An end with nonvanishing dλ-density is not a reparametrized Reeb orbit
ProvedFiniteEnergyPlane.exists_endW_ne_proj_reeb_compasymptotic-analysispseudoholomorphic-curvesreeb-dynamicssymplectization
Let be a finite-energy -holomorphic curve on (strictly star-shaped level , compatible ), and suppose that the density , , does not vanish identically on any punctured disk . Let be a periodic Reeb orbit and of class on some . Then for every there are and with
So such a curve is not, on any end, a reparametrization of the trivial cylinder over .
Formalization Note The density is dlambdaDensity H u z; the end is endW H u cylEnd (s, t).
Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real
/-- A finite-energy curve on `D \ {0}` whose `dλ`-density `ω₀(∂ₛw, ∂ₜw)` (`w = proj H ∘ u`) does
not vanish identically on any punctured neighbourhood of `0` is not, on any end `s ≥ s₀`, of the
form `w(s, t) = proj H (x(τ(s, t)))` with `x` a Reeb orbit and `τ` of class `C¹`: for every `s₀`
there are `s ≥ s₀` and `t` with `endW(s, t) ≠ proj H (x(τ(s, t)))`. -/
theorem exists_endW_ne_proj_reeb_comp {n : ℕ} (H : V n → ℝ) (hH : IsStrictlyStarShapedLevel H)
(J : V n → V n →L[ℝ] V n) (hJ : IsCompatibleXiStructure H J) (u : ℂ → V n)
(hu : IsFiniteEnergyCurve H J (ball 0 1 \ {0}) u) (P : ReebOrbit H)
(hden : ∀ r > 0, ∃ z ∈ ball (0 : ℂ) r \ {0}, dlambdaDensity H u z ≠ 0)
(τ : ℝ × ℝ → ℝ) (sτ : ℝ) (hτ : ContDiffOn ℝ 1 τ (Set.Ioi sτ ×ˢ Set.univ)) :
∀ s₀ : ℝ, ∃ s ≥ s₀, ∃ t : ℝ, endW H u cylEnd (s, t) ≠ proj H (P.x (τ (s, t))) := by
sorry
end FiniteEnergyPlane
Source
Used for U. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014), arXiv:1105.2077, Theorem 2.11 and Lemma 2.12; H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations I: asymptotics, Ann. Inst. H. Poincaré Anal. Non Linéaire 13 (1996)