\theta=f\left(\frac{\mathrm{d}x_1}{x_1}\wedge\cdots\wedge\frac{\mathrm{d}x_k}{x_k}\wedge\mathrm{d}y_1\wedge\cdots\wedge\mathrm{d}y_{\dim W}\right)^{\otimes m}.

Here ff is a unit at the generic point of WW. Its logarithmic residue is the rational mm-canonical form

θW=f∣W(dy1∧⋯∧dydim⁡W)⊗m.\theta_W=f|_W\left(\mathrm{d}y_1\wedge\cdots\wedge\mathrm{d}y_{\dim W}\right)^{\otimes m}.

The usual residue transformation rule makes this definition independent of the coordinates. Reordering the normal coordinates changes an ordinary residue by a sign, which disappears because mm is even. Consequently residues along flags agree with direct iterated residues. For W=YW=Y, set θW=θ\theta_W=\theta. These forms satisfy the actual degree-mm identity

Div⁡(θW)=−mΓW,m(KW+ΓW)∼0.\operatorname{Div}(\theta_W)=-m\Gamma_W,\qquad m(K_W+\Gamma_W)\sim0.

Indeed, pluricanonical adjunction with the different gives this identity for θW⊗b\theta_W^{\otimes b} when bb is sufficiently divisible [29 Definition 13]. The generic residue construction commutes with tensor powers, so division of that divisor identity by bb gives (7.2). In particular, mΓWm\Gamma_W is integral. No enlargement of mm depending on the stratum is required.

Lemma 7.1 (Comparison within a dlt pair). Let (Y,Γ)(Y,\Gamma) and θ\theta satisfy (7.1). For any two minimal strata A,A′A,A', there is a BB-birational map ϕ:(A,ΓA)⇢(A′,ΓA′)\phi:(A,\Gamma_A)\dashrightarrow(A',\Gamma_{A'}) such that

ϕ∗θA′=θA.\phi^*\theta_{A'}=\theta_A.

Proof. There is nothing to prove if the pair is klt. Otherwise apply Kollár [29 Proposition 14] to the morphism Y→Spec⁡CY\to\operatorname{Spec}\mathbb{C}. Its hypotheses hold in degree mm: the pair is dlt, its log canonical divisor is rationally trivial, and ωY[m](mΓ)≃OY\omega_Y^{[m]}(m\Gamma)\simeq\mathcal{O}_Y. That proposition provides a birational comparison commuting exactly with the degree-mm residue maps, and hence the displayed identity. The divisor identities (7.2) imply BB-birationality.

The exact equality, rather than proportionality, can also be seen in the proof of that proposition. The minimal centres are joined by P1\mathbb{P}^1-links [29 Theorem 10]. Over the function field of a link's base, the two sections are 0,∞0,\infty on P1\mathbb{P}^1, and the logarithmic form is a base form times (dz/z)⊗m(dz/z)^{\otimes m}. Its residues at the two sections agree for even mm. Composition along the links preserves this equality.

We also need a comparison between two different dlt pairs. A crepant birational map need not be defined along a chosen minimal stratum, so ordinary restriction of that map is insufficient. The following argument constructs appropriate strata on a common resolution and checks that passage to them introduces no additional scalar.

Lemma 7.2 (Comparison across a birational map). Let (S,ΔS)(S,\Delta_S) and (T,ΔT)(T,\Delta_T) be projective integral dlt pairs of the same dimension, with rational mm-canonical forms satisfying

Div⁡(θS)=−mΔS,Div⁡(θT)=−mΔT.\operatorname{Div}(\theta_S)=-m\Delta_S,\qquad\operatorname{Div}(\theta_T)=-m\Delta_T.

Suppose τ:S⇢T\tau:S\dashrightarrow T is birational and τ∗θT=rθS\tau^*\theta_T=r\theta_S for r∈C∗r\in\mathbb{C}^*. Then there are minimal strata A⊂SA\subset S and A′⊂TA'\subset T and a BB-birational map ψ:(A,ΔA)⇢(A′,ΔA′)\psi:(A,\Delta_A)\dashrightarrow(A',\Delta_{A'}) such that

ψ∗θA′=rθA.\psi^*\theta_{A'}=r\theta_A.

Proof. The form identity makes τ\tau BB-birational. If one pair is klt, both are klt, and we take A=SA=S, A′=TA'=T, and ψ=τ\psi=\tau. Suppose therefore that there are proper lc centres. Put n=dim⁡Sn=\dim S and let k>0k>0 be the largest codimension of an lc centre of SS. Choose such a centre AA.

Corresponding strata on a common resolution. Take a projective log resolution of SS which is unchanged over the simple-normal-crossing neighbourhood of the generic point of AA [39 Resolution Lemma, p. 633]. Resolve the map to TT and its boundary, using smooth blowup centres having normal crossings with the accumulated boundary [27 Definition 25 and Theorem 35]. This gives a common smooth model p:W→Sp:W\to S, q:W→Tq:W\to T. Write

KW+ΔW=p∗(KS+ΔS)=q∗(KT+ΔT),K_W+\Delta_W=p^*(K_S+\Delta_S)=q^*(K_T+\Delta_T),

with compatible canonical divisors. The subboundary ΔW\Delta_W need not be effective, but its total support is simple normal crossing.

There is a codimension-kk component ZZ of an intersection of kk coefficient-one divisors of ΔW\Delta_W dominating AA. To verify this during the chosen blowups, start with AA on the initial snc open. A blowup whose centre misses the generic point of the currently chosen intersection leaves that intersection unchanged there. If its centre contains that generic point, the centre is locally defined by a subset of the kk boundary parameters: any additional tangential equation would cut the intersection properly and so could not contain its generic point. For a nontrivial such blowup, the subset has size h≥2h \ge2 and the exceptional divisor has coefficient h−(h−1)=1h - (h - 1) = 1; in each relevant coordinate chart, the exceptional divisor and the surviving strict transforms again have a codimension-kk intersection dominating the old one. This proves the assertion inductively. In making the resolution, include the full total transforms of both boundaries among the normal-crossing divisors, including exceptional components of crepant coefficient zero.

Let C=q(Z)C = q(Z). The intersection ZZ determines an lc place: for k=1k = 1 it is itself a coefficient-one divisor, and for k>1k > 1 blow up its generic intersection. Hence CC is an lc centre of TT. Since dim⁡C≤dim⁡Z=n−k\dim C \le\dim Z = n - k, its codimension is at least kk. Repeating the same construction with S,TS,T interchanged shows that the largest codimensions of their lc centres agree. It follows that codim⁡TC=k\operatorname{codim}_{T} C = k, and both AA and CC are minimal strata. In particular Z→AZ \to A and Z→CZ \to C are generically finite.

Birationality and the exact residue comparison. We claim that these two maps are birational and that pullback through either one commutes exactly with the degree-mm residue. We prove this for qq. At the generic points of CC and ZZ, choose regular parameters x1,…,xkx_1,\ldots,x_k and z1,…,zkz_1,\ldots,z_k for the respective coefficient-one divisors, completed by separating coordinates y1,…,yn−ky_1,\ldots,y_{n-k} and w1,…,wn−kw_1,\ldots,w_{n-k} along the strata. The total transforms have normal crossings, so

q∗xi=ui∏j=1kzjeij,ui∈OW,ηZ∗,eij∈Z≥0.q^*x_i=u_i\prod_{j=1}^{k}z_j^{e_{ij}},\qquad u_i\in\mathcal{O}^{*}_{W,\eta_Z},\qquad e_{ij}\in\mathbb{Z}_{\ge0}.

In these coordinates the logarithmic Jacobian is the matrix expressing q∗(dxi/xi),q∗dylq^*(dx_i/x_i),q^*dy_l in terms of dzj/zj,dwldz_j/z_j,dw_l. Its determinant is a unit at ηZ\eta_Z: the pullback of θT\theta_T has exactly the logarithmic poles prescribed by the coefficient-one components through ZZ, and no other zero or pole there. Modulo the ideal of ZZ, the matrix has the form

(E∗0JC),E=(eij),\begin{pmatrix} E & * \\ 0 & J_C \end{pmatrix}, \qquad E=(e_{ij}),

where JCJ_C is the Jacobian along Z→CZ \to C. In particular det⁡E≠0\det E \ne0.

We now use birationality of the ambient map to strengthen this to

∣det⁡E∣=1,C(Z)=C(C).\lvert\det E\rvert=1,\qquad\mathbb{C}(Z)=\mathbb{C}(C).

Choose positive real numbers α1,…,αk\alpha_1,\ldots,\alpha_k linearly independent over Q\mathbb{Q}, and take the monomial valuation at ηZ\eta_Z assigning zjz_j the value αj\alpha_j. It can be constructed in the completed regular local ring and restricted to C(W)\mathbb{C}(W). Its value group is ∑jZαj\sum_j\mathbb{Z}\alpha_j, and its residue field is C(Z)\mathbb{C}(Z).

Here is the local calculation that also identifies this valuation from the target. If a real valuation vv is centred on a regular local ring RR with parameters t1,…,tkt_1,\ldots,t_k, and their positive values are Q\mathbb{Q}-linearly independent, then

v((Frac⁡R)∗)=∑iZv(ti),κ(v)=κ(R).v((\operatorname{Frac} R)^*)=\sum_i\mathbb{Z}v(t_i),\qquad\kappa(v)=\kappa(R).

To check the assertions, expand any nonzero f∈Rf\in R modulo mRN\mathfrak{m}_R^N as a polynomial in the tit_i, with coefficients lifting residue classes. Nonzero coefficients have value zero, distinct monomials have distinct values, and the remainder has value at least Nmin⁡iv(ti)N\min_i v(t_i). Taking NN so large that this exceeds v(f)v(f) gives a unique term of least value. Thus v(f)v(f) is an integral combination of the parameter values. For a quotient of two elements of equal value, independence forces their least terms to have the same exponent vector, so its residue is the ratio of their coefficients in κ(R)\kappa(R). Residue classes already have lifts in RR, proving the reverse inclusion as well.

By (7.4), the values of the xix_i are the rows of EE applied to (αj)(\alpha_j); they are positive and independent. Apply (7.6) to OT,ηC\mathcal{O}_{T,\eta_C}. Since qq is birational, its fraction field and that of OW,ηZ\mathcal{O}_{W,\eta_Z} are the same. The value groups and residue fields computed in the two rings must therefore agree. Equality of the value groups says that EE is unimodular, while equality of the residue fields gives C(Z)=C(C)\mathbb{C}(Z)=\mathbb{C}(C). This proves (7.5).

Taking the logarithmic residue of q∗θTq^*\theta_T along ZZ now gives the pullback of θC\theta_C multiplied by (det⁡E)m=1(\det E)^m=1. The tangential Jacobian JCJ_C is precisely the one appearing in pullback of the stratum form. The identical argument for pp compares the residue along ZZ with θA\theta_A and proves that Z→AZ\to A is birational. The equality q∗θT=rp∗θSq^*\theta_T=r p^*\theta_S therefore gives (7.3), with A′=CA'=C and the birational map induced through ZZ. Finally (7.2) shows that this map is B-birational. □

The local descent rule at a node

Let ξ\xi be a codimension-one point of a demi-normal variety at which it is not normal. After a faithfully flat extension splitting the node and completion, its local ring has the form

A=F[[x,y]]/(xy),A‾=F[[x]]⊕F[[y]].A=F[[x,y]]/(xy),\qquad\overline{A}=F[[x]]\oplus F[[y]].

where FF is the residue field after that extension. The image of AA in A‾\overline{A} consists of the pairs with the same constant term. A canonical generator has branch expressions

(dxx,−dyy)∧η\left(\frac{dx}{x},-\frac{dy}{y}\right)\wedge\eta

where η\eta is a nonzero top differential in the tangential directions. One obtains this calculation for absolute canonical forms by first lifting a separating transcendence basis of the node’s residue field and performing the nodal curve calculation over the resulting function field.

Thus the branch residues of a degree-aa canonical generator differ by (−1)a(-1)^a. Conversely, if two branch forms are generators and their residues satisfy this rule, divide them by the branches of (7.7) to the power aa. The resulting branch units have matching nonzero constant terms. They form a unit of AA, so the forms come from a generator at the node. Faithfully flat descent gives the same criterion before splitting or completion. For a nonsplit node the two residues are compared by the nontrivial automorphism of its quadratic branch-field extension. A boundary whose support avoids ξ\xi does not change this calculation.

Uniform trivialization on the demi-normal pair

Proof of Theorem 1.1. First let the ground field be C\mathbb{C}. Write D=KX+BD=K_X+B and let ν:X‾→X\nu:\overline{X}\to X be the normalization, with conductor divisor C‾\overline{C}. The normalization formula is

ν∗D=KX‾+C‾+ν∗−1B.\nu^*D=K_{\overline{X}}+\overline{C}+\nu_*^{-1}B.

Denote its component pairs by (Xi,Δi)(X_i,\Delta_i), i∈Ii\in I. They are projective integral lc dd-folds with effective boundary coefficients in Φ∪{1}\Phi\cup\{1\} and KXi+Δi∼Q0K_{X_i}+\Delta_i\sim_{\mathbb{Q}}0. By Theorem 2.2, there is a common principal multiple depending only on d,Φd,\Phi. Choose an even multiple m=m(d,Φ)m=m(d,\Phi) which also clears the coefficients of Φ\Phi. Fix rational mm-canonical forms θi\theta_i with

Div⁡(θi)=−mΔi.\operatorname{Div}(\theta_i)=-m\Delta_i.

Choose projective crepant Q\mathbb{Q}-factorial dlt modifications (Yi,Γi)→(Xi,Δi)(Y_i,\Gamma_i) \to(X_i,\Delta_i) [29 Proposition 5]. Use the same notation for the pulled-back forms, whose divisors are −mΓi-m\Gamma_i.

Form a finite graph with vertices II and one edge for each generic point of the double locus of XX. At a split node its two branches give conductor components on the normalization, possibly on the same XiX_i. Their strict transforms are strata S⊂YiS \subset Y_i, T⊂YjT \subset Y_j, and the identification of the branch function fields gives a birational map τ:S⇢T\tau:S\dashrightarrow T. At a nonsplit node there is one conductor component with a quadratic function-field extension over the node; use it twice and take τ\tau to be the nontrivial involution. This gives a loop at the corresponding vertex. The graph may have multiple edges and loops. We can treat its connected components separately.

The assumed rational linear triviality of DD supplies a principal Cartier multiple MDMD, with MM divisible by mm. A generator in degree MM pulls back to biθi⊗M/mb_i\theta_i^{\otimes M/m} for constants bi∈C∗b_i \in\mathbb{C}^*: on each projective normal component the ratio has zero divisor. Its branch residues satisfy the node rule. Since MM is even, for an oriented edge e:i→je:i\to j this gives

(τ∗θTθS)M/m=bibj.\left(\frac{\tau^*\theta_T}{\theta_S}\right)^{M/m}=\frac{b_i}{b_j}.

The ratio is therefore a nonzero constant in the conductor function field. Write

τ∗θT=reθS,re∈C∗,reˉ=re−1.\tau^*\theta_T=r_e\theta_S,\qquad r_e\in\mathbb{C}^*,\qquad r_{\bar e}=r_e^{-1}.

In particular the induced map of the two adjoint pairs is B-birational. The integer MM is used only to establish these constant comparisons; it will not enter the uniform bound.

For each oriented edge, Lemma 7.2 supplies minimal strata on its two branches and a birational comparison with multiplier rer_e. By adjunction these strata are also minimal strata of the corresponding YiY_i. Along any closed walk in the graph, join successive choices within a vertex by Lemma 7.1. These intermediate maps have multiplier one. Composing all comparisons gives a B-birational self-map ff of one projective integral klt pair (A,ΓA)(A,\Gamma_A), with

f∗θA=(∏e in the walkre)θA.f^*\theta_A=\left(\prod_{e\text{ in the walk}}r_e\right)\theta_A.

The product respects the orientations of the walk. Moreover dim⁡A≤d−1\dim A\le d-1 and m(KA+ΓA)∼0m(K_A+\Gamma_A)\sim0 by (7.2). Figure 1 displays the composition for a three-edge cycle. The same argument includes loops, including the involution at a nonsplit node.

Choose

L=lcm⁡{L(q,m):0≤q≤d−1},a=mL.L=\operatorname{lcm}\{L(q,m):0\le q\le d-1\},\qquad a=mL.

where L(q,m)L(q,m) is given by Theorem 6.1. Applying that theorem to (7.9) shows that the product of reLr_e^L around every closed walk is one. Consequently there are constants ci∈C∗c_i\in\mathbb{C}^* satisfying

ci=cjreLfor every oriented edge e:i→j.c_i=c_jr_e^L\qquad\text{for every oriented edge }e:i\to j.

For completeness, choose a spanning tree in each connected component, set ci=1c_i=1 at one vertex, and determine the other constants along its tree paths. Every additional edge is consistent because it closes a walk with product one. A loop imposes precisely reL=1r_e^L=1, already proved.

The forms ciθi⊗Lc_i\theta_i^{\otimes L} now have equal residues on every pair of conductor branches. Regard their tuple as a rational aa-canonical form σ\sigma on XX: it is an element of the product of the degree-aa canonical lines of the component function fields, a rank-one module over the total quotient ring ∏iC(Xi)\prod_i\mathbb{C}(X_i). At every normal codimension-one point, its divisor says that it generates the line corresponding to aDaD.

A conductor cycle represented by birational maps between minimal strata

Figure 1. A conductor cycle represented by birational maps between minimal strata. Each dashed box groups two choices inside one dlt component; it does not depict geometric intersections. The arrows are birational comparisons, labelled by their pullback multipliers. Their composition acts on A1+A_1^{+} with multiplier re1re2re3r_{e_1}r_{e_2}r_{e_3}.

At each generic node, its branches are generators and have matching residues, so the local rule (7.7) makes it a generator there as well; aa is even and BB avoids those points.

We explain why this proves Cartierness, rather than only triviality after normalization. Choose a big open immersion j:U↪Xj: U \hookrightarrow X containing all codimension-one points, such that XX is Gorenstein on UU, aBaB is Cartier on UU, and the preceding local comparisons make σ\sigma a generator of

La,U=ωU⊗a(aB∣U).\mathcal L_{a,U}=\omega_U^{\otimes a}(aB|_U).

The divisorial sheaf associated with aDaD is its S2S_2 extension Fa=j∗La,U\mathcal{F}_a = j_*\mathcal{L}_{a,U}. The generator identifies this sheaf with j∗OU=OXj_*\mathcal{O}_U = \mathcal{O}_X, the last equality following from S2S_2. Hence Fa\mathcal{F}_a is invertible. Equivalently, divide σ\sigma by the aath power of a rational canonical form, chosen to generate at the generic nodes. The ratio is an invertible element of the total quotient ring whose principal divisor is −aD-aD on UU and therefore on XX. Thus aDaD is principal Cartier. Isolated vertices of the conductor graph cause no difficulty: their chosen forms already satisfy the required condition.

Finally let the ground field kk be any algebraically closed field of characteristic zero. All the data descend to an algebraically closed subfield k0⊂kk_0 \subset k of finite transcendence degree over Q\mathbb{Q}, including the normalization, conductor, a principal Cartier multiple of DD, and a log resolution of the normalized pair. The field k0k_0 embeds in C\mathbb{C}. The hypotheses persist under these algebraically closed field extensions: S2S_2 and the smooth or nodal codimension-one charts are preserved, normalization and conductor commute with them, and the coefficients on the chosen log resolution test log canonicity after extension. We therefore obtain the degree-aa conclusion over C\mathbb{C} with the same integer (7.10).

On a fixed big Gorenstein open over k0k_0, form Fa\mathcal{F}_a as above. The open immersion is quasi-compact and separated, since XX is noetherian. Flat base change for quasi-coherent sheaves therefore shows that this extension by j∗j_* commutes with field extension, so its pullback to C\mathbb{C} is trivial. Invertibility descends faithfully flatly. For the resulting line bundle, proper cohomology and field extension identify its space of global sections after extension with H0(XC,OXC)=CH^0(X_{\mathbb{C}},\mathcal{O}_{X_{\mathbb{C}}}) = \mathbb{C}. Its one-dimensional space over k0k_0 therefore has a nonzero section whose evaluation becomes an isomorphism over C\mathbb{C} and hence is already an isomorphism over k0k_0. Thus Fa≃O\mathcal{F}_a \simeq\mathcal{O} over k0k_0, and extending to kk proves the theorem.

References

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