ScalingStacks

Verified tagged author-source HTML · 1904.03696v1 · cited publication edition alignment unverified.

00ME

Proof. Recall that one can find M∈ℕM\in\mathbb{N} such that L⊗ML^{\otimes M} is very ample and for any n≥Mn\geq M, the restriction map from Vn​(L)V_{n}(L) to Vn​(L|Y)V_{n}(L|_{Y}) is surjective.

By the asymptotic Fubini-Study assumption, there exist norms {∥⋅∥n}n∈ℕ\{\lVert\mathord{\cdot}\rVert_{n}\}_{n\in\mathbb{N}} on Vn​(L)V_{n}(L) such that ϕ\phi is given by 𝒫⁡({∥⋅∥n}n∈ℕ)\mathcal{P}(\{\lVert\mathord{\cdot}\rVert_{n}\}_{n\in\mathbb{N}}). Let ψn\psi_{n} denote the metric 1n​FS​(∥⋅∥)n\frac{1}{n}\mathrm{FS}(\lVert\mathord{\cdot}\rVert)_{n} on LL. By the continuity assumption, the convergence to envelop metric is uniform (see §3.1 12.). So for any ϵ>0\epsilon>0, there exists M′≥MM^{\prime}\geq M such that

dist⁡(ψM′,ϕ)≤13​ϵ,\dist(\psi_{M^{\prime}},\phi)\leq\frac{1}{3}\epsilon,

hence for any n∈ℕn\in\mathbb{N}, one has

dist⁡(∥⋅∥n​ψM′,∥⋅∥n​ϕ)≤13​n​ϵ,dist⁡(∥⋅∥n​ψM′,X|Y,∥⋅∥n​ϕ,X|Y)≤13​n​ϵ.\dist(\lVert\mathord{\cdot}\rVert_{n\psi_{M^{\prime}}},\lVert\mathord{\cdot}\rVert_{n\phi})\leq\frac{1}{3}n\epsilon,\quad\dist(\lVert\mathord{\cdot}\rVert_{n\psi_{M^{\prime}},X|Y},\lVert\mathord{\cdot}\rVert_{n\phi,X|Y})\leq\frac{1}{3}n\epsilon.

By Corollary 5.8, the Banach algebra V^∙​(LX|Y,(ψM′)X|Y)\widehat{V}_{{\scriptscriptstyle\bullet}}(L_{X|Y},(\psi_{M^{\prime}})_{X|Y}) is an affinoid algebra. By Proposition 5.9, there exists CM′​(X,Y,ϕ)>0C_{M^{\prime}}(X,Y,\phi)>0 such that

∀t¯∈V∙(LX|Y),⦀t¯⦀ψM′,X|Y≤CM′⋅⦀t¯⦀ψM′,X|Y;sp=⦀t¯⦀ψM′,Y.\forall\underline{t}\in V_{{\scriptscriptstyle\bullet}}(L_{X|Y}),\quad\vvvert\underline{t}\vvvert_{\psi_{M^{\prime}},X|Y}\leq C_{M^{\prime}}\cdot\vvvert\underline{t}\vvvert_{\psi_{M^{\prime}},X|Y;\mathrm{sp}}=\vvvert\underline{t}\vvvert_{\psi_{M^{\prime}},Y}.

Combining this comparison with above estimates, one has that for every n≥nY:=⌈ln⁡(CM′)/(ϵ/3)⌉n\geq n_{Y}:=\lceil\ln(C_{M^{\prime}})/(\epsilon/3)\rceil

∥tn∥n​ϕ,X|Y≤e13​n​ϵ⋅∥tn∥n​ψM′,X|Y≤e13​n​ϵ⋅CM′⋅∥tn∥n​ψM′|Y≤e23​n​ϵ⋅CM′⋅∥tn∥n​ϕ|Y≤en​ϵ⋅∥tn∥n​ϕ|Y.\begin{split}\lVert t_{n}\rVert_{n\phi,X|Y}&\leq\mathrm{e}^{\frac{1}{3}n\epsilon}\cdot\lVert t_{n}\rVert_{n\psi_{M^{\prime}},X|Y}\\ &\leq\mathrm{e}^{\frac{1}{3}n\epsilon}\cdot C_{M^{\prime}}\cdot\lVert t_{n}\rVert_{n\psi_{M^{\prime}}|_{Y}}\\ &\leq\mathrm{e}^{\frac{2}{3}n\epsilon}\cdot C_{M^{\prime}}\cdot\lVert t_{n}\rVert_{n\phi|_{Y}}\\ &\leq\mathrm{e}^{n\epsilon}\cdot\lVert t_{n}\rVert_{n\phi|_{Y}}.\end{split}

Hence there exists sn∈Vn​(L)s_{n}\in V_{n}(L) with ∥sn∥n​ϕ≤en​ϵ⋅∥tn∥n​ϕ|Y\lVert s_{n}\rVert_{n\phi}\leq\mathrm{e}^{n\epsilon}\cdot\lVert t_{n}\rVert_{n\phi|_{Y}}. ∎

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