Slice derivative bound for linear Cauchy–Riemann solutions with bounded growth rate
ProvedFiniteEnergyPlane.halfCyl_slice_deriv_sq_le_of_logDeriv_boundasymptotic-operatorpseudoholomorphic-curvessymplectic-geometry
Let be smooth and -periodic in , and let solve on the half-cylinder . Let , and be such that for all and all , the entries of , and are bounded in absolute value by , and
Then there are and such that for all ,
The hypothesis says that the logarithmic derivative of the slice energy is bounded. The conclusion bounds the -derivative of each slice by the slice itself, uniformly for large . It is used for FiniteEnergyPlane.halfCyl_slice_deriv_sq_le (Wendl, Lemma 4.8.8).
Formalization Note The solution is IsHalfCylSolution S ζ. The -derivatives of and are fderiv … (s, t) (1, 0), and the -derivative of the slice is deriv (fun x => ζ (s, x)) t.
Preamble
import Definitions.Def_FiniteEnergyPlane_Asymptotics
Formal statement
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real RealInnerProductSpace
/-- Let `ζ` solve `∂ₛζ + J₀ ∂ₜζ + S ζ = 0` on a half-cylinder, with smooth `1`-periodic `S` whose
entries and their first two `s`-derivatives are bounded for `s ≥ s₀`. If
`|⟨ζ, ∂ₛζ⟩_{L²}| ≤ Λ ‖ζ‖²_{L²}` on every slice `s ≥ s₀`, then for large `s` the `L²` norm of the
`t`-derivative of the slice `ζ(s, ·)` is bounded by a fixed multiple of the `L²` norm of the slice. -/
theorem halfCyl_slice_deriv_sq_le_of_logDeriv_bound {n : ℕ}
(S : ℝ × ℝ → CauchyRiemannIndex.Mat n)
(hS : ∀ i j, ContDiff ℝ ∞ (fun p : ℝ × ℝ => S p i j))
(hSper : ∀ s t : ℝ, S (s, t + 1) = S (s, t))
(ζ : ℝ × ℝ → CauchyRiemannIndex.Vec n) (hζ : IsHalfCylSolution S ζ)
(s₀ c Λ : ℝ) (hs₀ : 0 < s₀)
(hSb : ∀ s ≥ s₀, ∀ t : ℝ, ∀ i j, |S (s, t) i j| ≤ c ∧
|fderiv ℝ (fun p : ℝ × ℝ => S p i j) (s, t) (1, 0)| ≤ c ∧
|fderiv ℝ (fun p : ℝ × ℝ => fderiv ℝ (fun q : ℝ × ℝ => S q i j) p (1, 0)) (s, t) (1, 0)| ≤ c)
(hα : ∀ s ≥ s₀, |∫ t in (0:ℝ)..1, ⟪ζ (s, t), fderiv ℝ ζ (s, t) (1, 0)⟫| ≤
Λ * ∫ t in (0:ℝ)..1, ‖ζ (s, t)‖ ^ 2) :
∃ M s₁ : ℝ, ∀ s ≥ s₁,
∫ t in (0:ℝ)..1, ‖deriv (fun x => ζ (s, x)) t‖ ^ 2 ≤
M * ∫ t in (0:ℝ)..1, ‖ζ (s, t)‖ ^ 2 := by
sorry
end FiniteEnergyPlane
Source
C. Wendl, Lectures on Symplectic Field Theory (2026 notes), Lemma 4.8.8 (version with a bounded growth rate)