arXiv2015
Let $α$ be a contact form on $S^3$, let $ξ$ be its Reeb vector-field and let $v$ be a non-singular vector-field in $kerα$. Let $C_β$ be the space of curves $x$ on $S^3$ such $\dot x=aξ+bv, \dot a=0, a \gneq 0$. Let $L^+$, respectively $L^-$, be the set of curves in $C_β$ such that $b\geq 0$, respectively $b \leq 0$. Let, for $x \in C_β$, $J(x)=\int_0^1α_x(\dot x)dt$. We establish in this paper that an infinite number of cycles in the $S^1$-equivariant homology of $C_β$,{\bf relative} to $L^+ \cup L^-$ and to some specially designed "bottom set", see section 4, are achieved in the Morse complex of $(J, C_β)$ by unions of unstable manifolds of critical points (at infinity)which must include periodic orbits of $ξ$; ie unions of unstable manifolds of critical points at infinity alone cannot achieve these cycles. The topological argument of existence of a periodic orbit for $ξ$ turns out to be surprisingly close, in spirit, to the linking/equivariant argument of P.H. Rabinowitz in [12]. The objects and the frameworks are strikingly different, but the original proof of [12] can be recognized in our proof, which uses degree theory, the Fadell-Rabinowitz index [8] and the fact that $π_{n+1}(S^n)=\mathbb{Z}_2, n\geq 3$. The arguments hold under the basic assumption that no periodic orbit of index $1$ connects $L^+$ and $L^-$. To a certain extent, the present result runs, especially in the case of three-dimensional overtwisted [8] contact forms, against the existence of non-trivial algebraic invariants defined by the periodic orbits of $ξ$ and independent of what $ker α$ and/or $α$ are.