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Shifts that nearly fix a periodic map are close to exact periods

Proved
FiniteEnergyPlane.exists_period_near_of_forall_shift_close

by Mazecto · Oct 30, 2026 · Mathlib 0df444a (Lean v4.33.1)

real-analysistopology

Let EEE be a normed group, T>0T>0T>0, and x:R→Ex:\mathbb{R}\to Ex:R→E continuous and TTT-periodic. Then for every δ>0\delta>0δ>0 there is η>0\eta>0η>0 with the following property: if a∈Ra\in\mathbb{R}a∈R satisfies ∥x(y+a)−x(y)∥≤η\|x(y+a)-x(y)\|\le\eta∥x(y+a)−x(y)∥≤η for all y∈Ry\in\mathbb{R}y∈R, then there is an exact period ppp of xxx (that is, x(y+p)=x(y)x(y+p)=x(y)x(y+p)=x(y) for all yyy) with ∣a−p∣<δ|a-p|<\delta∣a−p∣<δ.

So a shift that moves xxx uniformly very little is close to a symmetry of xxx. Here TTT need not be the minimal period, and xxx may be constant. The statement is used to compare phases c,c′c,c'c,c′ for which x(⋅+c)x(\cdot+c)x(⋅+c) and x(⋅+c′)x(\cdot+c')x(⋅+c′) are uniformly close, for instance phases of a periodic orbit that may be a multiple cover.

Formalization Note Exact periods are the reals ppp with ∀ y, x (y + p) = x y; the conclusion gives one such ppp with |a - p| < δ.

Preamble
import Mathlib
Formal statement
namespace FiniteEnergyPlane

open Filter Topology

/-- Let `x : ℝ → E` be continuous and `T`-periodic. For every `δ > 0` there is `η > 0` such that
whenever the shift `x(· + a)` is uniformly `η`-close to `x`, the number `a` lies within `δ` of an
exact period `p` of `x` (`x(y + p) = x(y)` for all `y`). -/
theorem exists_period_near_of_forall_shift_close {E : Type*} [NormedAddCommGroup E]
    {x : ℝ → E} {T : ℝ} (hT : 0 < T) (hx : Continuous x) (hxT : Function.Periodic x T)
    (δ : ℝ) (hδ : 0 < δ) :
    ∃ η > 0, ∀ a : ℝ, (∀ y : ℝ, ‖x (y + a) - x y‖ ≤ η) →
      ∃ p : ℝ, (∀ y : ℝ, x (y + p) = x y) ∧ |a - p| < δ := by
  sorry

end FiniteEnergyPlane
Source
Used for H. Hofer, K. Wysocki, E. Zehnder, Properties of pseudoholomorphic curves in symplectisations I: asymptotics (1996), Theorem 1.3

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