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Poincaré inequality on an interval for a curve vanishing at the left endpoint, with a skew-twisted derivative

Proved
FiniteEnergyPlane.integral_norm_sq_le_of_skew

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

inequalitiesinner-product-spacesreal-analysis

Let EEE be a real inner product space and T:E→ET:E\to ET:E→E a bounded linear operator that is skew in the sense ⟨v,Tv⟩=0\langle v,Tv\rangle=0⟨v,Tv⟩=0 for all v∈Ev\in Ev∈E. Let w:R→Ew:\mathbb{R}\to Ew:R→E be differentiable with continuous derivative w′w'w′, and suppose w(x0)=0w(x_0)=0w(x0​)=0. Then for every L>0L>0L>0,

∫x0x0+L∥w(t)∥2 dt ≤ 4L2∫x0x0+L∥w′(t)−T w(t)∥2 dt.\int_{x_0}^{x_0+L}\|w(t)\|^2\,dt\ \le\ 4L^2\int_{x_0}^{x_0+L}\big\|w'(t)-T\,w(t)\big\|^2\,dt .∫x0​x0​+L​∥w(t)∥2dt ≤ 4L2∫x0​x0​+L​​w′(t)−Tw(t)​2dt.

For T=0T=0T=0 this is a one-dimensional Poincaré inequality for functions vanishing at an endpoint. The twisted form allows w′w'w′ to be replaced by w′−Tww'-Tww′−Tw for any skew TTT, for instance T=aJ0T=aJ_0T=aJ0​ with the standard complex structure J0J_0J0​ on R2n\mathbb{R}^{2n}R2n. It is a reusable estimate for loops with controlled twisted derivative, as in the spectral theory of asymptotic operators (C. Wendl, Lectures on Symplectic Field Theory, 2026 notes, Section 3.5).

Formalization Note TTT is a continuous linear map E →L[ℝ] E with ∀ v, ⟪v, T v⟫ = 0. The derivative is supplied as a continuous w' with HasDerivAt w (w' t) t for all t. The integrals are interval integrals over x₀..x₀ + L.

Preamble
import Mathlib
Formal statement
namespace FiniteEnergyPlane

open MeasureTheory
open scoped RealInnerProductSpace

/-- Let `T` be a skew operator (`⟪v, T v⟫ = 0`) on a real inner product space and let `w` be a
`C¹` curve with `w(x₀) = 0`. Then on `[x₀, x₀ + L]`,
`∫ ‖w‖² ≤ 4 L² ∫ ‖w' - T w‖²`. -/
theorem integral_norm_sq_le_of_skew {E : Type*} [NormedAddCommGroup E] [InnerProductSpace ℝ E]
    (T : E →L[ℝ] E) (hT : ∀ v, ⟪v, T v⟫ = 0) (w w' : ℝ → E)
    (hw : ∀ t, HasDerivAt w (w' t) t) (hw' : Continuous w') (x₀ L : ℝ) (hL : 0 < L)
    (h0 : w x₀ = 0) :
    ∫ t in x₀..x₀ + L, ‖w t‖ ^ 2 ≤ 4 * L ^ 2 * ∫ t in x₀..x₀ + L, ‖w' t - T (w t)‖ ^ 2 := by
  sorry

end FiniteEnergyPlane
Source
Elementary; used for the uniform spectral gaps of asymptotic operators in C. Wendl, Lectures on Symplectic Field Theory (2026 notes), Section 3.5

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