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Introduction [014P]

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Introduction

As is well-known, there is a natural bijection between (smooth, positive) volume forms on a complex manifold and smooth Hermitian metrics on its canonical bundle. Consequently, the data of a smooth family (νt)t∈𝔻∗(\nu_{t})_{t\in{\mathbb{D}}^{*}} of volume forms on a holomorphic family (Xt)t∈𝔻∗(X_{t})_{t\in{\mathbb{D}}^{*}} of compact complex manifolds is equivalent to that of a proper holomorphic submersion π:X→𝔻∗\pi\colon X\to{\mathbb{D}}^{*} together with a smooth metric ψ\psi on the relative canonical bundle KX/𝔻∗K_{X/{\mathbb{D}}^{*}}.

We say that the family (νt)(\nu_{t}) has analytic singularities at t=0t=0 if the following conditions hold:

  • (i)

    π:X→𝔻∗\pi\colon X\to{\mathbb{D}}^{*} is meromorphic at 0∈𝔻0\in{\mathbb{D}} in the sense that it extends to a proper, flat map π:𝒳→𝔻\pi\colon{\mathcal{X}}\to{\mathbb{D}}, with 𝒳{\mathcal{X}} normal;

  • (ii)

    𝒳{\mathcal{X}} can be chosen so that KX/𝔻∗K_{X/{\mathbb{D}}^{*}} extends to a ℚ{\mathbb{Q}}-line bundle ℒ{\mathcal{L}} on 𝒳{\mathcal{X}}, and ψ\psi extends continuously to ℒ{\mathcal{L}}.

When (i) holds, we call 𝒳{\mathcal{X}} a model of XX. Using resolution of singularities, we can always choose 𝒳{\mathcal{X}} as an snc model, that is, 𝒳{\mathcal{X}} is smooth and 𝒳0=∑i∈Ibi​Ei{\mathcal{X}}_{0}=\sum_{i\in I}b_{i}E_{i} has simple normal crossing support. To 𝒳{\mathcal{X}} is then associated a dual complex Δ⁡(𝒳)\Delta({\mathcal{X}}), with one vertex eie_{i} for each EiE_{i}, and a face σ\sigma for each connected component YY of a non-empty intersection EJ=⋂i∈JEiE_{J}=\bigcap_{i\in J}E_{i} with J⊂IJ\subset I.

In the spirit of the Morgan-Shalen topological compactification of affine varieties [MS84], we introduce a natural “hybrid” space

𝒳hyb:=X​∐Δ⁡(𝒳){\mathcal{X}}^{\mathrm{hyb}}:=X\coprod\Delta({\mathcal{X}})

associated to 𝒳{\mathcal{X}}; it is equipped with a topology defined in terms of a tropicalization map X→Δ⁡(𝒳)X\to\Delta({\mathcal{X}}), measuring the logarithmic rate of convergence of local coordinates compatible with 𝒳0{\mathcal{X}}_{0}.

Our first main result says that, after normalizing to unit mass, the volume forms νt\nu_{t} admit a “tropical” limit inside 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}}.

Theorem A.

Let (νt)t∈𝔻∗(\nu_{t})_{t\in{\mathbb{D}}^{*}} be a family of volume forms on a holomorphic family X→𝔻∗X\to{\mathbb{D}}^{*} of compact complex manifolds, with analytic singularities at t=0t=0. The asymptotic behavior of the total mass of νt\nu_{t} is then given by

νt​(Xt)∼c​|t|2​κmin​(log⁡|t|−1)d\nu_{t}(X_{t})\sim c|t|^{2\kappa_{\min}}(\log|t|^{-1})^{d}

with c∈ℝ+∗c\in{\mathbb{R}}_{+}^{*}, κmin∈ℚ\kappa_{\min}\in{\mathbb{Q}} and d∈ℕ∗d\in{\mathbb{N}}^{*}, where d≤n:=dimXtd\leq n:=\dim X_{t}. Further, given any snc model 𝒳→𝔻{\mathcal{X}}\to{\mathbb{D}} of X→𝔻∗X\to{\mathbb{D}}^{*} such that KX/𝔻∗K_{X/{\mathbb{D}}^{*}} extends to a ℚ{\mathbb{Q}}-line bundle on ℒ{\mathcal{L}} on 𝒳{\mathcal{X}} and ψ\psi extends to a continuous metric on ℒ{\mathcal{L}}, the rescaled measures

μt:=νt|t|2​κmin​(2​π​log⁡|t|−1)d,\mu_{t}:=\frac{\nu_{t}}{|t|^{2\kappa_{\min}}(2\pi\log|t|^{-1})^{d}},

viewed as measures on 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}}, converge weakly to a Lebesgue type measure μ0\mu_{0} on a dd-dimensional subcomplex Δ⁡(ℒ)\Delta({\mathcal{L}}) of Δ⁡(𝒳)\Delta({\mathcal{X}}).

The invariant κmin\kappa_{\min} and the subcomplex Δ⁡(ℒ)\Delta({\mathcal{L}}) only depend on ℒ{\mathcal{L}} (and not on the metric on ℒ{\mathcal{L}}). Consider the logarithmic relative canonical bundle

K𝒳/𝔻log:=K𝒳+𝒳0,red−π∗​(K𝔻+[0])=K𝒳/𝔻+𝒳0,red−𝒳0K^{\mathrm{log}}_{{\mathcal{X}}/{\mathbb{D}}}:=K_{\mathcal{X}}+{\mathcal{X}}_{0,\mathrm{red}}-\pi^{*}(K_{{\mathbb{D}}}+[0])=K_{{\mathcal{X}}/{\mathbb{D}}}+{\mathcal{X}}_{0,\mathrm{red}}-{\mathcal{X}}_{0}

and write K𝒳/𝔻log=ℒ+∑i∈Iai​EiK^{\mathrm{log}}_{{\mathcal{X}}/{\mathbb{D}}}={\mathcal{L}}+\sum_{i\in I}a_{i}E_{i} with ai∈ℚa_{i}\in{\mathbb{Q}}. Setting κi:=ai/bi\kappa_{i}:=a_{i}/b_{i}, we then have κmin=mini∈I⁡κi\kappa_{\min}=\min_{i\in I}\kappa_{i}, and Δ⁡(ℒ)\Delta({\mathcal{L}}) is the subcomplex of Δ⁡(𝒳)\Delta({\mathcal{X}}) whose vertices eie_{i} correspond to those i∈Ii\in I achieving the minimum.

On the other hand, the limit measure μ0\mu_{0} does depend on ψ\psi; it is given by

μ0=∑σ(∫YσResYσ⁡(ψ))​bσ−1​λσ.\mu_{0}=\sum_{\sigma}\left(\int_{Y_{\sigma}}\operatorname{Res}_{Y_{\sigma}}(\psi)\right)b_{\sigma}^{-1}\lambda_{\sigma}.

Here, σ\sigma ranges over the dd-dimensional faces of Δ⁡(ℒ)\Delta({\mathcal{L}}), with corresponding strata Yσ⊂𝒳0Y_{\sigma}\subset{\mathcal{X}}_{0}, ResYσ⁡(ψ)\operatorname{Res}_{Y_{\sigma}}(\psi) is a naturally defined residual positive measure on YσY_{\sigma}, λσ\lambda_{\sigma} is the Lebesgue measure of σ\sigma normalized by its natural integral affine structure, and bσ∈ℤ>0b_{\sigma}\in{\mathbb{Z}}_{>0} is an arithmetic coefficient.

The study of the asymptotics of integrals is a very classical subject and has been pursued by many people; see for example the book [AGZV88]. The assertions in Theorem A are closely related to results by Chambert-Loir and Tschinkel (who also worked over general local fields and in an adelic setting). Specifically, the estimate for νt​(Xt)\nu_{t}(X_{t}), suitably averaged over tt, is essentially equivalent to [CLT10, Theorem 1.2]. It also appears in [KS01, §3.1] and is exploited in [BHJ16].

The convergence result for the measures μt\mu_{t} is also closely related to [CLT10, Corollary 4.8], where, however, the limit measure lives on 𝒳0{\mathcal{X}}_{0} and not on Δ⁡(𝒳)\Delta({\mathcal{X}}).11 1 A. Chambert-Loir has pointed out that [CLT10, Corollary 4.8] is sufficiently precise, so that when applying it to toric blowups of 𝒳{\mathcal{X}} one can see the form of the limit measure μ0\mu_{0} in Theorem A. The main new feature of Theorem A is the precise and explicit convergence of the measure μt\mu_{t} to a “tropical” limit μ0\mu_{0}, living on a simplicial complex.

The following examples illustrate Theorem A. First consider the subvariety

𝒳:={(z0n+1+⋯+znn+1)+εtz0⋅…⋅zn=0}⊂ℂ×ℙn,{\mathcal{X}}:=\{(z_{0}^{n+1}+\dots+z_{n}^{n+1})+\varepsilon tz_{0}\cdot\ldots\cdot z_{n}=0\}\subset{\mathbb{C}}\times{\mathbb{P}}^{n},

where 0<ε≪10<\varepsilon\ll 1. Write X:=pr1−1​(ℂ∗)X:=\mathrm{pr}_{1}^{-1}({\mathbb{C}}^{*}). The fiber XtX_{t} over t∈𝔻∗t\in{\mathbb{D}}^{*} is a Calabi-Yau manifold, and we can choose a nonvanishing holomorphic nn-form ηt\eta_{t} on XtX_{t} to define a smooth metric ψ\psi on KX/𝔻∗K_{X/{\mathbb{D}}^{*}} that extends continuously to ℒ=K𝒳/𝔻{\mathcal{L}}=K_{{\mathcal{X}}/{\mathbb{D}}}. In the terminology of Theorem A we have νt:=2−n​in2​ηt∧η¯t\nu_{t}:=2^{-n}i^{n^{2}}\eta_{t}\wedge\overline{\eta}_{t}. Here 𝒳0{\mathcal{X}}_{0} is smooth, so Δ⁡(𝒳)\Delta({\mathcal{X}}) is a single point. Thus νt​(Xt)∼c\nu_{t}(X_{t})\sim c for some c>0c>0, and the limit measure μ0\mu_{0} is a point mass.

Now consider instead

𝒳:={tε(z0n+1+⋯+znn+1)+z0⋅…⋅zn=0}⊂ℂ×ℙn.{\mathcal{X}}:=\{t\varepsilon(z_{0}^{n+1}+\dots+z_{n}^{n+1})+z_{0}\cdot\ldots\cdot z_{n}=0\}\subset{\mathbb{C}}\times{\mathbb{P}}^{n}.

In this case, Δ⁡(ℒ)=Δ⁡(𝒳)\Delta({\mathcal{L}})=\Delta({\mathcal{X}}) is a union of (n+1)(n+1) simplices of dimension nn, and topologically a sphere. We have νt​(Xt)∼c​(log⁡|t|−1)n\nu_{t}(X_{t})\sim c(\log|t|^{-1})^{n} and the limit measure is a weighted sum of Lebesgue measures on each simplex. In fact, it is clear by symmetry that the weights are equal; this also follows from Theorem C below.

We also prove a logarithmic version of Theorem A, for a log smooth klt pair (X,B)(X,B), and a metric ψ\psi on K(X,B)/𝔻∗K_{(X,B)/{\mathbb{D}}^{*}}, see Theorem 8.4.

The space 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}} and the measure μ0\mu_{0} depend on the choice of snc model 𝒳{\mathcal{X}}. We obtain a more canonical situation by considering all possible snc models simultaneously. Namely, the set of snc models of XX is directed, and in §4 we define a locally compact (Hausdorff) topological space

Xhyb:=lim←𝒳⁡𝒳hyb,X^{\mathrm{hyb}}:=\varprojlim_{\mathcal{X}}{\mathcal{X}}^{\mathrm{hyb}},

fibering over 𝔻{\mathbb{D}}, with central fiber X0hyb:=lim←⁡Δ⁡(𝒳)X^{\mathrm{hyb}}_{0}:=\varprojlim\Delta({\mathcal{X}}). For any 𝒳{\mathcal{X}}, the dual complex Δ⁡(𝒳)\Delta({\mathcal{X}}) embeds in the central fiber X0hybX^{\mathrm{hyb}}_{0} of XhybX^{\mathrm{hyb}}.

Corollary B.

With assumptions and notation as in Theorem A, the measures μt\mu_{t}, viewed as measures on XhybX^{\mathrm{hyb}}, converge weakly to a measure μ0\mu_{0}. Further, μ0\mu_{0} is a Lebesgue type measure on a dd-dimensional complex in X0hybX^{\mathrm{hyb}}_{0}.

Now consider the case when X→𝔻∗X\to{\mathbb{D}}^{*} is projective. As we now explain, the central fiber of XhybX^{\mathrm{hyb}} is then a non-Archimedean space. Namely, XX induces a smooth projective variety XKX_{K} over the non-Archimedean field KK of complex formal Laurent series, to which we can associate a Berkovich analytification XKanX_{K}^{\mathrm{an}}. Similarly, any projective snc model 𝒳→𝔻{\mathcal{X}}\to{\mathbb{D}} of XX induces a projective model 𝒳R{\mathcal{X}}_{R} over the valuation ring RR of KK. The dual complex Δ⁡(𝒳)\Delta({\mathcal{X}}) then has a canonical realization as a compact ℤ{\mathbb{Z}}-PA subspace Sk⁡(𝒳)⊂XKan\operatorname{Sk}({\mathcal{X}})\subset X_{K}^{\mathrm{an}}, the skeleton of 𝒳{\mathcal{X}}. In fact, it is well known (see e.g. [BFJ16]) that there is a homeomorphism XKan​→∼​lim←𝒳⁡Sk⁡(𝒳)X_{K}^{\mathrm{an}}\overset{\sim}{\to}\varprojlim_{\mathcal{X}}\operatorname{Sk}({\mathcal{X}}), so we can identify the central fiber of the space XhybX^{\mathrm{hyb}} with the analytification XKanX_{K}^{\mathrm{an}}. In fact, as shown in Appendix A.6, using ideas from [Berk09], we can view the restriction of Xhyb→𝔻X^{\mathrm{hyb}}\to{\mathbb{D}} to a closed subdisc 𝔻¯r\overline{{\mathbb{D}}}_{r} as the analytification of the base change of XX to a suitable Banach ring ArA_{r}.

Assuming X→𝔻∗X\to{\mathbb{D}}^{*} is projective, we can describe the limit measure μ0\mu_{0} and its support Sk⁡(ℒ)≃Δ⁡(ℒ)\operatorname{Sk}({\mathcal{L}})\simeq\Delta({\mathcal{L}}) inside XKanX_{K}^{\mathrm{an}} in more detail. The skeleton Sk⁡(ℒ)\operatorname{Sk}({\mathcal{L}}) is of purely non-Archimedean nature, and can be seen as a mild generalization of the Kontsevich–Soibelman skeleton introduced in [KS06] and studied in [MN15, NX13, NX16]. The skeletal measure μ0\mu_{0}, on the other hand, depends on both Archimedean and non-Archimedean data. Namely, it is supported on the skeleton Sk⁡(ℒ)\operatorname{Sk}({\mathcal{L}}), but depends on the choice of metric on the restriction of the line bundle ℒ{\mathcal{L}} to the central fiber 𝒳0{\mathcal{X}}_{0} (viewed as a complex space) of any snc model 𝒳{\mathcal{X}}.

We also study both the skeleton and the skeletal measure in the more general case when the model 𝒳{\mathcal{X}} is allowed to have mild (dlt) singularities.

One major motivation for studying the above general setting comes from degenerations of Calabi–Yau manifolds. Thus suppose X→𝔻∗X\to{\mathbb{D}}^{*} is a projective holomorphic submersion, meromorphic at 0∈𝔻0\in{\mathbb{D}}, such that KX/𝔻∗=𝒪XK_{X/{\mathbb{D}}^{*}}={\mathcal{O}}_{X}. Any trivializing section η∈H0​(X,KX/𝔻∗)\eta\in H^{0}(X,K_{X/{\mathbb{D}}^{*}}) then defines a family ηt:=η|Xt\eta_{t}:=\eta|_{X_{t}} of trivializations of KXtK_{X_{t}}, and hence a smooth family of volume forms νt:=|ηt|2\nu_{t}:=|\eta_{t}|^{2} with analytic singularities at t=0t=0. Indeed, for any snc model 𝒳→𝔻{\mathcal{X}}\to{\mathbb{D}}, η\eta extends to a nowhere vanishing section of ℒ:=𝒪𝒳{\mathcal{L}}:={\mathcal{O}}_{\mathcal{X}}, and ψ:=log⁡|η|\psi:=\log|\eta| defines a smooth metric on ℒ{\mathcal{L}}.

The total mass νt​(Xt)=∫Xt|ηt|2\nu_{t}(X_{t})=\int_{X_{t}}|\eta_{t}|^{2} is then nothing but the L2L^{2} (or Hodge) metric on the direct image of KX/𝔻∗K_{X/{\mathbb{D}}^{*}}, whose asymptotic behavior at t=0t=0 is described in a very precise way by Schmid’s nilpotent orbit theorem [Sch73, Theorem 4.9] (compare for instance [GTZ13b, Proposition 2.1]).

On the other hand, the skeleton Sk⁡(ℒ)\operatorname{Sk}({\mathcal{L}}) described above coincides in the current context with the Kontsevich–Soibelman skeleton Sk⁡(X)\operatorname{Sk}(X) [KS06, MN15, NX13]. Its dimension dd, which features as the exponent of the log term in the asymptotics of the mass, measures how “bad” the degeneration is. Further, the family X→𝔻∗X\to{\mathbb{D}}^{*} admits a relative minimal model 𝒳{\mathcal{X}}, with certain mild (dlt) singularities [KNX15], and the essential skeleton can be identified with the dual complex of 𝒳{\mathcal{X}} [NX13]. In particular, d=0d=0 if and only if XX can filled in with a central fiber 𝒳0{\mathcal{X}}_{0} which is a Calabi–Yau variety with canonical singularities.

At the other end of the spectrum, d=n=dimXtd=n=\dim X_{t} if and only if XX is maximally degenerate, i.e. a “large complex structure limit”. In that case, the essential skeleton Sk⁡(X)\operatorname{Sk}(X) is shown to be a pseudomanifold in [NX13]. Building on this, we prove:

Theorem C.

Let X→𝔻∗X\to{\mathbb{D}}^{*} be a smooth projective family of Calabi–Yau varieties, meromorphic at 0∈𝔻0\in{\mathbb{D}}. Assume that XX is maximally degenerate and has semistable reduction. Then the skeletal measure μ0\mu_{0} is a multiple of the integral affine Lesbesgue measure on Sk⁡(X)\operatorname{Sk}(X).

This theorem also holds in the purely non-Archimedean setting of Calabi–Yau varieties defined over the field of Laurent series. The semistable reduction condition means that XX admits an snc model 𝒳{\mathcal{X}} with 𝒳0{\mathcal{X}}_{0} reduced. This condition is always satisfied after a finite base change.

Theorem C describes measure-theoretic degenerations of Calabi–Yau varieties. Let us briefly discuss the case of metric degenerations. Consider a smooth projective family X→𝔻∗X\to{\mathbb{D}}^{*} of Calabi–Yau varieties, meromorphic at 0∈𝔻0\in{\mathbb{D}}, and suppose the family is polarized, that is, we are given a relative ample line bundle AA on XX. By Yau’s theorem [Yau78], each fiber XtX_{t} carries a unique Ricci-flat Kähler metric ωt\omega_{t} in the cohomology class of AtA_{t}.

By [Wan03, Tos15, Taka15], the diameter DtD_{t} of (Xt,ωt)(X_{t},\omega_{t}) remains bounded if and only if d=0d=0, that is, XX admits a model 𝒳{\mathcal{X}} such that 𝒳0{\mathcal{X}}_{0} has klt singularities. In this case, it is shown in [RZ11, RZ13], building in part on [DS14], that (Xt,ωt)(X_{t},\omega_{t}) converges in the Gromov-Hausdorff sense to the Calabi–Yau variety 𝒳0{\mathcal{X}}_{0}, endowed with the metric completion of its singular Ricci-flat Kähler metric in the sense of [EGZ09].

The maximally degenerate case d=nd=n is the object of the Kontsevich–Soibelman conjecture [KS06]22 2 Essentially the same conjecture was stated independently by Gross–Wilson [GW00] and Todorov., which states that (Xt,Dt−2​ωt)(X_{t},D_{t}^{-2}\omega_{t}) (which has diameter one) converges in the Gromov-Hausdorff sense to the essential skeleton Sk⁡(X)\operatorname{Sk}(X) endowed with a piecewise smooth metric of Monge-Ampère type, i.e. locally given as the Hessian of a convex function satisfying a real Monge-Ampère equation. This conjecture has been verified for abelian varieties see e.g. [Oda14] but is largely open in general. The “mirror” situation, when one fixes the complex structure and degenerates the cohomology class of the Ricci-flat Kähler metric (along a line segment in the Kähler cone), is better understood [GW00, Tos09, Tos10, GTZ13a, GTZ13b, HT14, TWY14]. By performing a “hyper-Kähler rotation”, this implies a version of the Kontsevich–Soibelman conjecture for special cases of Type III degenerations of K3 surfaces [GW00].

Theorems A and C indicate a possible approach to the Kontsevich–Soibelman conjecture. Indeed, recall that the metric ωt\omega_{t} for t∈𝔻∗t\in{\mathbb{D}}^{*} is constructed as the curvature form of a smooth metric ϕt\phi_{t} on AtA_{t}, where ϕt\phi_{t} in turn is obtained as a solution of the complex Monge-Ampère equation MA⁡(ϕt)=μt\operatorname{MA}(\phi_{t})=\mu_{t}.

On the central fiber X0hyb=XKanX^{\mathrm{hyb}}_{0}=X_{K}^{\mathrm{an}} of XhybX^{\mathrm{hyb}}, it was shown in [BFJ15] that there exists a metric on the line bundle AKanA_{K}^{\mathrm{an}}, unique up to scaling, solving the non-Archimedean Monge-Ampère equation MA⁡(ϕ0)=μ0\operatorname{MA}(\phi_{0})=\mu_{0} (at least when XX is defined over an algebraic curve). It is now tempting to approach the Kontsevich–Soibelman conjecture by studying the behavior of ϕt\phi_{t} as t→0t\to 0. However, this seems to be a delicate issue since there is no a priori reason why the weak continuity at t=0t=0 of t↦μtt\mapsto\mu_{t} would imply continuity of the solutions t↦ϕtt\mapsto\phi_{t}.

Instead of Calabi-Yau manifolds, it would be interesting to study degenerating families X→𝔻∗X\to{\mathbb{D}}^{*} of canonically polarized projective manifolds, where the metric on KXtK_{X_{t}} would be the Kähler-Einstein metric or the Bergman metric, and prove versions of Theorems A and C in this context.

The paper is organized as follows. After recalling various facts in §1 we define in §2 the hybrid space 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}} associated to an SNC model 𝒳{\mathcal{X}}. The proof of Theorem A is given in §3. In §4 we define the space XhybX^{\mathrm{hyb}} associated to a degeneration as an inverse limit of the spaces 𝒳hyb{\mathcal{X}}^{\mathrm{hyb}}, and prove Corollary B. Various notions of skeleta are defined and studied in §5, and in §6 we formalize the notion of a residually metrized model of the canonical bundle, and associate to such an object a positive measure on the relevant Berkovich space. Degenerations of Calabi–Yau varieties are studied in §7 where we prove Theorem C. In §8 we study various extensions, and in Appendix A we recall the Berkovich analytification of a scheme over a Banach ring.

Acknowledgement. We are very grateful to Johannes Nicaise and Chenyang Xu for explaining the behavior of Poincaré residues in the present context. We also thank Vladimir Berkovich, Antoine Chambert-Loir, Antoine Ducros and Charles Favre for useful comments leading up to this work, Bernard Teissier for help with the Hironaka flattening theorem, and Matt Baker and Valentino Tosatti for comments on a preliminary version of this manuscript. Boucksom was supported by the ANR project GRACK. Jonsson was supported by NSF grant DMS-1266207, a grant from the Knut and Alice Wallenberg foundation and a grant from the United States—Israel Binational Science Foundation.

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