ScalingStacks

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Let N≃ℤn+1N\simeq\mathbb{Z}^{n+1}, and M=Hom⁡(N,ℤ)M=\Hom(N,\mathbb{Z}), and denote Nℝ=N⊗ℝN_{\mathbb{R}}=N\otimes\mathbb{R}, Mℝ=M⊗ℝM_{\mathbb{R}}=M\otimes\mathbb{R}. We regard ℂ​ℙn+1\mathbb{CP}^{n+1} as a toric Fano manifold ℙΔ\mathbb{P}_{\Delta}, with moment polytope Δ⊂Mℝ\Delta\subset M_{\mathbb{R}} corresponding to the anticanonical class 𝒪⁡(n+2)\mathcal{O}(n+2). More explicitly Δ\Delta is the (n+1)(n+1)-simplex inside Mℝ≃{∑0n+1yi=0}⊂ℝn+2M_{\mathbb{R}}\simeq\{\sum_{0}^{n+1}y_{i}=0\}\subset\mathbb{R}^{n+2} spanned by the vertices

(n+1,−1,…−1),(−1,n+1,−1,…−1),…,(−1,…,−1,n+1);(n+1,-1,\ldots-1),(-1,n+1,-1,\ldots-1),\ldots,(-1,\ldots,-1,n+1);

in particular Δ\Delta is a reflexive integral Delzant polytope, with dual polytope

Δ∨={w∈N⊗ℝ|⟨m,w⟩≥−1,∀m∈Δ}⊂ℝn+2/ℝ(1,1,…1)\Delta^{\vee}=\{w\in N\otimes\mathbb{R}|\langle m,w\rangle\geq-1,\forall m\in\Delta\}\subset\mathbb{R}^{n+2}/\mathbb{R}(1,1,\ldots 1)

being the (n+1)(n+1)-simplex spanned by the vertices (1,0,…,0),…,(0,…,0,1)(1,0,\ldots,0),\ldots,(0,\ldots,0,1). The integral points m∈Δℤ=Δ∩Mm\in\Delta_{\mathbb{Z}}=\Delta\cap M parametrize monomials zmz^{m} in the anticanonical linear system H0​(ℙΔ,𝒪⁡(n+2))H^{0}(\mathbb{P}_{\Delta},\mathcal{O}(n+2)). We study the family of hypersurfaces

Xs={Fs(z)=∑m∈Δℤames​λ​(m)zm=0}⊂ℙΔ,s≫1.X_{s}=\{F_{s}(z)=\sum_{m\in\Delta_{\mathbb{Z}}}a_{m}e^{s\lambda(m)}z^{m}=0\}\subset\mathbb{P}_{\Delta},\quad s\gg 1. (8)

Here ama_{m} are a fixed collection of coefficients, with a0=1a_{0}=1 corresponding to the unique interior integral point 0∈Δℤ0\in\Delta_{\mathbb{Z}}. For any vertex mm of Δ\Delta, we require am≠0a_{m}\neq 0. The function λ\lambda is defined for those m∈Δℤm\in\Delta_{\mathbb{Z}} for which am≠0a_{m}\neq 0; by assumption λ⁡(0)=0\lambda(0)=0, and λ⁡(m)<0\lambda(m)<0 otherwise. The natural piecewise linear extension of λ\lambda to MℝM_{\mathbb{R}} is assumed to be concave, whose domains of linearity are by assumption simplices, producing a triangulation of Δ\Delta. Using the adjunction formula, we can write down a holomorphic volume form Ωs\Omega_{s} on XsX_{s}, such that along XsX_{s}

d​Fs∧Ωs=d​log⁡z1∧…​d​log⁡zn+1,dF_{s}\wedge\Omega_{s}=d\log z^{1}\wedge\ldots d\log z^{n+1}, (9)

with z1,z2,…​zn+1z^{1},z^{2},\ldots z^{n+1} the standard coordinates on (ℂ∗)n+1⊂ℙΔ(\mathbb{C}^{*})^{n+1}\subset\mathbb{P}_{\Delta}. We will always assume s≫1s\gg 1, and all the constants in the estimates are independent of ss.

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