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Blow-up points with a doubling bound on shrinking discs

Proved
FiniteEnergyPlane.exists_blowup_points

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

analysisfinite-energypseudoholomorphic-curvesreal-analysis

For each k∈Nk\in\mathbb Nk∈N let Uk⊆CU_k\subseteq\mathbb CUk​⊆C and let gk:C→[0,∞)g_k:\mathbb C\to[0,\infty)gk​:C→[0,∞) be continuous on UkU_kUk​. Let ρ>0\rho>0ρ>0 and let zk∈Cz_k\in\mathbb Czk​∈C satisfy B‾(zk,ρ)⊆Uk\overline B(z_k,\rho)\subseteq U_kB(zk​,ρ)⊆Uk​, gk(zk)>0g_k(z_k)>0gk​(zk​)>0 and gk(zk)→∞g_k(z_k)\to\inftygk​(zk​)→∞. Then there are points ζk∈C\zeta_k\in\mathbb Cζk​∈C and radii εk>0\varepsilon_k>0εk​>0 such that

  • εk→0\varepsilon_k\to0εk​→0,  εk gk(ζk)→∞\ \varepsilon_k\,g_k(\zeta_k)\to\infty εk​gk​(ζk​)→∞ and ∣zk−ζk∣→0|z_k-\zeta_k|\to0∣zk​−ζk​∣→0;
  • gk(ζk)>0g_k(\zeta_k)>0gk​(ζk​)>0 and B‾(ζk,εk)⊆Uk\overline B(\zeta_k,\varepsilon_k)\subseteq U_kB(ζk​,εk​)⊆Uk​;
  • gk(y)≤2 gk(ζk)g_k(y)\le 2\,g_k(\zeta_k)gk​(y)≤2gk​(ζk​) for every y∈B‾(ζk,εk)y\in\overline B(\zeta_k,\varepsilon_k)y∈B(ζk​,εk​).

Near points where a sequence of functions blows up, there are nearby points where the function is controlled by twice its value on a disc whose radius, measured in units of 1/gk(ζk)1/g_k(\zeta_k)1/gk​(ζk​), tends to infinity.

Formalization Note The discs are closed balls closedBall. Continuity is ContinuousOn (g k) (U k); nonnegativity is required at every point of C\mathbb CC.

Preamble
import Definitions.Def_FiniteEnergyPlane_Setting
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology
open scoped ContDiff ENNReal Real

/-- Blow-up points with doubling control. Let `g_k ≥ 0` be continuous on `U_k ⊆ ℂ`, and let
`z_k` be points with `B̄(z_k, ρ) ⊆ U_k` for a fixed `ρ > 0`, `g_k(z_k) > 0` and
`g_k(z_k) → ∞`. Then there are points `ζ_k` and radii `ε_k > 0` with `ε_k → 0`,
`ε_k g_k(ζ_k) → ∞`, `|z_k - ζ_k| → 0`, `g_k(ζ_k) > 0`, `B̄(ζ_k, ε_k) ⊆ U_k`, and
`g_k ≤ 2 g_k(ζ_k)` on `B̄(ζ_k, ε_k)`. -/
theorem exists_blowup_points (g : ℕ → ℂ → ℝ) (U : ℕ → Set ℂ) (z : ℕ → ℂ) (ρ : ℝ) (hρ : 0 < ρ)
    (hball : ∀ k, closedBall (z k) ρ ⊆ U k) (hg : ∀ k, ContinuousOn (g k) (U k))
    (hg0 : ∀ k w, 0 ≤ g k w) (hpos : ∀ k, 0 < g k (z k))
    (hblow : Tendsto (fun k => g k (z k)) atTop atTop) :
    ∃ ζ : ℕ → ℂ, ∃ ε : ℕ → ℝ, (∀ k, 0 < ε k) ∧ Tendsto ε atTop (𝓝 0) ∧
      Tendsto (fun k => ε k * g k (ζ k)) atTop atTop ∧
      Tendsto (fun k => ‖z k - ζ k‖) atTop (𝓝 0) ∧ (∀ k, 0 < g k (ζ k)) ∧
      (∀ k, closedBall (ζ k) (ε k) ⊆ U k) ∧
      ∀ k, ∀ y ∈ closedBall (ζ k) (ε k), g k y ≤ 2 * g k (ζ k) := by
  sorry

end FiniteEnergyPlane
Source
U. Hryniewicz, Systems of global surfaces of section for dynamically convex Reeb flows on the 3-sphere, J. Symplectic Geom. 12 (2014), arXiv:1105.2077, proof of Lemma 2.20, p. 12; H. Hofer, Invent. Math. 114 (1993), Section 3

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