ScalingStacks

Verified tagged author-source HTML · 1912.02360v1 · cited publication edition alignment unverified.

00QL

Proposition 3.14. As s→+∞s\to+\infty, the pushforward measure (Logs)∗​d​μs(\text{Log}_{s})_{*}d\mu_{s} converges to the Lebesgue measure d​μ∞d\mu_{\infty} supported on ∂Δλ∨\partial\Delta_{\lambda}^{\vee}. In particular

∫Xsd​μs→Vol​(∂Δλ∨)=∫∂Δλ∨d​μ∞.\int_{X_{s}}d\mu_{s}\to\text{Vol}(\partial\Delta_{\lambda}^{\vee})=\int_{\partial\Delta_{\lambda}^{\vee}}d\mu_{\infty}. (15)

Morever, there is a uniform exponential measure decay estimate

d​μs​({z∈Xs:distℝn+1​(Logs​(z),∂Δλ∨)>s−1​Λ})≤C′​e−C​Λ,∀Λ>0.d\mu_{s}(\{z\in X_{s}:\text{dist}_{\mathbb{R}^{n+1}}(\text{Log}_{s}(z),\partial\Delta_{\lambda}^{\vee})>s^{-1}\Lambda\})\leq C^{\prime}e^{-C\Lambda},\quad\forall\Lambda>0. (16)
00QM

Proof. (Sketch) Using Lemma 3.5 and the holomorphic volume form formula (13), the neighbourhood of the toric boundary near 𝒜λ,σ∞\mathcal{A}_{\lambda,\sigma}^{\infty} only contributes O⁡(s−l)O(s^{-l}) to the normalised measure, where l=dimN​CΔ​(σ)l=\dim NC_{\Delta}(\sigma). The same lemmas imply (16) by summing over contributions from boundary type regions. In the toric region corresponding to the neighbourhood of ∂Δλ∨\partial\Delta_{\lambda}^{\vee}, the convergence of the normalised volume measure follows from Prop. 3.2 and formula (12). ∎

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