Linear Cauchy–Riemann equation with exponentially convergent coefficients for the normal part of an end
ProvedFiniteEnergyPlane.exists_crEquation_tubeNormal_expDecayLet be a finite-energy -holomorphic curve on , a periodic Reeb orbit, a unitary frame of along in which the asymptotic operator is with a smooth symmetric loop, , and suppose the end of at is written for as , , , -periodic, with and in , and with
Then there are , , and maps (matrix valued) and , smooth on , such that decays like in , and for : , are -periodic in , , and .
This turns the normal part of an exponentially convergent end into a solution of a linear Cauchy–Riemann equation whose coefficients converge exponentially.
Formalization Note Exponential convergence is IsExpAsymptoticTo (entrywise ExpDecayCInfty); the operator is CauchyRiemannIndex.crOp; the hypothesis on , is the identity hZS for every smooth -periodic .
import Definitions.Def_FiniteEnergyPlane_Asymptotics
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real
/-- Linear Cauchy–Riemann equation for the normal component of an end in tube coordinates, with
exponentially convergent coefficients. Let `u` be a finite-energy curve on `D \ {0}`, `P` a Reeb
orbit, `Z` a unitary frame of `ξ` along `P` in which `A_P` is `-J₀ ∂ₜ - S∞`, and suppose the end
is written as `w = proj H (x(τ) + h)`, `h ∈ ξ_{x(τ)}`, with `τ - εTt - c → 0` and `h → 0` in `C^∞`
and with `|τ - εTt - c| + ‖h‖ ≤ C₀ e^{-bs}`, `b > 0`. Then for some `s₁` and `d > 0` there are
`S` and `ζ`, smooth and `1`-periodic on `s > s₁`, with `h = Z(τ/T) ζ`, `∂ₛζ + J₀ ∂ₜζ + S ζ = 0`,
`‖ζ(s, t)‖ ≤ C e^{-ds}` for all `s > s₁`, and `S(s, t) - ε S∞(εt + c/T)` decaying like `e^{-ds}`
in `C^∞`. -/
theorem exists_crEquation_tubeNormal_expDecay {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)
(Z : ℝ → CauchyRiemannIndex.Vec n →L[ℝ] V n) (hZ : IsUnitaryXiFrame J P Z)
(Sinf : ℝ → CauchyRiemannIndex.Mat n) (hSinf : CauchyRiemannIndex.IsSymLoop Sinf)
(hSinf' : ∀ i j, ContDiff ℝ ∞ (fun t => Sinf t i j))
(hZS : ∀ η : ℝ → CauchyRiemannIndex.Vec n, ContDiff ℝ ∞ η → Function.Periodic η 1 →
∀ t : ℝ, asympOp J P (fun t => Z t (η t)) t =
Z t (-(Matrix.toEuclideanLin (CauchyRiemannIndex.J₀ n) (deriv η t)) -
Matrix.toEuclideanLin (Sinf t) (η t)))
(ε : ℝ) (hε : ε = 1 ∨ ε = -1) (c : ℝ) (τ : ℝ × ℝ → ℝ) (h : ℝ × ℝ → V n) (s₀ : ℝ)
(hτ : TendstoZeroCInfty (fun p : ℝ × ℝ => τ p - ε * P.T * p.2 - c))
(hh : TendstoZeroCInfty h)
(hrep : ∀ s ≥ s₀, ∀ t : ℝ,
τ (s, t + 1) = τ (s, t) + ε * P.T ∧ h (s, t + 1) = h (s, t) ∧
IsInXi H (P.x (τ (s, t))) (h (s, t)) ∧
endW H u cylEnd (s, t) = proj H (P.x (τ (s, t)) + h (s, t)))
(b C₀ : ℝ) (hb : 0 < b)
(hdec : ∀ s ≥ s₀, ∀ t : ℝ,
|τ (s, t) - ε * P.T * t - c| + ‖h (s, t)‖ ≤ C₀ * Real.exp (-(b * s))) :
∃ (s₁ d C : ℝ) (S : ℝ × ℝ → CauchyRiemannIndex.Mat n) (ζ : ℝ × ℝ → CauchyRiemannIndex.Vec n),
0 < d ∧
(∀ i j, ContDiffOn ℝ ∞ (fun p : ℝ × ℝ => S p i j) (Set.Ioi s₁ ×ˢ Set.univ)) ∧
IsExpAsymptoticTo S (fun t => ε • Sinf (ε * t + c / P.T)) d ∧
ContDiffOn ℝ ∞ ζ (Set.Ioi s₁ ×ˢ Set.univ) ∧
∀ s > s₁, ∀ t : ℝ, S (s, t + 1) = S (s, t) ∧ ζ (s, t + 1) = ζ (s, t) ∧
CauchyRiemannIndex.crOp S ζ (s, t) = 0 ∧ h (s, t) = Z (τ (s, t) / P.T) (ζ (s, t)) ∧
‖ζ (s, t)‖ ≤ C * Real.exp (-(d * s)) := by
sorry
end FiniteEnergyPlane