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7.1.1. Tian-Yau spaces and their asymptotic rates [03IY]

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7.1.1. Tian-Yau spaces and their asymptotic rates

To start with, for two positive integers

(7.1) b−,b+∈{1,2,…,9},b_{-},b_{+}\in\{1,2,\ldots,9\},

let (Xb−4,gb−,q−)(X_{b_{-}}^{4},g_{b_{-}},q_{-}) and (Xb+4,gb+,q+)(X_{b_{{}_{+}}}^{4},g_{b_{+}},q_{+}) be fixed hyperkähler Tian-Yau spaces with reference points q−∈Xb−4q_{-}\in X_{b_{-}}^{4} and q+∈Xb+4q_{+}\in X_{b_{+}}^{4} such that their degrees are b−b_{-} and b+b_{+} respectively. See Section 3 for the definition of a Tian-Yau space and the natural coordinate outside a large compact subset. On (Xb−4,gb−,q−)(X_{b_{-}}^{4},g_{b_{-}},q_{-}) and (Xb+4,gb+,q+)(X_{b_{+}}^{4},g_{b_{+}},q_{+}), there are diffeomorphisms

(7.2) Φ±:[ζ0±,+∞)×Nilb±3→Xb±4∖K±\Phi_{\pm}:[\zeta_{0}^{\pm},+\infty)\times\Nil_{b_{\pm}}^{3}\rightarrow X_{b_{\pm}}^{4}\setminus K_{\pm}

between the Gibbons-Hawking space which models over a flat cylinder 𝕋2×ℝ\mathbb{T}^{2}\times\mathbb{R}. We define the definite constants D0±D_{0}^{\pm} by

(7.3) D0±≡The distance between​q±​and the level set​{𝒙∈Xb±4|z±​(𝒙)=ζ0±}.\displaystyle D_{0}^{\pm}\equiv\text{The distance between}\ q_{\pm}\ \text{and the level set}\ \{\bm{x}\in X_{b_{\pm}}^{4}|z_{\pm}(\bm{x})=\zeta_{0}^{\pm}\}.

Proposition 3.4 shows that there are some positive constants

(7.4) δ¯1>0,δ¯2>0\dl>0,\ \dr>0

such that for any k∈ℕk\in\mathbb{N},

(7.5) |∇g𝒞±k(Φ∗​ωT​Y±−ω𝒞±)|g𝒞±=O⁡(e−δ¯1⁡z±),|\nabla_{g_{\mathcal{C}}^{\pm}}^{k}(\Phi^{*}\omega_{TY}^{\pm}-\omega_{\mathcal{C}}^{\pm})|_{g_{\mathcal{C}}^{\pm}}=O(e^{-\dl z_{\pm}}),

where ωT​Y±\omega_{TY}^{\pm}, ω𝒞±\omega_{\mathcal{C}}^{\pm} are the Kähler forms on the Tian-Yau spaces Xb±4X_{b_{\pm}}^{4},and the Calabi model spaces respectively.

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