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Monotone energy ratio for maps ∂tu=A ∂su\partial_t u=A\,\partial_s u∂t​u=A∂s​u with AAA close to a complex structure

Proved
FiniteEnergyPlane.monotoneOn_energy_ratio

by Mazecto · Oct 23, 2026 · Mathlib 0df444a (Lean v4.33.1)

energymonotonicitypseudoholomorphic-curvessymplectic-geometry

Let FFF be a real inner product space and J0:F→FJ_0:F\to FJ0​:F→F a continuous linear map with J02=−1J_0^2=-1J02​=−1 and ∥J0∥≤b\|J_0\|\le b∥J0​∥≤b, where b≥1b\ge1b≥1. Put γ=1+b2\gamma=1+b^2γ=1+b2 and g(v,v′)=⟨v,v′⟩+⟨J0v,J0v′⟩g(v,v')=\langle v,v'\rangle+\langle J_0v,J_0v'\rangleg(v,v′)=⟨v,v′⟩+⟨J0​v,J0​v′⟩. Let Λ≥0\Lambda\ge0Λ≥0 and S>0S>0S>0 with ΛS≤1/(4γ2b)\Lambda S\le 1/(4\gamma^2b)ΛS≤1/(4γ2b), let q∈Fq\in Fq∈F, U⊆CU\subseteq\mathbb CU⊆C open and u:C→Fu:\mathbb C\to Fu:C→F of class C2C^2C2 on UUU. Assume that at every z∈Uz\in Uz∈U with ∥u(z)−q∥<S\|u(z)-q\|<S∥u(z)−q∥<S one has ∂tu(z)=A(z) ∂su(z)\partial_tu(z)=A(z)\,\partial_su(z)∂t​u(z)=A(z)∂s​u(z) and ∥A(z)−J0∥≤Λ∥u(z)−q∥\|A(z)-J_0\|\le\Lambda\|u(z)-q\|∥A(z)−J0​∥≤Λ∥u(z)−q∥, and that the sets {z∈U:∥u(z)−q∥≤ρ}\{z\in U:\|u(z)-q\|\le\rho\}{z∈U:∥u(z)−q∥≤ρ} are compact for every ρ<S\rho<Sρ<S.

Let φ:R→[0,1]\varphi:\mathbb R\to[0,1]φ:R→[0,1] be C1C^1C1, nonincreasing, with φ=0\varphi=0φ=0 on [3/4,∞)[3/4,\infty)[3/4,∞), φ′=0\varphi'=0φ′=0 on (3/4,∞)(3/4,\infty)(3/4,∞) and φ′\varphi'φ′ bounded. For 0<s<S0<s<S0<s<S set

Φs(z)=1U(z) φ ⁣(g(u(z)−q, u(z)−q)s2)g(J0∂su(z), ∂tu(z)).\Phi_s(z)=\mathbf 1_U(z)\,\varphi\!\left(\frac{g(u(z)-q,\,u(z)-q)}{s^2}\right) g\bigl(J_0\partial_su(z),\,\partial_tu(z)\bigr).Φs​(z)=1U​(z)φ(s2g(u(z)−q,u(z)−q)​)g(J0​∂s​u(z),∂t​u(z)).

Then each Φs\Phi_sΦs​ is integrable and nonnegative, and with C=(γb+2γ2b)ΛC=(\gamma b+2\gamma^2b)\LambdaC=(γb+2γ2b)Λ the function

s↦e2Css2∫CΦss\mapsto \frac{e^{2Cs}}{s^2}\int_{\mathbb C}\Phi_ss↦s2e2Cs​∫C​Φs​

is nondecreasing on (0,S)(0,S)(0,S).

Role. This is the monotone quantity behind the monotonicity lemma for pseudoholomorphic curves, stated for a model map into a vector space, where the almost complex structure along uuu is only close to the constant structure J0J_0J0​.

Formalization Note. ∂su=Du(z) 1\partial_s u=Du(z)\,1∂s​u=Du(z)1, ∂tu=Du(z) i\partial_t u=Du(z)\,i∂t​u=Du(z)i; the integrals are Bochner integrals over C\mathbb CC for Lebesgue measure; the function Φs\Phi_sΦs​ is written out with Set.indicator and the inner product.

Preamble
import Mathlib.Analysis.InnerProductSpace.LinearMap
import Mathlib.Analysis.Normed.Operator.Bilinear
import Mathlib.Analysis.Calculus.ParametricIntegral
import Mathlib.Analysis.SpecialFunctions.ExpDeriv
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory Metric Filter Topology Set
open scoped ContDiff ENNReal

/-- Monotone energy ratio near a complex structure. Let `J₀` be a complex structure on a real inner
product space with `‖J₀‖ ≤ b`, `1 ≤ b`, `γ = 1 + b²`, and `g(v, v') = ⟪v, v'⟫ + ⟪J₀ v, J₀ v'⟫`. Let
`Λ ≥ 0`, `S > 0` with `Λ S ≤ 1 / (4 γ² b)`, `U ⊆ ℂ` open, `u` a `C²` map on `U` with
`∂ₜu = A(z) ∂ₛu` and `‖A(z) - J₀‖ ≤ Λ ‖u z - q‖` wherever `‖u z - q‖ < S`, and with compact sets
`{z ∈ U | ‖u z - q‖ ≤ ρ}` for `ρ < S`. Let `φ` be a nonincreasing `C¹` cutoff in `[0, 1]`
vanishing on `[3/4, ∞)` with bounded derivative vanishing on `(3/4, ∞)`. Put
`Φ_s(z) = 1_U(z) φ(g(u z - q, u z - q) / s²) g(J₀ ∂ₛu, ∂ₜu)`. Then for `0 < s < S`, `Φ_s` is
integrable and nonnegative, and `s ↦ e^{2 C s} ∫ Φ_s / s²` is nondecreasing on `(0, S)`, where
`C = (γ b + 2 γ² b) Λ`. -/
theorem monotoneOn_energy_ratio {F : Type*} [NormedAddCommGroup F] [InnerProductSpace ℝ F]
    (J₀ : F →L[ℝ] F) (hJ : J₀.comp J₀ = -ContinuousLinearMap.id ℝ F) {b : ℝ} (hb1 : 1 ≤ b)
    (hJb : ‖J₀‖ ≤ b) {Λ S : ℝ} (hΛ : 0 ≤ Λ) (hS : 0 < S)
    (hΛS : Λ * S ≤ 1 / (4 * (1 + b ^ 2) ^ 2 * b)) (q : F) {U : Set ℂ} {u : ℂ → F}
    (A : ℂ → F →L[ℝ] F) (hU : IsOpen U) (hu : ContDiffOn ℝ 2 u U)
    (hhol : ∀ z ∈ U, ‖u z - q‖ < S → fderiv ℝ u z Complex.I = A z (fderiv ℝ u z 1) ∧
      ‖A z - J₀‖ ≤ Λ * ‖u z - q‖)
    (hprop : ∀ ρ, ρ < S → IsCompact {z | z ∈ U ∧ ‖u z - q‖ ≤ ρ})
    {φ : ℝ → ℝ} (hφc : ContDiff ℝ 1 φ) (hφ0 : ∀ t, 3 / 4 ≤ t → φ t = 0)
    (hφb : ∀ t, 0 ≤ φ t ∧ φ t ≤ 1) (hφd : ∀ t, deriv φ t ≤ 0)
    (hφd0 : ∀ t, 3 / 4 < t → deriv φ t = 0) {Mφ : ℝ} (hMφ : ∀ t, |deriv φ t| ≤ Mφ) :
    (∀ s ∈ Ioo 0 S, Integrable (fun z => U.indicator (fun z => φ ((s ^ 2)⁻¹ * (inner ℝ (u z - q) (u z - q) + inner ℝ (J₀ (u z - q)) (J₀ (u z - q))))) z *
          (inner ℝ (J₀ (fderiv ℝ u z 1)) (fderiv ℝ u z Complex.I) +
          inner ℝ (J₀ (J₀ (fderiv ℝ u z 1))) (J₀ (fderiv ℝ u z Complex.I)))) ∧ ∀ z, 0 ≤ U.indicator (fun z => φ ((s ^ 2)⁻¹ * (inner ℝ (u z - q) (u z - q) + inner ℝ (J₀ (u z - q)) (J₀ (u z - q))))) z *
          (inner ℝ (J₀ (fderiv ℝ u z 1)) (fderiv ℝ u z Complex.I) +
          inner ℝ (J₀ (J₀ (fderiv ℝ u z 1))) (J₀ (fderiv ℝ u z Complex.I)))) ∧
    MonotoneOn (fun s => Real.exp (2 * (((1 + b ^ 2) * b + 2 * (1 + b ^ 2) ^ 2 * b) * Λ) * s) *
      (∫ z, U.indicator (fun z => φ ((s ^ 2)⁻¹ * (inner ℝ (u z - q) (u z - q) + inner ℝ (J₀ (u z - q)) (J₀ (u z - q))))) z *
          (inner ℝ (J₀ (fderiv ℝ u z 1)) (fderiv ℝ u z Complex.I) +
          inner ℝ (J₀ (J₀ (fderiv ℝ u z 1))) (J₀ (fderiv ℝ u z Complex.I)))) / s ^ 2) (Ioo 0 S) := by
  sorry

end FiniteEnergyPlane
Source
A. Zinger, Notes on J-holomorphic maps, arXiv:1706.00331, Proposition 3.12; C. Wendl, Lectures on Symplectic Field Theory, arXiv:1612.01009, p. 152

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