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Pointwise exponential bound for a Lipschitz function dominated by the derivative of an exponentially small function

Proved
FiniteEnergyPlane.le_exp_of_deriv_ge_of_lipschitz

by Mazecto · Oct 29, 2026 · Mathlib 0df444a (Lean v4.33.1)

inequalitiesreal-analysis

Let a,E:R→Ra,E:\mathbb{R}\to\mathbb{R}a,E:R→R, let aaa be differentiable on (s0,∞)(s_0,\infty)(s0​,∞) with derivative a′a'a′, and let A,M,K∈RA,M,K\in\mathbb{R}A,M,K∈R, κ,β>0\kappa,\beta>0κ,β>0. Assume, for all s,x,y>s0s,x,y>s_0s,x,y>s0​,

∣a(s)∣≤Ae−κs,∣E(x)−E(y)∣≤M∣x−y∣,E(s)−Ke−βs≤a′(s).|a(s)|\le Ae^{-\kappa s},\qquad |E(x)-E(y)|\le M|x-y|,\qquad E(s)-Ke^{-\beta s}\le a'(s).∣a(s)∣≤Ae−κs,∣E(x)−E(y)∣≤M∣x−y∣,E(s)−Ke−βs≤a′(s).

Then there are κ′>0\kappa'>0κ′>0, CCC and s1s_1s1​ with E(s)≤Ce−κ′sE(s)\le Ce^{-\kappa' s}E(s)≤Ce−κ′s for all s≥s1s\ge s_1s≥s1​.

It upgrades exponential decay of a quantity aaa to a pointwise exponential bound on a regular quantity EEE that a′a'a′ controls from below, for instance an energy density along a half-cylinder.

Formalization Note No sign condition on EEE is assumed; the conclusion is an upper bound only.

Preamble
import Mathlib
Formal statement
namespace FiniteEnergyPlane

open Set Filter Topology

/-- If `|a| ≤ A e^{-κs}`, `E` is `M`-Lipschitz and `a' ≥ E - K e^{-βs}` on `(s₀, ∞)` with
`κ, β > 0`, then `E` is bounded above by a decaying exponential for large `s`. -/
theorem le_exp_of_deriv_ge_of_lipschitz (a a' E : ℝ → ℝ) (s₀ A κ M K β : ℝ) (hκ : 0 < κ)
    (hβ : 0 < β) (hd : ∀ s > s₀, HasDerivAt a (a' s) s)
    (ha : ∀ s > s₀, |a s| ≤ A * Real.exp (-(κ * s)))
    (hE : ∀ x > s₀, ∀ y > s₀, |E x - E y| ≤ M * |x - y|)
    (hineq : ∀ s > s₀, E s - K * Real.exp (-(β * s)) ≤ a' s) :
    ∃ κ' > 0, ∃ C s₁ : ℝ, ∀ s ≥ s₁, E s ≤ C * Real.exp (-(κ' * s)) := by
  sorry

end FiniteEnergyPlane
Source
Elementary real analysis; used for U. Hryniewicz, J. Symplectic Geom. 12 (2014), Theorem 2.10

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