Curves of zeros of the weighted operator give families of -holomorphic planes
OpenFiniteEnergyPlane.exists_jbar_family_of_qMap_curveelliptic-pdepseudoholomorphic-curvessymplectic-geometry
Let , let be a standard tube structure (IsStdTubeStructure ρ b Jbar Jinf Sinf), let and , let satisfy IsSlopeWeight χT π (2π + δT), IsSlopeWeight χN π δ and IsLeftCutoff β, and let . Then there is with the following property.
Let and let be on , with , , and, for every , and qMap Jbar χT χN β (γ t) = 0. Then there are and , on , such that
- for all , and , the -component of ;
- for each the map is , takes values in , is -holomorphic on , and satisfies, for some and , , , and for every there is with and ;
- for every there is such that for and all : , , and .
The hypothesis that every member is a zero is essential.
Role. Weak solutions of the -Cauchy–Riemann equation in weighted Sobolev coordinates are turned into an honest family of smooth -holomorphic planes, jointly regular in the parameter, with pointwise weighted bounds.
Preamble
import Definitions.Def_FiniteEnergyPlane_TubeFamily
Formal statement
namespace FiniteEnergyPlane
open MeasureTheory Metric Filter Topology CauchyRiemannIndex
open scoped ContDiff ENNReal Real
/-- For a standard tube structure there is `ε₀ > 0` such that every `C^∞` curve `γ` of zeros of
`qMap` in `ball 0 ε₀` (every member a zero) with `γ 0 = 0` and velocity `k` at `0` defines a jointly
`C^l` family `G(·, t)` of `Jbar`-holomorphic planes through `G(·, 0) = (z, 0)`, with normal
velocity `k.2.1` at `z = 0`, the weighted bounds on each member, and weighted `C¹` convergence to
`(z, 0)` as `t → 0`. -/
theorem exists_jbar_family_of_qMap_curve (ρ b : ℝ) (hρ : 0 < ρ) (hb : 0 < b)
(Jbar : ℂ × ℂ → ℂ × ℂ →L[ℝ] ℂ × ℂ) (Jinf : ℝ × ℂ → ℂ × ℂ →L[ℝ] ℂ × ℂ)
(Sinf : ℝ → Mat 1) (hstd : IsStdTubeStructure ρ b Jbar Jinf Sinf)
(δ δT : ℝ) (hδ : δ < 0) (hδT : δT ∈ Set.Ioo (max δ (-(2 * π))) 0)
(χT χN β : ℝ → ℝ) (hχT : IsSlopeWeight χT π (2 * π + δT)) (hχN : IsSlopeWeight χN π δ)
(hβ : IsLeftCutoff β) (l : ℕ) :
∃ ε₀ > 0, ∀ r > 0, ∀ (γ : ℝ → QDom) (k : QDom), ContDiffOn ℝ ∞ γ (Set.Ioo (-r) r) →
γ 0 = 0 → HasDerivAt γ k 0 →
(∀ t ∈ Set.Ioo (-r) r, γ t ∈ ball 0 ε₀ ∧ qMap Jbar χT χN β (γ t) = 0) →
∃ r > 0, ∃ G : ℂ × ℝ → ℂ × ℂ, ContDiffOn ℝ l G (Set.univ ×ˢ Set.Ioo (-r) r) ∧
(∀ z, G (z, 0) = (z, 0)) ∧ (fderiv ℝ G (0, 0) (0, 1)).2 = k.2.1 ∧
(∀ t ∈ Set.Ioo (-r) r,
ContDiff ℝ ∞ (fun z => G (z, t)) ∧ (∀ z, (G (z, t)).2 ∈ ball (0 : ℂ) ρ) ∧
JHolomorphic.IsJHolomorphicOn Jbar Set.univ (fun z => G (z, t)) ∧
(∃ C β : ℝ, 0 < β ∧ ∀ z, ‖(G (z, t)).1 - z‖ ≤ C * (1 + ‖z‖) ^ (1 - β)) ∧
(∃ C : ℝ, ∀ z, ‖(G (z, t)).2‖ ≤ C * (1 + ‖z‖) ^ (δ / (2 * π))) ∧
∃ C : ℝ, ∀ z, ∃ Δ : ℂ, (fderiv ℝ G (z, t) (Δ, 1)).1 = 0 ∧
‖(fderiv ℝ G (z, t) (Δ, 1)).2‖ ≤ C * (1 + ‖z‖) ^ (δ / (2 * π))) ∧
∀ ε > 0, ∃ r' ∈ Set.Ioc 0 r, ∀ t ∈ Set.Ioo (-r') r', ∀ z,
‖(G (z, t)).1 - z‖ ≤ ε * (1 + ‖z‖) ∧ ‖(G (z, t)).2‖ ≤ ε ∧
‖fderiv ℝ (fun z => (G (z, t)).1) z - ContinuousLinearMap.id ℝ ℂ‖ ≤ ε ∧
(1 + ‖z‖) * ‖fderiv ℝ (fun z => (G (z, t)).2) z‖ ≤ ε := by
sorry
end FiniteEnergyPlane
Source
Toward U. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. AMS 364 (2012), arXiv:0812.4076, Lemmas 6.10 and 6.20 (families of fast planes); operators in the setting of C. Wendl, Lectures on Holomorphic Curves in Symplectic and Contact Geometry, arXiv:1011.1690, Ch. 4