2019
DOI: 10.48550/arxiv.1907.09510
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Symplectic fillings of asymptotically dynamically convex manifolds I

Zhengyi Zhou

Abstract: We consider exact fillings with vanishing first Chern class of asymptotically dynamically convex (ADC) manifolds. We construct two structure maps on positive symplectic cohomology and prove that they are independent of the filling for ADC manifolds. The invariance of the structure maps implies that vanishing of symplectic cohomology and existence of symplectic dilation are properties independent of the filling for ADC manifolds. Using them, various topological applications on symplectic fillings are obtained. … Show more

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Cited by 4 publications
(24 citation statements)
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“…As explained in [16], being terminal is equivalent to have positive minimal SFT degree for some contact forms, which is closely related to the concept of asymptotically dynamically convexity [14] 1 . In particular, the result here bears certain similarity with [20]. However, we do not assume the exact filling to have any topological properties (e.g.…”
Section: Introductionsupporting
confidence: 64%
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“…As explained in [16], being terminal is equivalent to have positive minimal SFT degree for some contact forms, which is closely related to the concept of asymptotically dynamically convexity [14] 1 . In particular, the result here bears certain similarity with [20]. However, we do not assume the exact filling to have any topological properties (e.g.…”
Section: Introductionsupporting
confidence: 64%
“…In higher dimensions, the first, third and fourth inclusions were shown to be proper by Bowden, Crowley, and Stipsicz [4], Bowden, Gironella, and Moreno [5], Massot, Niederkrüger, and Wendl [15] respectively. See also [20] for exactly fillable, almost Weinstein fillable, but not Weinstein fillable examples. The situation in dimension three differs from higher dimensions in the sense that we have gauge theoretic tools as well as better holomorphic curve theories, but also face more topological constraints.…”
Section: Introductionmentioning
confidence: 99%
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“…The above difference is simply H(γ) − H(γ), where γ is seen as a point in X. Then (19) follows from ( 11), ( 13) and (14). Now assume γ is a non-constant orbit, then γ belongs to the neck where H i = f i , Hi = F i .…”
Section: 3mentioning
confidence: 99%
“…We do not know if this can be proved using purely algebro-geometric techniques (for example by computing their log Kodaira dimensions). A simpler proof of a more general version of this fact follows from uniruledness considerations by Zhou [19], see Theorem 5.10.…”
mentioning
confidence: 98%