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Normal form: after a signed coordinate bijection every coordinate moves inward

Proved
Plasticity.CUB37.normal_form

by scanstone · Oct 14, 2026 · Mathlib 0df444a (Lean v4.33.1)

Let XXX be a space between c00(Γ)c_{00}(\Gamma)c00​(Γ) and c0(Γ)c_0(\Gamma)c0​(Γ), YYY one between c00(Δ)c_{00}(\Delta)c00​(Δ) and c0(Δ)c_0(\Delta)c0​(Δ), and F ⁣:BX→BYF\colon B_X\to B_YF:BX​→BY​ a nonexpansive bijection of their closed unit balls (supremum norm). No assumption is made on F−1F^{-1}F−1. Then there are a bijection σ ⁣:Γ→Δ\sigma\colon\Gamma\to\Deltaσ:Γ→Δ and signs αn∈{1,−1}\alpha_n\in\{1,-1\}αn​∈{1,−1} such that, for every x∈BXx\in B_Xx∈BX​ and every n∈Γn\in\Gamman∈Γ, the number

H(x)n=αn F(x)σ(n)H(x)_n=\alpha_n\,F(x)_{\sigma(n)}H(x)n​=αn​F(x)σ(n)​

lies between 000 and xnx_nxn​: 0≤H(x)n≤xn0\le H(x)_n\le x_n0≤H(x)n​≤xn​ if xn≥0x_n\ge0xn​≥0, and xn≤H(x)n≤0x_n\le H(x)_n\le0xn​≤H(x)n​≤0 if xn≤0x_n\le0xn​≤0.

In words, FFF is a signed coordinate bijection followed by a map that moves every coordinate weakly towards zero without changing its sign. This is the first step of the proof that such bijections are signed bijections.

Formalization Note Spaces are submodules of ℓ∞\ell_\inftyℓ∞​ as in the definitions Plasticity_SeqSpace; balls are ballIn. Index sets may be empty.

Preamble
import Definitions.Def_Plasticity_SeqSpace
import Mathlib.Topology.EMetricSpace.Lipschitz
Formal statement
namespace Plasticity.CUB37
theorem normal_form {Γ Δ : Type*} (X : Submodule ℝ (Linf Γ)) (Y : Submodule ℝ (Linf Δ))
    (hX0 : c00 Γ ≤ X) (hX1 : X ≤ c0 Γ) (hY0 : c00 Δ ≤ Y) (hY1 : Y ≤ c0 Δ)
    (F : Linf Γ → Linf Δ)
    (hbij : Set.BijOn F (ballIn X) (ballIn Y))
    (hlip : LipschitzOnWith 1 F (ballIn X)) :
    ∃ σ : Γ ≃ Δ, ∃ α : Γ → ℝ, (∀ n, α n = 1 ∨ α n = -1) ∧
      ∀ x ∈ ballIn X, ∀ n, (0 ≤ x n → 0 ≤ α n * F x (σ n) ∧ α n * F x (σ n) ≤ x n) ∧
        (x n ≤ 0 → x n ≤ α n * F x (σ n) ∧ α n * F x (σ n) ≤ 0) := by sorry
end Plasticity.CUB37
Source
This repository: expositions/c0_between_spaces.md §2, Proposition 1 (N1); after Leo's Lemmas 3.1–3.4 (R. Leo, Plasticity of the unit ball of c and c₀, J. Math. Anal. Appl. 2022)

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