2023
DOI: 10.1515/crelle-2023-0016
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Hodge theory on ALG manifolds

Abstract: We develop a Fredholm theory for the Hodge Laplacian in weighted spaces on ALG∗ manifolds in dimension four. We then give several applications of this theory. First, we show the existence of harmonic functions with prescribed asymptotics at infinity. A corollary of this is a non-existence result for ALG∗ manifolds with non-negative Ricci curvature having group Γ = … Show more

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Cited by 2 publications
(5 citation statements)
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“…In this subsection, we review the Gibbons–Hawking construction of the ALG${\rm ALG}^*$ model metric. See [10, Section 2] for more details. Let ν$\nu$ be any positive integer.…”
Section: The Model Hyperkähler Structuresmentioning
confidence: 99%
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“…In this subsection, we review the Gibbons–Hawking construction of the ALG${\rm ALG}^*$ model metric. See [10, Section 2] for more details. Let ν$\nu$ be any positive integer.…”
Section: The Model Hyperkähler Structuresmentioning
confidence: 99%
“…Proof Since (re1θ1)2$(r e^{\sqrt {-1}\theta _{1}})^2$ is invariant under ι$\iota$, by [10, Theorem 1.3], there exists a harmonic function z$z$ on X$X$ such that Φz$\Phi ^* z$ is asymptotic to (re1θ1)2$(r e^{\sqrt {-1}\theta _{1}})^2$ on M2ν(R)$\mathfrak {M}_{2\nu }(R)$. Since IMd((re1θ1)2)badbreak=badbreak−1d((re1θ1)2),$$\begin{equation} \operatorname{I}_{\mathfrak {M}}^* d ((r e^{\sqrt {-1}\theta _{1}})^2) = \sqrt {-1}d ((r e^{\sqrt {-1}\theta _{1}})^2), \end{equation}$$we have ηbadbreak≡IXdzgoodbreak−badbreak−1dzgoodbreak=O(s1+μ)$$\begin{equation} \eta \equiv \operatorname{I}_{X}^* d z - \sqrt {-1}d z = O(s^{-1 + \mu }) \end{equation}$$for all …”
Section: Classification Of Alg∗${\rm Alg}^*$ Gravitational Instantonsmentioning
confidence: 99%
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