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Lemma 4.4, p. 21 — the second time scale exceeds the first

Proved
KangKurtz.SecondScale.lemma_4_4

by mikedeng1 · Oct 9, 2026 · Mathlib 0df444a (Lean v4.33.1)

multiscalep2o-batch-pfp2ap2o-gran-per-chapterp2o-plan-paperp2o-v1reaction-networkstime-scales

For a finite reaction network, let r1=min⁡iγir_1=\min_i\gamma_ir1​=mini​γi​ be the first natural time scale. Let K2\mathbb K_2K2​ consist of the nonnegative weighted combinations unchanged by the projected first-scale reactions, and set r2=inf⁡θ∈K2γθr_2=\inf_{\theta\in\mathbb K_2}\gamma_\thetar2​=infθ∈K2​​γθ​. If at least one reaction changes at least one species, then

r2>r1.r_2>r_1.r2​>r1​.

This separates the first and second natural time scales defined in Section 4.

Formalization Note The requirement that some ζik≠0\zeta_{ik}\ne0ζik​=0 makes r1r_1r1​ finite. It is a necessary explicit addition: if every reaction has zero net change, both time scales are +∞+\infty+∞ and the strict inequality is false. The infimum is over all of K2\mathbb K_2K2​, including combinations unchanged by every reaction.

Preamble
import Mathlib
import Definitions.Def_KangKurtz_SecondScale_Setting
Formal statement
namespace KangKurtz.SecondScale

theorem lemma_4_4 {s r : ℕ} (ν ν' : Fin r → Fin s → ℕ)
    (α : Fin s → ℝ) (hα : ∀ i, 0 ≤ α i) (β : Fin r → ℝ)
    (hζ : ∃ k i, ν' k i ≠ ν k i) :
    r1 ν ν' α β < r2 ν ν' α β := by sorry

end KangKurtz.SecondScale
Source
Kang and Kurtz, Separation of time-scales and model reduction for stochastic reaction networks, arXiv:1011.1672v1, p. 21, Lemma 4.4, second part
Human review
  • Endorsed by Shuze Chen · Oct 9, 2026

    Confirmed by the moderator at approval.

  • Endorsed by mikedeng1 · Oct 9, 2026

    Confirmed by the mission captain (proposal self-audit).

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