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Euclidean derivative bounded by the R\mathbb{R}R-invariant gradient norm on a slab

Proved
FiniteEnergyPlane.norm_fderiv_le_mul_gradNorm

by Mazecto · Oct 25, 2026 · Mathlib 0df444a (Lean v4.33.1)

finite-energypseudoholomorphic-curvessymplectic-geometrysymplectization

Let S=H−1(1)⊂R2n+2S=H^{-1}(1)\subset\mathbb R^{2n+2}S=H−1(1)⊂R2n+2 be a strictly star-shaped level and JJJ a smooth dλ0d\lambda_0dλ0​-compatible complex structure on ξ\xiξ. Write y=e2axy=e^{2a}xy=e2ax with x=proj(y)∈Sx=\mathrm{proj}(y)\in Sx=proj(y)∈S for y≠0y\ne0y=0. Then for every A∈RA\in\mathbb RA∈R there is a constant MMM such that for every map u:C→R2n+2u:\mathbb C\to\mathbb R^{2n+2}u:C→R2n+2 and every z∈Cz\in\mathbb Cz∈C with uuu differentiable at zzz, u(z)≠0u(z)\ne0u(z)=0 and ∣a(u(z))∣≤A|a(u(z))|\le A∣a(u(z))∣≤A,

∥Du(z)∥ ≤ M (∥D(a∘u)(z)∥+∥D(proj∘u)(z)∥).\|Du(z)\|\ \le\ M\,\big(\|D(a\circ u)(z)\|+\|D(\mathrm{proj}\circ u)(z)\|\big).∥Du(z)∥ ≤ M(∥D(a∘u)(z)∥+∥D(proj∘u)(z)∥).

So on a slab ∣a∣≤A|a|\le A∣a∣≤A the Euclidean derivative is controlled by the R\mathbb RR-invariant gradient norm.

Formalization Note The right-hand side is M * gradNorm H u z. The compatible structure JJJ does not enter the conclusion.

Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- On a slab of the symplectization the Euclidean size of the derivative is controlled by the
`ℝ`-invariant one. For a strictly star-shaped level and `A ∈ ℝ` there is `M` such that for every
map `u : ℂ → ℝ^{2n+2}` differentiable at `z` with `u(z) ≠ 0` and `|a(u(z))| ≤ A`,
`‖Du(z)‖ ≤ M |∇u(z)|`, where `|∇u| = ‖D(a ∘ u)‖ + ‖D(proj ∘ u)‖` is `gradNorm`. -/
theorem norm_fderiv_le_mul_gradNorm {n : ℕ} (H : V n → ℝ) (hH : IsStrictlyStarShapedLevel H)
    (J : V n → V n →L[ℝ] V n) (hJ : IsCompatibleXiStructure H J) (A : ℝ) :
    ∃ M : ℝ, ∀ (u : ℂ → V n) (z : ℂ), DifferentiableAt ℝ u z → u z ≠ 0 →
      |aCoord H (u z)| ≤ A → ‖fderiv ℝ u z‖ ≤ M * gradNorm H u z := by
  sorry

end FiniteEnergyPlane
Source
H. Hofer, Invent. Math. 114 (1993), Section 3, (42)-(43); U. Hryniewicz, J. Symplectic Geom. 12 (2014), arXiv:1105.2077, Section 2

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