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Symplectic Reduction and the Homogeneous Complex Monge–Ampère Equation

机译:辛约简和齐次复蒙格-安培方程

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A Riemannian manifold ( $mathcal{M}^n $ n , g) is said to be the center of thecomplex manifold $mathcal{X}^n $ n if $mathcal{M}$ is the zero set of a smooth strictly plurisubharmonic exhaustion function ν2 on $mathcal{X}$ such that ν is plurisubharmonic and solves theMonge–Ampère equation (∂ $bar partial $ ν) n = 0 off $mathcal{M}$ , and g is induced by the canonical Kähler metric withfundamental two-form $ - sqrt { - 1} $ ∂ $bar partial $ ν2. Insisting that ν be unbounded puts severe restrictions on $mathcal{X}$ as acomplex manifold as well as on ( $mathcal{M}$ , g). It is an open problemto determine the class Riemannian manifolds that are centers of complexmanifolds with unbounded ν. Before the present work, the list of knownexamples of manifolds in that class was small. In the main result of thispaper we show, by means of the moment map corresponding to isometric actionsand the associated bundle construction, that such class is larger than originally thought and contains many metrically and diffeomorphically`exotic' examples.
机译:如果$ mathcal {M} $为$,则说黎曼流形($ mathcal {M} ^ n $ n ,g)是复流形$ mathcal {X} ^ n $ n 的中心在$ mathcal {X} $上的光滑严格多次谐波耗竭函数ν2的零集,使得ν是多次谐波并解决Monge–Ampère方程(∂$ bar部分$ν)n = 0 off $ mathcal {M} $和g由规范的Kähler度量导出,其基本形式为$-sqrt {-1} $∂$ bar部分$ν2。坚持ν是无界的,对作为复杂流形的$ mathcal {X} $以及($ mathcal {M} $,g)都施加了严格的限制。确定类别Riemannian流形是具有无界ν的复流形的中心是一个开放的问题。在当前工作之前,该类歧管的已知示例列表很小。在本文的主要结果中,我们通过与等距动作对应的矩图和相关的束构造显示,该类比最初考虑的要大,并且包含许多度量和变构的“奇异”示例。

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