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Theorem 2 (17): contractivity of Sb under global wirings

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QAlgorithms.Papers.Independent.Intakethird100.P29.global_contractivity

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

All Bell scenarios have independent finite, nonempty Alice and Bob input and output alphabets. A behavior is a nonnegative conditional output law normalized at every input pair; NS\mathrm{NS}NS imposes both no-signaling marginal identities. Processing uses one initial box with rules and randomness fixed independently of the supplied behavior. Write D(P∥Q)D(P\Vert Q)D(P∥Q) for classical Kullback–Leibler divergence with natural logarithms, zero numerator contributing zero and positive numerator over zero contributing +∞+\infty+∞. Define Sb(P∥Q)=max⁡x,yD(P(⋅,⋅∣x,y)∥Q(⋅,⋅∣x,y))S_b(P\Vert Q)=\max_{x,y}D(P(\cdot,\cdot\mid x,y)\Vert Q(\cdot,\cdot\mid x,y))Sb​(P∥Q)=maxx,y​D(P(⋅,⋅∣x,y)∥Q(⋅,⋅∣x,y)). For every pair P,Q∈NSP,Q\in\mathrm{NS}P,Q∈NS with the same alphabets and every global wiring GGG between arbitrary scenarios,

Sb(G(P)∥G(Q))≤Sb(P∥Q).S_b(G(P)\Vert G(Q))\le S_b(P\Vert Q).Sb​(G(P)∥G(Q))≤Sb​(P∥Q).

The input and output processing kernels of GGG are arbitrary normalized kernels. Its output behaviors may be signaling. This is data processing for the maximized conditional-output divergence.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P29
Formal statement
noncomputable section

open scoped BigOperators ENNReal

namespace QAlgorithms.Papers.Independent.Intakethird100.P29

attribute [local instance] Classical.propDecidable Classical.decEq

open QAlgorithms.Papers.Independent.Advance50.P47
  (Box IsCorrelation IsNoSignaling HasLocalModel TwoLocalBoxes losrTransform
   correlationMixture)

open QAlgorithms.Papers.Independent.Information100.P56 (IsLaw)

open QAlgorithms.Papers.Independent.Dependency50.P47 (Law)

/-- PDF p.5, Theorem 2, (17), proved on pp.11–12. The two input boxes are NS;
GW output boxes are allowed to be signaling. -/
theorem global_contractivity {s t : BellScenario} (g : GlobalWiring s t)
    (p q : Behavior s) (hp : IsNS p) (hq : IsNS q) :
    sb (g.apply p) (g.apply q) ≤ sb p q := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P29

end
Source
Nonlocality free wirings and the distinguishability between Bell boxes, arXiv:1611.06932v2, PDF p. 5, Theorem 2 (17)
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What the Lean code literally says, in plain math · gpt-6.1-sol

For any scenarios s,ts,ts,t, any nonnegative probability kernels I(x,y∣χ,ψ)I(x,y\mid\chi,\psi)I(x,y∣χ,ψ) on source input pairs and O(α,β∣a,b,x,y,χ,ψ)O(\alpha,\beta\mid a,b,x,y,\chi,\psi)O(α,β∣a,b,x,y,χ,ψ) on target output pairs, and any nonsignaling source correlations p,qp,qp,q, define

G(r)χψαβ=∑a,b,x,yO(α,β∣a,b,x,y,χ,ψ) rxyab I(x,y∣χ,ψ).G(r)_{\chi\psi}^{\alpha\beta} =\sum_{a,b,x,y} O(\alpha,\beta\mid a,b,x,y,\chi,\psi)\,r_{xy}^{ab}\,I(x,y\mid\chi,\psi).G(r)χψαβ​=a,b,x,y∑​O(α,β∣a,b,x,y,χ,ψ)rxyab​I(x,y∣χ,ψ).

Then S(G(p),G(q))≤S(p,q)S(G(p),G(q))\le S(p,q)S(G(p),G(q))≤S(p,q). Every scenario has positive integer input and output sizes; nonsignaling means nonnegative entries, ∑a,bpxyab=1\sum_{a,b}p_{xy}^{ab}=1∑a,b​pxyab​=1, Bob’s marginal independent of xxx, and Alice’s marginal independent of yyy, and likewise for qqq. The kernels are normalized for every choice of their conditioning arguments, with no locality requirement. For any real arrays r,ur,ur,u, S(r,u)=sup⁡x,yD(rxy∥uxy)S(r,u)=\sup_{x,y}D(r_{xy}\Vert u_{xy})S(r,u)=supx,y​D(rxy​∥uxy​), where D(P∥Q)=∞D(P\Vert Q)=\inftyD(P∥Q)=∞ if some Pi>0P_i>0Pi​>0 has Qi=0Q_i=0Qi​=0, and otherwise D(P∥Q)=max⁡{0,∑iPilog⁡(Pi/Qi)}D(P\Vert Q)=\max\{0,\sum_iP_i\log(P_i/Q_i)\}D(P∥Q)=max{0,∑i​Pi​log(Pi​/Qi​)}, interpreted in [0,∞][0,\infty][0,∞], using natural logarithms and the total conventions a/0=0a/0=0a/0=0, log⁡0=0\log0=0log0=0.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

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

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