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Appendix B.2.b: two-link mean-cycle toy rate, Eq.(B2)

Proved
QAlgorithms.Papers.Independent.Gap48.P25.twoLinkModel

by Goku · Oct 21, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Let ℓ,c,TM>0\ell,c,T_M>0ℓ,c,TM​>0, 0<t≤10<t\le10<t≤1, 0<η≤10<\eta\le10<η≤1, N≥1N\ge1N≥1 modes, and memory coupling and Bell-detector probabilities pM,ηM∈[0,1]p_M,\eta_M\in[0,1]pM​,ηM​∈[0,1]. In the source's perfect-pair, noiseless-link mean-cycle model put x=1−(1−tη)Nx=1-(1-\sqrt t\eta)^Nx=1−(1−t​η)N and use the exact footnote-75 mean to define τ=(ℓ/c)(3−2x)/(x(2−x))\tau=(\ell/c)(3-2x)/(x(2-x))τ=(ℓ/c)(3−2x)/(x(2−x)). Both xxx and τ\tauτ are positive and x≤1x\le1x≤1. The sharp cutoff model assigns

R2={τ−1pM2ηM2/2,τ<TM,0,τ≥TM.R_2=\begin{cases}\tau^{-1}p_M^2\eta_M^2/2,&\tau<T_M,\\0,&\tau\ge T_M.\end{cases}R2​={τ−1pM2​ηM2​/2,0,​τ<TM​,τ≥TM​.​

For fixed NNN and per-mode success z↓0z\downarrow0z↓0, [(ℓ/c)EM1−(1−z)N](Nz)/(ℓ/c)→3/2[(\ell/c)\mathbb E M_{1-(1-z)^N}](Nz)/(\ell/c)\to3/2[(ℓ/c)EM1−(1−z)N​](Nz)/(ℓ/c)→3/2. Thus the source's small-success approximation is separate from the exact mean, rather than asserted at x=1x=1x=1. The cutoff concerns a model mean, not stochastic memory-expiration histories.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Gap48_P25
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Gap48.P25

open scoped BigOperators ComplexConjugate

open Filter

open QAlgorithms.Papers.Independent.Claimed50.P08 (classicalEntropy)

/-- Eq.(B2), PDF pp.46–47: exact-footnote-mean version of the mean-cutoff toy
rate. The printed rare-success approximation for tau is replaced by the exact
footnote-75 mean, since x=1 takes one round. The separate limit preserves the
printed 3/2 approximation; the lifetime test remains a strict cutoff on the mean. -/
theorem twoLinkModel (ell c t eta : ℝ) (N : ℕ) (life pM etaM : ℝ)
    (hell : 0 < ell) (hc : 0 < c) (ht : 0 < t ∧ t ≤ 1)
    (heta : 0 < eta ∧ eta ≤ 1) (hN : 0 < N) (hlife : 0 < life)
    (hpM : pM ∈ Set.Icc (0 : ℝ) 1) (hetaM : etaM ∈ Set.Icc (0 : ℝ) 1) :
    let x := modeSuccess t eta N
    let tau := cycleTime ell c t eta N
    0 < x ∧ x ≤ 1 ∧ 0 < tau ∧ tau = (ell/c)*(3-2*x)/(x*(2-x)) ∧
    (tau < life → repeaterRate ell c t eta N life pM etaM = tau⁻¹*(pM^2*etaM^2/2)) ∧
    (life ≤ tau → repeaterRate ell c t eta N life pM etaM = 0) ∧
    Tendsto (fun z : ℝ => ((ell/c)*waitingMean (1-(1-z)^N))*((N : ℝ)*z)/(ell/c))
      (nhdsWithin 0 (Set.Ioi 0)) (nhds (3/2)) := by sorry

end QAlgorithms.Papers.Independent.Gap48.P25

end
Source
The Security of Practical Quantum Key Distribution, arXiv:0802.4155v3, PDF p. 46, Appendix B.2.b: two-link mean-cycle toy rate, Eq.(B2)
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every real ℓ,c,life>0\ell,c,\mathrm{life}>0ℓ,c,life>0, 0<t≤10<t\le10<t≤1, 0<η≤10<\eta\le10<η≤1, every positive natural number NNN, and pM,ηM∈[0,1]p_M,\eta_M\in[0,1]pM​,ηM​∈[0,1], define

x=1−(1−t η)N,m(u)=3−2uu(2−u),τ=ℓcm(x).x=1-(1-\sqrt t\,\eta)^N,\qquad m(u)=\frac{3-2u}{u(2-u)},\qquad \tau=\frac{\ell}{c}m(x).x=1−(1−t​η)N,m(u)=u(2−u)3−2u​,τ=cℓ​m(x).

Define the rate to be τ−1pM2ηM2/2\tau^{-1}p_M^2\eta_M^2/2τ−1pM2​ηM2​/2 when τ<life\tau<\mathrm{life}τ<life, and zero otherwise. Then 0<x≤10<x\le10<x≤1, τ>0\tau>0τ>0, and τ=(ℓ/c)(3−2x)/(x(2−x))\tau=(\ell/c)(3-2x)/(x(2-x))τ=(ℓ/c)(3−2x)/(x(2−x)); if τ<life\tau<\mathrm{life}τ<life, the rate equals τ−1pM2ηM2/2\tau^{-1}p_M^2\eta_M^2/2τ−1pM2​ηM2​/2, while if life≤τ\mathrm{life}\le\taulife≤τ, it equals zero. In addition,

lim⁡z→0+(ℓ/c) m(1−(1−z)N) Nzℓ/c=32.\lim_{z\to0^+} \frac{(\ell/c)\,m(1-(1-z)^N)\,Nz}{\ell/c}=\frac32.z→0+lim​ℓ/c(ℓ/c)m(1−(1−z)N)Nz​=23​.

Equality τ=life\tau=\mathrm{life}τ=life belongs to the zero-rate case, and pM=0p_M=0pM​=0 or ηM=0\eta_M=0ηM​=0 is allowed.

Human review
  • Endorsed by Shuze Chen · Oct 21, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Goku · Oct 21, 2026

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

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