2008
DOI: 10.2140/agt.2008.8.381
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On tight contact structures with negative maximal twisting number on small Seifert manifolds

Abstract: We study some properties of transverse contact structures on small Seifert manifolds, and we apply them to the classification of tight contact structures on a family of small Seifert manifolds.

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Cited by 25 publications
(41 citation statements)
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References 19 publications
(33 reference statements)
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“…In particular, we used the fact that the unique tight contact structure on this manifold is not supported by a planar open book. A similar argument can be made for k D 0; 1; 2; 3 to obtain rightveering, not destabilizable monodromies which support overtwisted contact structures (using the classification result in [11], which in particular says that all the tight contact structures on these manifolds are Stein fillable). However, we do not know if is overtwisted or tight for k > 4.…”
Section: An Example 41 Poincaré Homology Spherementioning
confidence: 72%
“…In particular, we used the fact that the unique tight contact structure on this manifold is not supported by a planar open book. A similar argument can be made for k D 0; 1; 2; 3 to obtain rightveering, not destabilizable monodromies which support overtwisted contact structures (using the classification result in [11], which in particular says that all the tight contact structures on these manifolds are Stein fillable). However, we do not know if is overtwisted or tight for k > 4.…”
Section: An Example 41 Poincaré Homology Spherementioning
confidence: 72%
“…The proof in [29] combines the Eliashberg-Thurston perturbation theorem with the more analytical adjunction inequality in symplectic geometry. In the case g D 0, r D 3 and b D 2, a topological proof of Theorem B by P Ghiggini appeared in [11] while this paper was in preparation.…”
Section: Introductionmentioning
confidence: 99%
“…The main invariant in the classification of tight Seifert fibered manifolds is the maximal twisting number (that is, the difference between the contact framing and the fibration framing, maximized in the smooth isotopy class of a regular fiber)applied in convex surface theory, it allows one to give upper bounds on the number of tight structures. By the results of Wu [20] all tight contact structures when e 0 ≤ −2 have negative maximal twisting, while for e 0 ≥ 0 they are all zero-twisting; in the work of Ghiggini [3] the negative maximal twisting is further related to the existence of transverse contact structures. This, in the case of L-spaces, results in a simple division: maximal twisting is equal to zero when e 0 ≥ −1, and has value −1 when e 0 ≤ −2.…”
Section: Introductionmentioning
confidence: 92%