Abstract
This paper helps to clarify the status of cylindrical contact homology, a conjectured contact invariant introduced by Eliashberg, Givental, and Hofer in 2000. We explain how heuristic arguments fail to yield a well-defined homological invariant in the presence of multiply covered curves. We then introduce a large subclass of dynamically convex contact forms in dimension 3, termed dynamically separated, and demonstrate automatic transversality holds, thereby allowing us to define the desired chain complex. The Reeb orbits of dynamically separated contact forms satisfy a uniform growth condition on their Conley–Zehnder index under iteration, typically up to large action; see Definition 1.15. These contact forms arise naturally as perturbations of Morse–Bott contact forms such as those associated to \(S^1\)-bundles. In subsequent work, we give a direct proof of invariance for this subclass and, when further proportionality holds between the index and action, powerful geometric computations in a wide variety of examples.
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Notes
Nondegeneracy of the contact form means that all the Reeb orbits associated to the Reeb vector field \(R_\alpha \) are nondegenerate; see below.
Simple is synonymous with embedded in other literature.
The symplectization of \((M,\alpha )\) is given by the manifold \(\mathbb {R}\times M\) and symplectic form
$$\begin{aligned} \omega = e^\tau (d\alpha - \alpha \wedge d\tau ) = d (e^\tau \alpha ). \end{aligned}$$Here \(\tau \) is the coordinate on \(\mathbb {R}\) and \(\alpha \) is understood to be the 1-form on \(\mathbb {R}\times M\), obtained via pullback under the projection \(\mathbb {R}\times M \rightarrow M\) and \({J}\) is an \(\alpha \) -compatible almost complex structure; see Definition 2.1.
Note that when considering genus 0 domains, we can alternatively fix a standard \(j_0\) on \(\Sigma :=S^2\) and only keep track of the location of the punctures.
Note that \((S^2 {\setminus } \{x\}, j_0)\) is biholomorphic to \((\mathbb {C}, j_0)\), hence the terminology plane.
The different ways of defining differential is rather ambiguous in older literature.
Co-oriented means that there exists a globally defined \(\alpha \in \Omega ^1(M)\) such that \(\xi = \ker \alpha \).
We use the convention \(\omega (X_H, \cdot ) = dH.\)
See Definition 4.13 for the precise definition of a building.
In [15], they only require the exclusion of contractible orbits of degree 1 in order to prove \(\partial ^2=0\) in Proposition 1.9.1. The exclusion of the contractible orbits of degree 0 and \(-1\) is necessary to obtain the existence of a chain map and the homotopy of homotopies respectively when proving invariance.
While the result is expected to be true, there appear to be problems with some details of Dragnev’s proof in [14], particularly regarding the claimed existence of certain rather special cut-off functions on page 757. Rather than rely on [14] directly, we appeal to [25, 37, 60]. It is not immediately clear whether or not the proof has a simple fix, however a complete proof should follow by modifying arguments in [2, 60, 61]. A detailed proof of the desired result in the more general setting of stable Hamiltonian structures appears in Wendl’s blog: https://symplecticfieldtheorist.wordpress.com/2014/11/27/generic-transversality-in-symplectizations-part-1/, https://symplecticfieldtheorist.wordpress.com/2014/11/27/generic-transversality-in-symplectizations-part-2/, https://symplecticfieldtheorist.wordpress.com/2014/11/28/an-easy-proof-of-the-pi-du-lemma/.
Otherwise we must keep track of a \(-1\) associated to each building component arising from the compactification \(\overline{\mathcal {M}}^{{J}}(x;z)\), which is annoying.
The smooth one parameter family of diffeomorphic contact manifolds can be obtained via the flow of the Liouville vector field \(u \frac{\partial }{\partial u} + v \frac{\partial }{\partial v}\) on \(\mathbb {C}^2 {\setminus } \{ 0 \}\), which has been appropriately reparametrized so that at time 0 one starts from \(E_-\) and lands on \(E_+\) at time 1.
Isomorphism classes of symplectic vector bundles are in a 1-1 correspondence with complex vector bundles. As a result \((\xi , \bar{J})\) is frequently said to be a complex vector bundle, and one suppresses the ‘almost’ in almost complex structure despite the fact that we do not require elements of \(\mathcal {J}\) to be integrable.
In earlier literature these were sometimes referred to as finite energy parametrized surfaces.
This includes unbranched multiply covered cylinders.
The proof of Theorem 3.7 is modeled on the blog post by Chris Wendl, https://symplecticfieldtheorist.wordpress.com/2014/12/10/somewhere-injective-vs-multiply-covered/. This was in turn modeled on the “shorter” proof of Proposition 2.5.1 [43]. The “longer” proof of Proposition 2.5.1 was adapted to give a proof of Theorem 3.7 for finite energy planes, subsuming the 11-page Appendix of [24]. This longer proof extends to asymptotically cylindrical pseudoholomorphic curves we are considering, but this paper is already long enough.
This theorem holds for almost complex manifolds with noncompact cylindrical ends approaching codimension 1 manifolds \(M_\pm \) equipped with stable Hamiltonian structures, and allows for Morse–Bott orbits.
This is in the case that the orbits are nondegenerate. If the orbits are Morse–Bott, the definition is more complicated; see [60].
Note b could be 0 since the result holds if \(u_1\) does not have any branch points.
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Acknowledgments
I thank Mohammed Abouzaid, Kai Cieliebak, Helmut Hofer, Michael Hutchings, Dusa McDuff, Joel Fish, Alex Oancea, Katrin Wehrheim, and Chris Wendl for their interest in my work and our assorted insightful discussions. I would especially like to thank Mohammed Abouzaid for being a wonderful and generous advisor as well as for his comments on my thesis, from which this paper has been extracted. I am very grateful to Michael Hutchings for showing me example 1.26 and our discussions of index calculations which gave rise to many of the results in Sect. 4; these generalized those that appeared in my thesis and spawned our joint projects [33–35]. Special thanks are due to Michael Hutchings, Janko Latschev, Dusa McDuff, Andrew McInerney, and the referee for their helpful comments on this paper.
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J. Nelson is supported by NSF grant DMS-1303903, the Bell Companies Fellowship and the Fund for Mathematics at the Institute for Advanced Study.
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Nelson, J. Automatic transversality in contact homology I: regularity. Abh. Math. Semin. Univ. Hambg. 85, 125–179 (2015). https://doi.org/10.1007/s12188-015-0112-3
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DOI: https://doi.org/10.1007/s12188-015-0112-3