Transversality of a J-holomorphic family at one point holds along a fast member
ProvedFiniteEnergyPlane.fderiv_family_add_smul_eq_zeroLet be a strictly star-shaped level with a compatible complex structure on the contact planes, and let be a periodic Reeb orbit. Let be such that every eigenvalue of the asymptotic operator below has winding number at most and every eigenvalue above has winding number at least , in the global frame of . Let be with every -holomorphic, and let be such that is a fast finite-energy plane asymptotic to at , is smooth, and for some and every some has .
If the identity forces , and , then for every the identity forces the same.
Role. The tangent plane of the member, the parameter direction and the -translation direction then span at every point of the member, not only at .
Formalization Note. The symplectization is , with , = aCoord H y and = proj H y. Winding numbers are HasEigenWind; is the cylindrical weight for . The bound measures the -derivative modulo the tangent plane of the member, relative to . The point is only a convenient base point.
import Definitions.Def_FiniteEnergyPlane_CylClose
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real
/-- Transversality of a family of `J̃`-holomorphic maps at one point of a fast member holds along the
whole member. Let `δ < 0` be such that every eigenvalue of `A_P` below `δ` has winding number at most
`1` and every eigenvalue above `δ` has winding number at least `2`. Let `g : ℂ × (-r, r) → V 1` be
`C²` with every `g(·, t')` `J̃`-holomorphic, and let `g(·, t)` be a fast finite-energy plane
asymptotic to `P` at `∞`, with `∂ₜg(·, t)` smooth and with `Δ` at each `z` such that
`‖Dg(z, t)(Δ, 1)‖ ≤ C (1 + ‖z‖)^{δ/2π} ‖g(z, t)‖`. If `Dg(0, t)(Δ, δt) + λ • g(0, t) = 0` forces
`Δ = 0`, `δt = 0`, `λ = 0`, then the same holds with `0` replaced by any `z`. -/
theorem fderiv_family_add_smul_eq_zero (H : V 1 → ℝ) (hH : IsStrictlyStarShapedLevel H)
(J : V 1 → V 1 →L[ℝ] V 1) (hJ : IsCompatibleXiStructure H J)
(P : ReebOrbit H) (δ : ℝ) (hδ : δ < 0)
(hwin : ∀ (μ : ℝ) (k : ℤ), HasEigenWind J P μ k → (μ < δ ∧ k ≤ 1) ∨ (δ < μ ∧ 2 ≤ k))
(r : ℝ) (g : ℂ × ℝ → V 1) (hg : ContDiffOn ℝ 2 g (Set.univ ×ˢ Set.Ioo (-r) r))
(hgJ : ∀ t' ∈ Set.Ioo (-r) r,
JHolomorphic.IsJHolomorphicOn (Jtilde H J) Set.univ (fun z => g (z, t')))
(t : ℝ) (ht : t ∈ Set.Ioo (-r) r)
(hfast : IsFastPlane H J (fun z => g (z, t)))
(hend : IsNondegenerateEnd H (fun z => g (z, t)) cylInf P 1)
(hX : ContDiff ℝ ∞ (fun z => fderiv ℝ g (z, t) (0, 1)))
(C : ℝ) (hrate : ∀ z, ∃ Δ : ℂ, ‖fderiv ℝ g (z, t) (Δ, 1)‖ ≤
C * (1 + ‖z‖) ^ (δ / (2 * π)) * ‖g (z, t)‖)
(htr : ∀ (Δ : ℂ) (δt lam : ℝ), fderiv ℝ g (0, t) (Δ, δt) + lam • g (0, t) = 0 →
Δ = 0 ∧ δt = 0 ∧ lam = 0) (z : ℂ) (Δ : ℂ) (δt lam : ℝ)
(h0 : fderiv ℝ g (z, t) (Δ, δt) + lam • g (z, t) = 0) :
Δ = 0 ∧ δt = 0 ∧ lam = 0 := by
sorry
end FiniteEnergyPlane