Exponential decay on an end for Cauchy–Riemann equations asymptotic to a loop along a drifting phase
ProvedFiniteEnergyPlane.halfCyl_exp_decay_of_driftLet be the standard complex structure on and a smooth -periodic loop of symmetric matrices whose asymptotic operator is nondegenerate. Let and let be smooth on with there. Let be a phase such that is smooth for large and every derivative of order of tends to as , uniformly in (no limit of is assumed). Suppose that each entry of
tends to in as . If is smooth on , -periodic in , solves there, and uniformly in , then there are , and with for .
This is the form needed for the normal component of a pseudoholomorphic end in tube coordinates around a nondegenerate periodic Reeb orbit, before the convergence of the asymptotic phase is known. With a constant phase it reduces to halfCyl_exp_decay_eventually (8ec20b66).
Formalization Note "Tends to in " is TendstoZeroCInfty; derivatives of are iteratedFDeriv ℝ m (fun p => φ p - p.2). The equation is CauchyRiemannIndex.crOp S ζ (s, t) = 0.
import Definitions.Def_FiniteEnergyPlane_Asymptotics
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real
/-- Exponential decay for linear Cauchy–Riemann equations on an end `(s₁, ∞) × ℝ/ℤ` whose
coefficient is asymptotic to a nondegenerate loop along a drifting phase: if `S` is smooth and
`1`-periodic in `t` for `s > s₁`, `φ(s, t) - t` is smooth for large `s` with every derivative of
order `≥ 1` tending to `0` uniformly, `S(s, t) - S∞(φ(s, t)) → 0` in `C^∞`, the asymptotic operator
`-J₀ ∂ₜ - S∞` is nondegenerate, and the `1`-periodic smooth solution `ζ` of
`∂ₛζ + J₀ ∂ₜζ + S ζ = 0` on `s > s₁` tends to `0` uniformly, then `ζ` decays exponentially. -/
theorem halfCyl_exp_decay_of_drift {n : ℕ} (s₁ : ℝ) (S : ℝ × ℝ → CauchyRiemannIndex.Mat n)
(hS : ∀ i j, ContDiffOn ℝ ∞ (fun p : ℝ × ℝ => S p i j) (Set.Ioi s₁ ×ˢ Set.univ))
(Sinf : ℝ → CauchyRiemannIndex.Mat n) (hSinf : CauchyRiemannIndex.IsSymLoop Sinf)
(hSinf' : ∀ i j, ContDiff ℝ ∞ (fun t => Sinf t i j))
(hnd : CauchyRiemannIndex.IsNondegenerate Sinf) (φ : ℝ × ℝ → ℝ)
(hφs : ∃ s₂ : ℝ, ContDiffOn ℝ ∞ (fun p : ℝ × ℝ => φ p - p.2) (Set.Ioi s₂ ×ˢ Set.univ))
(hφ : ∀ m : ℕ, 1 ≤ m → ∀ η > 0, ∃ s₂ : ℝ, ∀ s ≥ s₂, ∀ t : ℝ,
‖iteratedFDeriv ℝ m (fun p : ℝ × ℝ => φ p - p.2) (s, t)‖ ≤ η)
(hSas : ∀ i j, TendstoZeroCInfty (fun p : ℝ × ℝ => S p i j - Sinf (φ p) i j))
(ζ : ℝ × ℝ → CauchyRiemannIndex.Vec n) (hζ : ContDiffOn ℝ ∞ ζ (Set.Ioi s₁ ×ˢ Set.univ))
(hper : ∀ s > s₁, ∀ t : ℝ, S (s, t + 1) = S (s, t) ∧ ζ (s, t + 1) = ζ (s, t))
(heq : ∀ s > s₁, ∀ t : ℝ, CauchyRiemannIndex.crOp S ζ (s, t) = 0)
(hζ0 : TendstoZeroUnif ζ) :
∃ δ > 0, ∃ C s₂ : ℝ, ∀ s ≥ s₂, ∀ t : ℝ, ‖ζ (s, t)‖ ≤ C * Real.exp (-(δ * s)) := by
sorry
end FiniteEnergyPlane