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Volume renormalization of strictly pseudoconvex domains

机译:严格伪凸域的体积重归一化

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There has been much recent activity in the area of conformal geometry and conformally compact Einstein manifolds centered around volume renormalization [?], [?]; there one considers a complete Einstein metric g+ on the interior Ω of a compact manifold with boundary Ω = Ω ∪partial derivΩ and a conformal structure [g] on partial derivΩ, which is obtained as a scaling limit of g+. For a choice of a denning function ρ such that Ω = {ρ > 0}, one can consider the volume expansion of subdomain Ω_ε = {ρ > ε} with respect to g+. If n = dim partial derivΩ is even, it takes the form Vol(Ω_ε) = Σ_(j=0)~(n/2-1) C_jε~(2j-n) + L(partial derivΩ)log ε+ (bounded term), where C_j are constants (which depend on the choice of p) and L is a conformal invariant of (partial derivΩ,[g]). Moreover, it is shown that this conformal invariant L can be expressed as the integral of Branson's Q-curvature [?], a local Riemannian invariant which naturally arises from conformally invariant differential operators. Both L and Q have been studied extensively.
机译:在保形几何学和保形紧密的爱因斯坦流形的领域中,最近有很多活动,其以体积再归一化为中心。在那里,我们考虑了一个紧凑流形的内部Ω的完整爱因斯坦度量g +,其中边界Ω=Ω∪偏导数Ω和在偏导数上的共形结构[g]作为g +的缩放极限而获得。为了选择一个使Ω= {ρ> 0}的定义函数ρ,可以考虑子域Ω_ε= {ρ>ε}相对于g +的体积膨胀。如果n =暗的偏导数Ω是偶数,则形式为Vol(Ω_ε)=Σ_(j = 0)〜(n / 2-1)C_jε〜(2j-n)+ L(偏导数)logε+(有界项),其中C_j是常数(取决于p的选择),L是(偏导数,[g])的保形不变。而且,表明该保形不变性L可以表示为布兰森Q-曲率[α]的积分,它是自然地由保形不变性微分算子产生的局部黎曼不变量。 L和Q都已被广泛研究。

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