Shifted cylindrical coordinates of an end converge in to a trivial cylinder
ProvedFiniteEnergyPlane.exists_subseq_tendstoCInftyLocOn_cylEnd_shiftLet be a strictly star-shaped level with contact form , Reeb field and a -compatible complex structure on , and let be a finite-energy -holomorphic curve on the punctured unit disc. Let be a periodic Reeb orbit (degenerate orbits allowed) and . Write , for the components of in the cylindrical coordinates at the puncture.
Assume that for every there is such that for each some phase satisfies
Then for every sequence there are a subsequence (not relabelled) and a phase such that
in , i.e. with all derivatives, uniformly on compact subsets of .
This is the compactness statement behind the convergence, up to phase, of the end to the trivial cylinder over .
Formalization Note endA H u cylEnd and endW H u cylEnd are and in the coordinates cylEnd s t ; the shifted maps are p ↦ endA H u cylEnd (p + (s_j, 0)) - endA H u cylEnd (s_j, 0) and p ↦ endW H u cylEnd (p + (s_j, 0)) on ℝ × ℝ. convergence is JHolomorphic.TendstoCInftyLocOn on Set.univ; the subsequence is a strictly monotone φ. The loop hypothesis uses loopInS H u (cwLoop 0 r), eventually in 𝓝[>] 0.
import Definitions.Def_FiniteEnergyPlane_Asymptotics
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real
/-- Let `u` be a finite-energy `J̃`-holomorphic curve on `D \ {0}`, `P = (x, T)` a periodic Reeb
orbit and `σ = ±1`. Suppose that for every `ε > 0`, every clockwise loop
`t ↦ proj(u(r e^{-2π i t}))` of sufficiently small radius `r > 0` is uniformly `ε`-close to some
reparametrization `t ↦ x(σ T t + c')`. Then for every sequence `s_j → ∞` there are a subsequence
and a phase `c` such that, in the cylindrical coordinates `cylEnd` at `0`, the shifted maps
`(s, t) ↦ a(s + s_j, t) - a(s_j, 0)` converge in `C^∞_loc(ℝ²)` to `(s, t) ↦ σ T s`, and the shifted
maps `(s, t) ↦ w(s + s_j, t)` converge in `C^∞_loc(ℝ²)` to `(s, t) ↦ x(σ T t + c)`. -/
theorem exists_subseq_tendstoCInftyLocOn_cylEnd_shift {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) (σ : ℝ)
(hσ : σ = 1 ∨ σ = -1)
(hloop : ∀ ε : ℝ, 0 < ε → ∀ᶠ r in 𝓝[>] (0 : ℝ), ∃ c' : ℝ, ∀ t : ℝ,
‖loopInS H u (cwLoop 0 r) t - P.x (σ * P.T * t + c')‖ ≤ ε)
(s : ℕ → ℝ) (hs : Tendsto s atTop atTop) :
∃ φ : ℕ → ℕ, StrictMono φ ∧ ∃ c : ℝ,
JHolomorphic.TendstoCInftyLocOn
(fun j (p : ℝ × ℝ) => endA H u cylEnd (p + (s (φ j), 0)) - endA H u cylEnd (s (φ j), 0))
(fun p => σ * P.T * p.1) Set.univ ∧
JHolomorphic.TendstoCInftyLocOn
(fun j (p : ℝ × ℝ) => endW H u cylEnd (p + (s (φ j), 0)))
(fun p => P.x (σ * P.T * p.2 + c)) Set.univ := by
sorry
end FiniteEnergyPlane