ScalingStacks

Proof. [03JB]

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Proof.

Let (Mjn~,g~j,Γj,p~j)(\widetilde{M_{j}^{n}},\tilde{g}_{j},\Gamma_{j},\tilde{p}_{j}) be the Riemannian universal covers of (Mjn,gj)(M_{j}^{n},g_{j}) which converge to the limit product space (ℝn−1×Y,d~∞,Γ∞,p~∞)(\mathbb{R}^{n-1}\times Y,\tilde{d}_{\infty},\Gamma_{\infty},\tilde{p}_{\infty}) in the equivariant Gromov-Hausdorff topology, where Γj≡π1​(Mjn)\Gamma_{j}\equiv\pi_{1}(M_{j}^{n}) and Γj→Γ∞≤Isom⁡(ℝn−1×Y)\Gamma_{j}\to\Gamma_{\infty}\leq\Isom(\mathbb{R}^{n-1}\times Y). See Section 3 of [FY92] for the precise definition of the equivariant Gromov-Hausdorff convergence. In summary, we have the following diagram

(7.43) (Mjn~,g~j,p~j)\textstyle{(\widetilde{M_{j}^{n}},\tilde{g}_{j},\tilde{p}_{j})\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces\ignorespaces}e​q​G​H\scriptstyle{eqGH}prj\scriptstyle{\pr_{j}}ℝn−1×Y\textstyle{\mathbb{R}^{n-1}\times Y\ignorespaces\ignorespaces\ignorespaces\ignorespaces}pr∞\scriptstyle{\pr_{\infty}}(Mjn,gj,pj)\textstyle{(M_{j}^{n},g_{j},p_{j})\ignorespaces\ignorespaces\ignorespaces\ignorespaces}G​H\scriptstyle{GH}ℝn−1,\textstyle{\mathbb{R}^{n-1},}

where the covering maps prj:Mjn~→Mjn\pr_{j}:\widetilde{M_{j}^{n}}\to M_{j}^{n} converge to a natural projection map pr∞:ℝn−1×Y→ℝn−1\pr_{\infty}:\mathbb{R}^{n-1}\times Y\to\mathbb{R}^{n-1}.

The main part is to prove the claim that YY is isometric to ℝ\mathbb{R}.

Applying Cheeger-Colding’s quantitative splitting theorem (see [CC96]), the convergence assumption (7.41) implies that for any fixed R>0R>0, there are harmonic splitting maps Φj≡(uj(1),…,uj(n−1)):B10​R​(pj)→ℝn−1\Phi_{j}\equiv(u_{j}^{(1)},\ldots,u_{j}^{(n-1)}):B_{10R}(p_{j})\to\mathbb{R}^{n-1} which realize the Gromov-Hausdorff maps such that

(7.44) ∑α,β=1n−1⨏B5​R​(pj)|⟨∇uj(α),∇uj(β)⟩−δα​β|+∑α=1n−1⨏B5​R​(pj)|∇2uj(α)|2→0.\sum\limits_{\alpha,\beta=1}^{n-1}\fint_{B_{5R}(p_{j})}|\langle\nabla u_{j}^{(\alpha)},\nabla u_{j}^{(\beta)}\rangle-\delta_{\alpha\beta}|+\sum\limits_{\alpha=1}^{n-1}\fint_{B_{5R}(p_{j})}|\nabla^{2}u_{j}^{(\alpha)}|^{2}\to 0.

Let Φ~j≡(u~j(1),…,u~j(n−1))\widetilde{\Phi}_{j}\equiv(\tilde{u}_{j}^{(1)},\ldots,\tilde{u}_{j}^{(n-1)}) be the lifted harmonic functions on the universal covers, then the volume comparison theorem implies that

(7.45) ∑α,β=1n−1⨏B5​R​(p~j)|⟨∇~​u~j(α),∇~​u~j(β)⟩−δα​β|+∑α=1n−1⨏B5​R​(p~j)|∇~2​u~j(α)|2→0.\sum\limits_{\alpha,\beta=1}^{n-1}\fint_{B_{5R}(\tilde{p}_{j})}|\langle\tilde{\nabla}\tilde{u}_{j}^{(\alpha)},\tilde{\nabla}\tilde{u}_{j}^{(\beta)}\rangle-\delta_{\alpha\beta}|+\sum\limits_{\alpha=1}^{n-1}\fint_{B_{5R}(\tilde{p}_{j})}|\tilde{\nabla}^{2}\tilde{u}_{j}^{(\alpha)}|^{2}\to 0.

By the definition of the splitting maps, YY is the Gromov-Hausdorff limit of the level sets of the lifted splitting maps Φ~j−1​(0n−1)\widetilde{\Phi}_{j}^{-1}(0^{n-1}). Since Γ2​(pj)≤π1​(Mjn)\Gamma_{2}(p_{j})\leq\pi_{1}(M_{j}^{n}) is of infinite order which acts on M~jn\widetilde{M}_{j}^{n} isometrically and discretely, the limit space YY must be non-compact.

On other hand hand, notice that Φ~j−1​(0n−1)\widetilde{\Phi}_{j}^{-1}(0^{n-1}) is invariant under the deck transformation group Γj\Gamma_{j} and Γj\Gamma_{j} converge to some limiting group Γ∞≤Isom⁡(ℝn−1×Y)\Gamma_{\infty}\leq\Isom(\mathbb{R}^{n-1}\times Y) such that pr∞\pr_{\infty} is given by the quotient (ℝn−1×Y)/Γ∞=ℝn−1(\mathbb{R}^{n-1}\times Y)/\Gamma_{\infty}=\mathbb{R}^{n-1}. Hence Γ∞≤Isom⁡(Y)\Gamma_{\infty}\leq\Isom(Y) and Γ∞\Gamma_{\infty} acts homogeneously on YY.

Therefore, by standard arguments, the noncompact homogeneous space YY admits a line (see [CG72] or lemma 2.4 in [NZ16]). The Ricci curvature assumption implies that YY is isometric to ℝ\mathbb{R}. This completes the proof of the claim.

The curvature estimate (7.42) immediately follows from the ϵ\epsilon-regularity theorem for noncollapsed Einstein manifolds (for example see Section 7 in [CC97]).

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