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2.11.3. Generalisation of ALF geometry [041V]

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2.11.3. Generalisation of ALF geometry

We now discuss the problems of generalising the Taub-NUT type ℂ3\mathbb{C}^{3} to higher dimensional exotic metrics on ℂn\mathbb{C}^{n}. The key issue seems to be an extra layer of combinatorial complexity of recursive nature. This calls for a theory which deals with linear analysis on quasi-ALF geometry. Roughly put, a quasi-ALF geometry of complexity 1 asymptotically looks like a flat torus fibration over a flat base. A quasi-ALF geometry of complexity kk is a singular torus fibration, whose asymptotic behaviour away from the neighbourhood of a lower dimensional stratified singular set looks ALF, and whose behaviour transverse to the singular locus is modelled on a quasi-ALF geometry of complexity k−1k-1. We shall not attempt to make a formal definition, but merely point out that theories of a very similar flavour are much studied, such as QALE spaces by Joyce [15], and QAC spaces by Degeratu and Mazzeo [4].

A conjectural example which illustrates the main ideas is the direct generalisation of our Taub-NUT type metric to ℂn\mathbb{C}^{n} with n≥4n\geq 4. We take the holomorphic fibration

ℂn→η=z0​z1​…​zn−1ℂη,Ω=−1n−1​d​z0∧d​z1​…∧d​zn−1.\mathbb{C}^{n}\xrightarrow{\eta=z_{0}z_{1}\ldots z_{n-1}}\mathbb{C}_{\eta},\quad\Omega=\sqrt{-1}^{n-1}dz_{0}\wedge dz_{1}\ldots\wedge dz_{n-1}.

which admits the action by the diagonal torus Tn−1⊂SL​(n,ℂ)T^{n-1}\subset\text{SL}(n,\mathbb{C}). The asymptotic geometry is as follows:

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    Far away from ∪{zi=zj=0}\cup\{z_{i}=z_{j}=0\}, the metric looks like a flat Tn−1T^{n-1}-fibration over a flat base. In the holomorphic persepcitive, the fibres of η=z0​…​zn−1\eta=z_{0}\ldots z_{n-1} have a almost flat cylindrical metric on (ℂ∗)n−1(\mathbb{C}^{*})^{n-1}, and the horizontal part of the metric looks like the pullback of a Euclidean metric on ℂη\mathbb{C}_{\eta}.

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    Near ∪{zi=zj=0}\cup\{z_{i}=z_{j}=0\} but far from ∪{zi=zj=zk}\cup\{z_{i}=z_{j}=z_{k}\}, we see the Taub-NUT metric appearing in the transverse direction to ∪{zi=zj=0}\cup\{z_{i}=z_{j}=0\}.

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    Near ∪{zi=zj=zk}\cup\{z_{i}=z_{j}=z_{k}\} but far from the intersection of 4 coordinate hyperplanes, we see the Taub-NUT type ℂ3\mathbb{C}^{3} appearing in the transverse direction to ∪{zi=zj=zk}\cup\{z_{i}=z_{j}=z_{k}\}.

    …

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    Near {z1=…zn−1=0}\{z_{1}=\ldots z_{n-1}=0\} but far from {z0=0}\{z_{0}=0\}, we see the conjectural metric on ℂn−1\mathbb{C}^{n-1} appearing in the transverse direction.

The point is that if one has a sufficiently powerful linear theory which could correct the initial volume form errors to have faster than quadratic decay near infinity, then one can invoke Hein’s package to produce a global Calabi-Yau metric. The whole construction follows a clearly inductive pattern.

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