ScalingStacks

003K

Proposition 6.4. [53, Lemma 4.1, 4.2] Given any ϵ≪1\epsilon\ll 1, and let tt be small enough depending on ϵ\epsilon. There is a Kähler metric ωψ,t\omega_{\psi,t}, such that

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    On Log𝒳−1​(Int​(ΔJ))\text{Log}_{\mathcal{X}}^{-1}(\text{Int}(\Delta_{J})), the local Kähler potentials ϕJ,t\phi_{J,t} of ωψ,t\omega_{\psi,t} can be chosen to satisfy |ϕJ,t−ϕ0∘Log𝒳|<ϵ|\phi_{J,t}-\phi_{0}\circ\text{Log}_{\mathcal{X}}|<\epsilon.

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    The total variation ∫Xt||log⁡|t||n​ωψ,tn(Ln)−d​μt|<ϵ.\int_{X_{t}}|\frac{|\log|t||^{n}\omega_{\psi,t}^{n}}{(L^{n})}-d\mu_{t}|<\epsilon.

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    The Kähler potential of ωψ,t\omega_{\psi,t} relative to a fixed Fubini-Study reference metric, is uniformly bounded independent of t,ϵt,\epsilon.

003L

Proof. (Sketch)

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    We first C0C^{0} approximate the NA metric ‖⋅‖C​Y\left\lVert\cdot\right\rVert_{CY} by some NA Fubini-Study metric, which arises naturally as a hybrid topology limit of usual Fubini-Study metrics on XtX_{t} (cf. section 5.3). The Fubini-Study metrics are positive, and by construction their local potentials differ from ϕ0∘Log𝒳\phi_{0}\circ\text{Log}_{\mathcal{X}} by an arbitrarily small amount in the C0C^{0} sense.

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    We do not have direct control on the volume form of the Fubini-Study metrics; the degrees of the associated projective embeddings are gigantic. In contrast, the volume form of the local potential ϕ0∘Log𝒳\phi_{0}\circ\text{Log}_{\mathcal{X}} has negligible difference from (Ln)|log⁡|t||n​d​μt\frac{(L^{n})}{|\log|t||^{n}}d\mu_{t}, by the volume asymptote in section 3.1 and the real MA equation (17).

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    The idea is to perform a further regularization. We modify the Fubini-Study metric in the generic region of XtX_{t}, so that it essentially agrees with ϕ0∘Log𝒳\phi_{0}\circ\text{Log}_{\mathcal{X}} in the generic region up to C2C^{2}-small error. In this step we appealed also to the regularity theory of real MA equation. The end result is ωψ,t\omega_{\psi,t}, which is Kähler by construction.

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    In the non-generic region, we do not perform regularization. Since the generic region already takes up 99.9%99.9\% of the ωψ,tn\omega_{\psi,t}^{n} measure for |t|≪1|t|\ll 1, the non-generic region has negligible total measure. We use this to argue for the total variation bound.

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Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.