Weinstein conjecture
Canonical statement
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Let \(M^{2n-1}\) be a closed smooth manifold and let \(\alpha\) be a contact form, so \(\alpha\wedge(d\alpha)^{n-1}\) is nowhere zero. The Reeb vector field \(R_\alpha\), uniquely defined by \(\alpha(R_\alpha)=1\) and \(d\alpha(R_\alpha,\cdot)=0\), has a nonconstant periodic orbit.Notes
The Weinstein conjecture predicts that Reeb dynamics on a closed contact manifold always exhibits periodicity: if is a contact form on a closed manifold , the associated Reeb vector field must have a nonconstant periodic orbit. Weinstein raised the question in 1978, prompted by an analysis of the hypotheses in Rabinowitz's periodic-orbit theorems for Hamiltonian systems [Weinstein1979PeriodicOrbits].
In dimension three the conjecture is a theorem: Taubes proved it for every closed contact -manifold using the Seiberg–Witten equations [Taubes2007Weinstein3D], following a long line of special cases. In higher dimensions many classes of contact manifolds are known to satisfy the conjecture, and the surrounding techniques, from variational methods to holomorphic curves, are surveyed in [Ding2025WeinsteinSurvey].
The general case in dimension at least remains open: for an arbitrary contact form on an arbitrary closed manifold of dimension or more, no current argument produces a closed Reeb orbit, and a resolution would require methods that work without any restriction on the contact manifold.
References (3)
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