ScalingStacks

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

00T2

Proof. (Thm. 5.10) By Thm 5.6 we already know the metric convergence over any properly contained open subset of ℛ\mathcal{R}, which corresponds to a region Us⊂XsU_{s}\subset X_{s}, with nearly the full measure:

Vol​(Us)>(1−ϵ)​Vol​(Xs),\text{Vol}(U_{s})>(1-\epsilon)\text{Vol}(X_{s}),

where ϵ\epsilon can be chosen arbitrarily small. It now suffices to show any point p∈Xs∖Usp\in X_{s}\setminus U_{s} is close to UsU_{s}. For any r>0r>0 such that the geodesic ball BgC​Y,s​(p,r)⊂Xs∖UsB_{g_{CY,s}}(p,r)\subset X_{s}\setminus U_{s}, the Bishop-Gromov inequality implies

(rdiam​(Xs))2​n≤Vol​(BgC​Y,s​(p,r))Vol​(Xs)≤Vol​(Xs∖Us)Vol​(Xs)<ϵ.\left(\frac{r}{\text{diam}(X_{s})}\right)^{2n}\leq\frac{\text{Vol}(B_{g_{CY,s}}(p,r))}{\text{Vol}(X_{s})}\leq\frac{\text{Vol}(X_{s}\setminus U_{s})}{\text{Vol}(X_{s})}<\epsilon.

Taking the sup of all such rr,

distgC​Y,s​(p,Us)≤ϵ1/2​n​diam​(Xs)≤C​ϵ1/2​n,\text{dist}_{g_{CY,s}}(p,U_{s})\leq\epsilon^{1/2n}\text{diam}(X_{s})\leq C\epsilon^{1/2n},

which can be made arbitrarily small. ∎

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