ScalingStacks

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

00Q4

Proposition 3.2. (cf. [23, Prop. 3.2]) The amoebas 𝒜λs\mathcal{A}_{\lambda}^{s} converge in the Hausdorff distance to 𝒜λ∞\mathcal{A}_{\lambda}^{\infty} in the Hausdorff distance as s→∞s\to\infty. In fact

{distℝn+1(x,𝒜λ∞)≤Cs,∀x∈Logs(Xs),distℝn+1(x,Logs(Xs))≤Cs,∀x∈𝒜λ∞.\begin{cases}\text{dist}_{\mathbb{R}^{n+1}}(x,\mathcal{A}_{\lambda}^{\infty})\leq\frac{C}{s},\quad\forall x\in\text{Log}_{s}(X_{s}),\\ \text{dist}_{\mathbb{R}^{n+1}}(x,\text{Log}_{s}(X_{s}))\leq\frac{C}{s},\quad\forall x\in\mathcal{A}_{\lambda}^{\infty}.\end{cases}
00Q5

Proof. (sketch) Let x=Logs​(z)x=\text{Log}_{s}(z) and let m′∈Δℤm^{\prime}\in\Delta_{\mathbb{Z}} saturate the maximum for Lλ​(x)L_{\lambda}(x). Applying Logs\text{Log}_{s} to the inequality

|es​λ​(m′)zm′|=|−∑m≠m′amam′es​λ​(m)zm|≤Cmaxm≠m′{es​λ​(m)|zm|},|e^{s\lambda(m^{\prime})}z^{m^{\prime}}|=|-\sum_{m\neq m^{\prime}}\frac{a_{m}}{a_{m^{\prime}}}e^{s\lambda(m)}z^{m}|\leq C\max_{m\neq m^{\prime}}\{e^{s\lambda(m)}|z^{m}|\},

we see

Lλ​(x)=⟨x,m′⟩+λ⁡(m′)≤maxm≠m′⁡{⟨x,m⟩+λ⁡(m)}+Cs,L_{\lambda}(x)=\langle x,m^{\prime}\rangle+\lambda(m^{\prime})\leq\max_{m\neq m^{\prime}}\{\langle x,m\rangle+\lambda(m)\}+\frac{C}{s},

so distℝn+1​(x,𝒜λ∞)≤Cs\text{dist}_{\mathbb{R}^{n+1}}(x,\mathcal{A}_{\lambda}^{\infty})\leq\frac{C}{s}. The other inequality of the claim can be proved by constructing local models of XsX_{s} in regions whose Logs\text{Log}_{s}-images are close to x∈𝒜λ∞x\in\mathcal{A}_{\lambda}^{\infty}, and then use the implicit function theorem to show XsX_{s} is a small perturbation of these local models. ∎

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