ScalingStacks

Verified tagged author-source HTML · 0905.4718v1 · cited publication edition alignment unverified.

First of all let us recall our setup from the introduction: (X,ωX)(X,\omega_{X}) is a compact Kähler manifold of complex dimension nn with c1​(X)=0c_{1}(X)=0, or in other words a Calabi-Yau manifold. We have a map holomorphic map f:X→Zf:X\to Z, where (Z,ωZ)(Z,\omega_{Z}) is another compact Kähler manifold, with image Y⊂ZY\subset Z and so that f:X→Yf:X\to Y has connected fibers. YY is assumed to be an irreducible normal subvariety of ZZ of dimension mm with 0<m<n0<m<n, and we let ωY\omega_{Y} be the restriction of ωZ\omega_{Z} to the regular part of YY. We also set ω0=f∗​ωZ\omega_{0}=f^{*}\omega_{Z}, which is a smooth nonnegative (1,1)(1,1) form on XX whose cohomology class lies on the boundary of the Kähler cone. There is a proper subvariety S⊂XS\subset X such that Y\f⁡(S)Y\backslash f(S) is smooth and f:X\S→Y\f⁡(S)f:X\backslash S\to Y\backslash f(S) is a smooth submersion. Yau’s theorem [Y1] says that in each Kähler class of XX there is a unique Kähler metric with Ricci curvature identically zero. For each 0<t≤10<t\leq 1 we call ω~t\tilde{\omega}_{t} the Ricci-flat Kähler metric cohomologous to [ω0]+t⁡[ωX][\omega_{0}]+t[\omega_{X}], and we wish to study the behaviour of these metrics when tt goes to zero. On XX we have

ω0k∧ωXn−k=0,\omega_{0}^{k}\wedge\omega_{X}^{n-k}=0,

for m+1≤k≤nm+1\leq k\leq n, and

(2.1) ω0m∧ωXn−m=H​ωXn,\omega_{0}^{m}\wedge\omega_{X}^{n-m}=H\omega_{X}^{n},

where the smooth non-negative function HH vanishes precisely on SS and is such that H−γH^{-\gamma} is in L1L^{1} for some small γ>0\gamma>0. This is because HH is locally comparable to a sum of squares of holomorphic functions (the minors of the Jacobian of ff). In particular it follows that

∫Xω0m∧ωXn−m>0.\int_{X}\omega_{0}^{m}\wedge\omega_{X}^{n-m}>0.

For later purposes we need the following construction. Let ℐ\mathcal{I} be the ideal sheaf of f⁡(S)f(S) inside ZZ. We cover ZZ by a finite number of open sets UkU_{k} so that on each UkU_{k} the ideal ℐ\mathcal{I} is generated by holomorphic functions hk,jh_{k,j}, with 1≤j≤Nk1\leq j\leq N_{k}. We then fix ηk\eta_{k} a partition of unity subordinate to the covering {Uk}\{U_{k}\} and we let

(2.2) σ=∑k,jηk​|hk,j|2,\sigma=\sum_{k,j}\eta_{k}|h_{k,j}|^{2},

if S≠∅S\neq\emptyset and otherwise we just set σ=1\sigma=1. Then σ\sigma is a smooth nonnegative function on ZZ with zero locus precisely f⁡(S)f(S) and there is a constant CC so that on ZZ we have

(2.3) σ≤C,0≤−1​∂σ∧∂¯​σ≤C​ωZ,−C​ωZ≤−1​∂∂¯​σ≤C​ωZ.\sigma\leq C,\quad 0\leq\sqrt{-1}\partial\sigma\wedge\overline{\partial}\sigma\leq C\omega_{Z},\quad-C\omega_{Z}\leq\sqrt{-1}\partial\overline{\partial}\sigma\leq C\omega_{Z}.

Then for any y∈Y\f⁡(S)y\in Y\backslash f(S) we have the inequality

(2.4) σ​(y)λ≤C​infXyH,\sigma(y)^{\lambda}\leq C\inf_{X_{y}}H,

for some constants C,λC,\lambda, and we are free to enlarge λ\lambda if needed. This is because both of the function HH and f∗​σf^{*}\sigma on XX are locally comparable to a sum of squares of holomorphic functions and they both have zero set equal to SS. By taking a log resolution of the ideal sheaf of SS inside XX and we can assume that SS is a divisor with simple normal crossings, and then the holomorphic functions have well defined vanishing orders along the irreducible components of SS, and (2.4) follows.

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