ScalingStacks

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3. Preliminary remarks

In this section we will prove a uniform diameter bound and use this to compare our results to the existing literature.

Let the setting be as in the Introduction, namely let XX be a projective Calabi-Yau n−n-fold and α∈N1​(X)ℝ\alpha\in N^{1}(X)_{\mathbb{R}} a big and nef class that is not ample. Given αt:[0,1]→𝒦¯N​S\alpha_{t}:[0,1]\to\overline{\mathcal{K}}_{NS} a smooth path such that αt∈𝒦N​S\alpha_{t}\in\mathcal{K}_{NS} for t<1t<1 and α1=α\alpha_{1}=\alpha, Yau’s Theorem [Y2] gives us a unique Ricci-flat Kähler metric ωt∈αt\omega_{t}\in\alpha_{t} for any t<1t<1. Then

−1​∂∂¯​log⁡ωtnω0n=Ric⁡(ω0)−Ric⁡(ωt)=0\sqrt{-1}\partial\overline{\partial}\log\frac{\omega_{t}^{n}}{\omega_{0}^{n}}=\mathrm{Ric}(\omega_{0})-\mathrm{Ric}(\omega_{t})=0

implies that ωtn=Ct​ω0n\omega_{t}^{n}=C_{t}\omega_{0}^{n} for some constant CtC_{t}, which is easily computed by

αtn=∫Xωtn=Ct​∫Xω0n=Ct​α0n.\alpha_{t}^{n}=\int_{X}\omega_{t}^{n}=C_{t}\int_{X}\omega_{0}^{n}=C_{t}\alpha_{0}^{n}.

In particular Ct>0C_{t}>0 and 0<limt→1Ct<∞0<\lim_{t\to 1}C_{t}<\infty, which means that the volume form of ωt\omega_{t} is uniformly equivalent to the volume form of ω0\omega_{0}. We claim that the diameter of (X,ωt)(X,\omega_{t}) is uniformly bounded above when tt approaches 11. First we need a lemma, which appears as Lemma 1.3 in [DPS1]. For the reader’s convenience, we include a proof here.

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Lemma 3.1. In the above situation, given any δ>0\delta>0 and t<1t<1, there exists an open set Ut,δ⊂XU_{t,\delta}\subset X such that its diameter with respect to ωt\omega_{t} is less than C1δ−1/2C_{1}\delta^{-1/2} and its volume with respect to ω0\omega_{0} is at least ∫Xω0n−δ\int_{X}\omega_{0}^{n}-\delta, where C1C_{1} is a constant independent of t,δt,\delta.

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Proof. First notice that

∫Xωt∧ω0n−1=αt⋅α0n−1≤C,\int_{X}\omega_{t}\wedge\omega_{0}^{n-1}=\alpha_{t}\cdot\alpha_{0}^{n-1}\leq C,

which gives a uniform L1L^{1} bound on ωt\omega_{t}. Up to covering XX by finitely many charts, we may assume that X=KX=K is a compact convex set in ℂn\mathbb{C}^{n}, and we will denote by gEg_{E} the Euclidean metric on KK. If x1,x2∈Kx_{1},x_{2}\in K, we denote by [x1,x2][x_{1},x_{2}] the segment joining them in KK, and we compute the average of the length square of [x1,x2][x_{1},x_{2}] with respect to ωt\omega_{t}, when the endpoints vary. Using Fubini’s Theorem and the Cauchy-Schwarz inequality we get

(3.1) ∫K×K(∫01ωt​((1−t)​x1+t​x2)​(x2−x1)​dt)2​d​x1​d​x2≤‖x2−x1‖gE2​∫01∫K×K|ωt​((1−t)​x1+t​x2)|​d​x1​d​x2​𝑑t≤diamgE2​(K)​22​n​(∫012∫K×K|ωt​(y+t​x2)|​𝑑y​d​x2​𝑑tCLOSE+∫121∫K×K|ωt((1−t)x1+y)|dydx1dt)≤diamgE2​(K)​22​n​VolgE​(K)​‖ωt‖L1​(K)≤C1,\begin{split}&\int_{K\times K}\left(\int_{0}^{1}\sqrt{\omega_{t}((1-t)x_{1}+tx_{2})(x_{2}-x_{1})}dt\right)^{2}dx_{1}dx_{2}\\ &\leq\|x_{2}-x_{1}\|^{2}_{g_{E}}\int_{0}^{1}\int_{K\times K}|\omega_{t}((1-t)x_{1}+tx_{2})|dx_{1}dx_{2}dt\\ &\leq\mathrm{diam}_{g_{E}}^{2}(K)2^{2n}\biggl(\int_{0}^{\frac{1}{2}}\int_{K\times K}|\omega_{t}(y+tx_{2})|dydx_{2}dt\\ &+\int_{\frac{1}{2}}^{1}\int_{K\times K}|\omega_{t}((1-t)x_{1}+y)|dydx_{1}dt\biggr)\\ &\leq\mathrm{diam}_{g_{E}}^{2}(K)2^{2n}\mathrm{Vol}_{g_{E}}(K)\|\omega_{t}\|_{L^{1}(K)}\leq C_{1},\end{split}

where C1C_{1} is a uniform constant, we changed variable y=(1−t)​x1y=(1-t)x_{1} if t≤12t\leq\frac{1}{2} and y=t​x2y=tx_{2} when t≥12t\geq\frac{1}{2} and integrated first with respect to yy. Then the set SS of pairs (x1,x2)∈K×K(x_{1},x_{2})\in K\times K such that the length of [x1,x2][x_{1},x_{2}] with respect to ωt\omega_{t} is more than (C1/δ)1/2(C_{1}/\delta)^{1/2} has Euclidean measure less than or equal δ\delta: otherwise

∫K×K(∫01ωt​((1−t)​x1+t​x2)​(x2−x1)​dt)2​d​x1​d​x2≥∫S(∫01ωt​((1−t)​x1+t​x2)​(x2−x1)​dt)2​d​x1​d​x2≥C1δ​VolgE​(S)\begin{split}&\int_{K\times K}\left(\int_{0}^{1}\sqrt{\omega_{t}((1-t)x_{1}+tx_{2})(x_{2}-x_{1})}dt\right)^{2}dx_{1}dx_{2}\\ &\geq\int_{S}\left(\int_{0}^{1}\sqrt{\omega_{t}((1-t)x_{1}+tx_{2})(x_{2}-x_{1})}dt\right)^{2}dx_{1}dx_{2}\geq\frac{C_{1}}{\delta}\mathrm{Vol}_{g_{E}}(S)\end{split}

which is more than C1C_{1}, and this contradicts (3.1). If x1∈Kx_{1}\in K we let S⁡(x1)S(x_{1}) to be the set of the x2∈Kx_{2}\in K such that (x1,x2)∈S(x_{1},x_{2})\in S, and we let QQ to be the set of the x1∈Kx_{1}\in K such that VolgE​(S⁡(x1))≥12​VolgE​(K)\mathrm{Vol}_{g_{E}}(S(x_{1}))\geq\frac{1}{2}\mathrm{Vol}_{g_{E}}(K) and RR to be the set of (x1,x2)∈S(x_{1},x_{2})\in S such that x1∈Qx_{1}\in Q. Then by Fubini’s Theorem

δ≥VolgE​(R)=∫Rd​x2​d​x1=∫Q(∫S⁡(x1)d​x2)​d​x1≥12​VolgE​(K)​VolgE​(Q),\delta\geq\mathrm{Vol}_{g_{E}}(R)=\int_{R}dx_{2}dx_{1}=\int_{Q}\left(\int_{S(x_{1})}dx_{2}\right)dx_{1}\geq\frac{1}{2}\mathrm{Vol}_{g_{E}}(K)\mathrm{Vol}_{g_{E}}(Q),

and so VolgE​(Q)≤2​δVolgE​(K).\mathrm{Vol}_{g_{E}}(Q)\leq\frac{2\delta}{\mathrm{Vol}_{g_{E}}(K)}. We let Ut,δ=K\QU_{t,\delta}=K\backslash Q. Then Ut,δU_{t,\delta} is open and if x1,x2∈Ut,δx_{1},x_{2}\in U_{t,\delta} then VolgE​(S⁡(xi))<12​VolgE​(K)\mathrm{Vol}_{g_{E}}(S(x_{i}))<\frac{1}{2}\mathrm{Vol}_{g_{E}}(K), for i=1,2i=1,2. Hence VolgE​((K\S⁡(x1))∩(K\S⁡(x2)))>0\mathrm{Vol}_{g_{E}}((K\backslash S(x_{1}))\cap(K\backslash S(x_{2})))>0 and so this set is nonempty. If yy belongs to it, then (x1,y)(x_{1},y) and (x2,y)(x_{2},y) are not in SS, which means that the lengths with respect to ωt\omega_{t} of the segments [x1,y][x_{1},y] and [y,x2][y,x_{2}] are both less than (C1/δ)1/2(C_{1}/\delta)^{1/2}. Concatenating these two segments we get a path from x1x_{1} to x2x_{2} with length less than 2​(C1/δ)1/22(C_{1}/\delta)^{1/2}. We also have that

Volω0​(Q)≤C2​VolgE​(Q)≤2​C2​δVolgE​(K).\mathrm{Vol}_{\omega_{0}}(Q)\leq C_{2}\mathrm{Vol}_{g_{E}}(Q)\leq\frac{2C_{2}\delta}{\mathrm{Vol}_{g_{E}}(K)}.

Up to adjusting the constants, this is what we want. ∎

Choose δ≤min(C12,1/2∫Xω0n)\delta\leq\min(C_{1}^{2},1/2\int_{X}\omega_{0}^{n}), and for any t<1t<1 pick any pt∈Ut,δp_{t}\in U_{t,\delta}. If we denote the metric ball of ωt\omega_{t} centered at pp and with radius rr by Bt​(p,r)B_{t}(p,r), then we get that Ut,δ⊂Bt​(pt,C2)U_{t,\delta}\subset B_{t}(p_{t},C_{2}), where C2=C1δ−1/2≥1C_{2}=C_{1}\delta^{-1/2}\geq 1. Then

∫Bt​(pt,C2)ω0n≥∫Ut,δω0n≥12​∫Xω0n,\int_{B_{t}(p_{t},C_{2})}\omega_{0}^{n}\geq\int_{U_{t,\delta}}\omega_{0}^{n}\geq\frac{1}{2}\int_{X}\omega_{0}^{n},

and so

(3.2) ∫Bt​(pt,C2)ωtn≥C3>0,\int_{B_{t}(p_{t},C_{2})}\omega_{t}^{n}\geq C_{3}>0,

for some constant C3C_{3} independent of tt. Since Ric⁡(ωt)=0\mathrm{Ric}(\omega_{t})=0, the Bishop volume comparison Theorem and (3.2) give that

(3.3) ∫Bt​(pt,1)ωtn≥∫Bt​(pt,C2)ωtnC22​n≥C4>0.\int_{B_{t}(p_{t},1)}\omega_{t}^{n}\geq\frac{\int_{B_{t}(p_{t},C_{2})}\omega_{t}^{n}}{C_{2}^{2n}}\geq C_{4}>0.

The following lemma is due to Yau (see e.g. Theorem I.4.1 in [SY]), but we provide a proof for completeness.

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Lemma 3.2. Let (M2​n,g)(M^{2n},g) be a closed Riemannian manifold with Ric⁡(g)≥0\mathrm{Ric}(g)\geq 0, let p∈Mp\in M and 1<R<diam⁡(g)1<R<\mathrm{diam}(g). Then

R−14​n≤Vol​(B​(p,2​(R+1)))Vol⁡(B⁡(p,1)).\frac{R-1}{4n}\leq\frac{\mathrm{Vol}(B(p,2(R+1)))}{\mathrm{Vol}(B(p,1))}.
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Proof. Choose x0∈∂B⁡(p,R)x_{0}\in\partial B(p,R), so that d⁡(x0,p)=Rd(x_{0},p)=R, and denote by ρ⁡(x)=d⁡(x,x0)\rho(x)=d(x,x_{0}). The Laplacian comparison theorem gives Δ​ρ2≤4​n\Delta\rho^{2}\leq 4n in the sense of distributions. Let φ⁡(x)=ψ⁡(ρ⁡(x))\varphi(x)=\psi(\rho(x)) where

ψ⁡(t)={1if 0≤t≤R−1,12​(R+1−t)if R−1<t<R+1,0if t≥R+1.\psi(t)=\left\{\begin{array}[]{lll}1&\mbox{if $0\leq t\leq R-1$},\\ \frac{1}{2}(R+1-t)&\mbox{if $R-1<t<R+1$},\\ 0&\mbox{if $t\geq R+1$}.\end{array}\right.

Then φ\varphi is a nonnegative Lipschitz function supported in B⁡(x0,R+1)B(x_{0},R+1), and we have that

∫Mφ​Δ​ρ2​d​Vg=−∫B⁡(x0,R+1)∇φ⋅∇ρ2dVg=−2∫B⁡(x0,R+1)ρ|∇ρ|2ψ′(ρ(x))dVg=∫B⁡(x0,R+1)\B⁡(x0,R−1)ρ​d​Vg≥(R−1)​Vol​(B⁡(x0,R+1)\B⁡(x0,R−1)),\begin{split}\int_{M}\varphi\Delta\rho^{2}dV_{g}&=-\int_{B(x_{0},R+1)}\nabla\varphi\cdot\nabla\rho^{2}dV_{g}=-2\int_{B(x_{0},R+1)}\rho|\nabla\rho|^{2}\psi^{\prime}(\rho(x))dV_{g}\\ &=\int_{B(x_{0},R+1)\backslash B(x_{0},R-1)}\rho dV_{g}\\ &\geq(R-1)\mathrm{Vol}(B(x_{0},R+1)\backslash B(x_{0},R-1)),\end{split}

and also

∫Mφ​Δ​ρ2​d​Vg≤4​n​∫B⁡(x0,R+1)φ​d​Vg≤4​n​Vol​(B⁡(x0,R+1)).\int_{M}\varphi\Delta\rho^{2}dV_{g}\leq 4n\int_{B(x_{0},R+1)}\varphi dV_{g}\leq 4n\mathrm{Vol}(B(x_{0},R+1)).

Notice that B⁡(p,1)⊂B⁡(x0,R+1)\B⁡(x0,R−1)B(p,1)\subset B(x_{0},R+1)\backslash B(x_{0},R-1) and so the previous two equations give

(R−1)​Vol​(B⁡(p,1))≤4​n​Vol​(B⁡(x0,R+1)).(R-1)\mathrm{Vol}(B(p,1))\leq 4n\mathrm{Vol}(B(x_{0},R+1)).

The conclusion follows from the fact that B⁡(x0,R+1)⊂B⁡(p,2​(R+1))B(x_{0},R+1)\subset B(p,2(R+1)). ∎

Lemma 3.2 gives that for any 1<R<diam⁡(ωt)1<R<\mathrm{diam}(\omega_{t}) we have

(3.4) R−14​n≤∫Bt​(pt,2​(R+1))ωtn∫Bt​(pt,1)ωtn.\frac{R-1}{4n}\leq\frac{\int_{B_{t}(p_{t},2(R+1))}\omega_{t}^{n}}{\int_{B_{t}(p_{t},1)}\omega_{t}^{n}}.

Choosing R=diam⁡(ωt)−1R=\mathrm{diam}(\omega_{t})-1 and using (3.3) we get

diam⁡(ωt)≤2+4​nC4​∫Xωtn,\mathrm{diam}(\omega_{t})\leq 2+\frac{4n}{C_{4}}\int_{X}\omega_{t}^{n},

which is bounded independent of t<1t<1, and proves our claim (a similar argument can be found in [P1]). Once we have the diameter bound, we can apply the Bishop volume comparison Theorem again and get that for any point p∈Xp\in X and any r>0r>0, t<1t<1

(3.5) ∫Bt​(p,r)ωtn≥r2​n​∫Xωtndiam​(ωt)2​n≥c​r2​n,\int_{B_{t}(p,r)}\omega_{t}^{n}\geq r^{2n}\frac{\int_{X}\omega_{t}^{n}}{\mathrm{diam}(\omega_{t})^{2n}}\geq cr^{2n},

where c>0c>0 is a uniform constant. A well-known computation in Chern-Weil theory gives

1n⁡(n−1)​∫X‖Rmt‖t2​ωtn=∫Xc2​(X,ωt)∧ωtn−2=c2​(X)⋅αtn−2≤C,\frac{1}{n(n-1)}\int_{X}\|\textrm{Rm}_{t}\|^{2}_{t}\omega_{t}^{n}=\int_{X}c_{2}(X,\omega_{t})\wedge\omega_{t}^{n-2}=c_{2}(X)\cdot\alpha_{t}^{n-2}\leq C,

where Rmt\textrm{Rm}_{t} is the Riemann curvature tensor of ωt\omega_{t} and c2​(X,ωt)c_{2}(X,\omega_{t}) is the second Chern form of ωt\omega_{t}. If n=2n=2 we can thus apply Theorem C of [An], Theorem 5.5 of [BKN] or Proposition 3.2 of [Ti] and get that a subsequence of (X,ωt)(X,\omega_{t}) converges to an Einstein orbifold with isolated singularities in the Gromov-Hausdorff topology, and also in the C∞C^{\infty} topology on compact sets outside the orbifold points. If n>2n>2 these theorems require a uniform bound on

∫X‖Rmt‖tn​ωtn,\int_{X}\|\textrm{Rm}_{t}\|^{n}_{t}\omega_{t}^{n},

which in general can not be expressed in terms of topological data as above. Instead when n>2n>2 we apply a general theorem of Gromov [Gr] that says that any sequence of compact Riemannian manifolds of dimension 2​n2n with diameter bounded above and Ricci curvature bounded below, has a subsequence that converges in the Gromov-Hausdorff topology to a compact length space. Thus a subsequence of (X,ωt)(X,\omega_{t}) converges to a compact metric space YY, and Theorem 1.15 in [CCT] says that YY is a complex manifold outside a rectifiable set R⊂YR\subset Y of real Hausdorff codimension at least 44. Moreover their Theorem 9.1 gives supporting evidence that RR should in fact be a complex subvariety of YY.

On the other hand our Theorem 1.1 gives the convergence of the whole sequence of metrics, and not just of a subsequence, and the limit metric is uniquely determined by the class α\alpha. When n>2n>2 the convergence we get is stronger than Gromov-Hausdorff convergence, but it only happens outside the singular set EE. Also, when α=c1​(L)\alpha=c_{1}(L), we see precisely who the limit space YY is, namely the Calabi-Yau model of XX associated to LL. It has canonical singularities, so its singular set is a subvariety of complex codimension at least 22, and when n=2n=2 canonical singularities are precisely rational double points, that are of orbifold type. We will discuss the case n=2n=2 with more details in section 5. Let us also mention the results of Ruan [Ru]. He studies the Gromov-Hausdorff limits of sequences of Kähler metrics on a fixed compact manifold XX, with uniformly bounded sectional curvature. Roughly speaking, he proves that there exists an analytic subvariety E⊂XE\subset X such that a subsequence of the metrics converges in the Gromov-Hausdorff topology on X\EX\backslash E to ω\omega a smooth Hermitian form, which is either Kähler (non-collapsing) or pointwise nonnegative with determinant zero (collapsing). Moreover in the collapsing case, the kernel of ω\omega gives a holomorphic foliation with singularities on XX. Unfortunately in our setting the curvature is not bounded in general, so Ruan’s results don’t apply, but our Theorem 1.1 gives in particular Ruan’s conclusion in the non-collapsing case. We’ll discuss the collapsing case in section 5.

Of course, the above-mentioned results apply in more general situations than ours. Also, all the results in this section work in the case when XX is not projective, and the ample cone is replaced by the (bigger) Kähler cone. Then the above theorems still apply, but for technical reasons our Theorem 1.1 doesn’t (see section 6 for more discussions).

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