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Smoothness of the radial projection and the aaa-coordinate

Proved
FiniteEnergyPlane.contDiffOn_proj_aCoord

by Mazecto · Nov 4, 2026 · Mathlib 0df444a (Lean v4.33.1)

pseudoholomorphic-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: HHH is smooth, every ray from the origin meets SSS exactly once, and dHx(x)>0dH_x(x)>0dHx​(x)>0 for x∈Sx\in Sx∈S. For y≠0y\neq0y=0 let r(y)>0r(y)>0r(y)>0 be the unique scalar with H(r(y)y)=1H(r(y)y)=1H(r(y)y)=1, and put proj(y)=r(y) y∈S\mathrm{proj}(y)=r(y)\,y\in Sproj(y)=r(y)y∈S and a(y)=−12log⁡r(y)a(y)=-\tfrac12\log r(y)a(y)=−21​logr(y), so that y=e2a(y)proj(y)y=e^{2a(y)}\mathrm{proj}(y)y=e2a(y)proj(y). Then proj\mathrm{proj}proj and aaa are C∞C^\inftyC∞ on R2n+2∖{0}\mathbb{R}^{2n+2}\setminus\{0\}R2n+2∖{0}.

This is the smoothness of the identification R2n+2∖{0}≅R×S\mathbb{R}^{2n+2}\setminus\{0\}\cong\mathbb{R}\times SR2n+2∖{0}≅R×S of the symplectization.

Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- On a strictly star-shaped level `S = H⁻¹(1)`, the radial projection `proj H` and the
symplectization coordinate `aCoord H` are `C^∞` on `V n \ {0}`. -/
theorem contDiffOn_proj_aCoord {n : ℕ} (H : V n → ℝ) (hH : IsStrictlyStarShapedLevel H) :
    ContDiffOn ℝ ∞ (proj H) {0}ᶜ ∧ ContDiffOn ℝ ∞ (aCoord H) {0}ᶜ := by
  sorry

end FiniteEnergyPlane
Source
U. Hryniewicz, Fast finite-energy planes in symplectizations and applications, Trans. Amer. Math. Soc. 364 (2012), 1859–1931, arXiv:0812.4076, § 4 (supporting lemma for Lemma 4.16)

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