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Exact GHZ strengths and optimal sampling laws

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QAlgorithms.Papers.Independent.Intakethird100.P80.ghz_strength

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

prove2quantum

Use the fixed GHZ experiment of Appendix III-F. On settings 111,122,212,221111,122,212,221111,122,212,221, four allowed parity outcomes have probability 1/41/41/4 each: the number of TTT outcomes is odd at 111111111 and even at the other three settings. At all other settings every outcome has probability 1/81/81/8. Let σ∘\sigma^\circσ∘ sample all eight settings uniformly and let σ∗\sigma^*σ∗ assign probability 1/41/41/4 to each of the four parity settings.

The uniform law is optimal among product setting laws, while σ∗\sigma^*σ∗ is optimal among all setting laws, and

SGHZUNI=SGHZUC=12log⁡2(4/3),SGHZCOR=log⁡2(4/3).S^{\rm UNI}_{\rm GHZ}=S^{\rm UC}_{\rm GHZ}=\tfrac12\log_2(4/3),\qquad S^{\rm COR}_{\rm GHZ}=\log_2(4/3).SGHZUNI​=SGHZUC​=21​log2​(4/3),SGHZCOR​=log2​(4/3).

A single local law realizes Table XXIX at every setting: its probabilities at a parity setting are 3/163/163/16 on allowed outcomes and 1/161/161/16 on the others, and are 1/81/81/8 at other settings. This law is optimal for both displayed setting laws.

The four settings and the 1/41/41/4 masses follow Table XXVIII and equation (35); the p.24 prose mistakenly prints (0.125,0)(0.125,0)(0.125,0) and an even number of setting-1 measurements. This statement corrects those two typos and makes no factor-4.5 comparison.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P80
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P80

open scoped BigOperators ENNReal Topology Classical

open MeasureTheory Filter

/-- PDF pp.8,17,21,24: exact GHZ optima, optimal setting laws and a common realizing
local law for Table XXIX. The p.24 prose typos are corrected as documented above.
No equality or literal lower bound with the factor 4.5 is claimed. -/
theorem ghz_strength :
    ghzCorrelatedSettings ∈ stdSimplex ℝ (Settings GHZScenario) ∧
    Uncorrelated (uniformSettings GHZScenario) ∧
    uniformStrength ghzTable = uncorrelatedStrength ghzTable ∧
    uncorrelatedStrength ghzTable = ENNReal.ofReal (Real.logb 2 (4 / 3) / 2) ∧
    lowerValue ghzTable ghzCorrelatedSettings = correlatedStrength ghzTable ∧
    correlatedStrength ghzTable = ENNReal.ofReal (Real.logb 2 (4 / 3)) ∧
    ∃ p : PiLocal GHZScenario, localTable p.1 = ghzLocalTable ∧
      statisticalPayoff ghzTable (uniformSettings GHZScenario) p.1 = uniformStrength ghzTable ∧
      statisticalPayoff ghzTable ghzCorrelatedSettings p.1 = correlatedStrength ghzTable := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P80

end
Source
The statistical strength of nonlocality proofs, arXiv:quant-ph/0307125v2, PDF p. 8, Appendix III-F: optimal GHZ setting laws and exact strengths
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What the Lean code literally says, in plain math · gpt-6.1-sol

Consider three parties, each with settings and outcomes in {0,1}\{0,1\}{0,1}. Let A={0,1}3A=\{0,1\}^3A={0,1}3 be the setting space, and let VVV consist of assignments via∈{0,1}v_{ia}\in\{0,1\}via​∈{0,1} for every party i∈{0,1,2}i\in\{0,1,2\}i∈{0,1,2} and setting a∈{0,1}a\in\{0,1\}a∈{0,1}. Denote the probability simplices on these spaces by ΔA,ΔV\Delta_A,\Delta_VΔA​,ΔV​, and let U⊆ΔA\mathcal U\subseteq\Delta_AU⊆ΔA​ consist of distributions factoring into three single-party setting distributions. A setting aaa is constrained when a0+a1+a2a_0+a_1+a_2a0​+a1​+a2​ is 000 or 222; an outcome xxx is allowed when (x0+x1+x2) mod 2(x_0+x_1+x_2)\bmod2(x0​+x1​+x2​)mod2 is 111 if a=(0,0,0)a=(0,0,0)a=(0,0,0) and is 000 otherwise. Define Q(a,x)Q(a,x)Q(a,x) to be 1/41/41/4 for allowed outcomes at constrained settings, 000 for other outcomes at constrained settings, and 1/81/81/8 at unconstrained settings. Define R(a,x)R(a,x)R(a,x) to be 3/163/163/16 for allowed outcomes at constrained settings, 1/161/161/16 for other outcomes at constrained settings, and 1/81/81/8 at unconstrained settings. Put u(a)=1/8u(a)=1/8u(a)=1/8 and let s∗(a)=1/4s_*(a)=1/4s∗​(a)=1/4 at constrained settings and 000 otherwise. For p∈ΔVp\in\Delta_Vp∈ΔV​, set Lp(a,x)=∑v: ∀i, vi,ai=xip(v)L_p(a,x)=\sum_{v:\,\forall i,\ v_{i,a_i}=x_i}p(v)Lp​(a,x)=∑v:∀i, vi,ai​​=xi​​p(v). Define K(s,p)K(s,p)K(s,p) using the joint functions q(a,x)=s(a)Q(a,x)q(a,x)=s(a)Q(a,x)q(a,x)=s(a)Q(a,x) and r(a,x)=s(a)Lp(a,x)r(a,x)=s(a)L_p(a,x)r(a,x)=s(a)Lp​(a,x): it is +∞+\infty+∞ if some q(a,x)>0q(a,x)>0q(a,x)>0 has r(a,x)=0r(a,x)=0r(a,x)=0, and otherwise it is the nonnegative part of ∑a,xq(a,x)log⁡2(q(a,x)/r(a,x))\sum_{a,x}q(a,x)\log_2(q(a,x)/r(a,x))∑a,x​q(a,x)log2​(q(a,x)/r(a,x)), with every summand having q(a,x)=0q(a,x)=0q(a,x)=0 replaced by 000. All these values lie in [0,+∞][0,+\infty][0,+∞]. Set F=inf⁡p∈ΔVK(u,p)F=\inf_{p\in\Delta_V}K(u,p)F=infp∈ΔV​​K(u,p), U=sup⁡s∈Uinf⁡p∈ΔVK(s,p)U=\sup_{s\in\mathcal U}\inf_{p\in\Delta_V}K(s,p)U=sups∈U​infp∈ΔV​​K(s,p), and C=sup⁡s∈ΔAinf⁡p∈ΔVK(s,p)C=\sup_{s\in\Delta_A}\inf_{p\in\Delta_V}K(s,p)C=sups∈ΔA​​infp∈ΔV​​K(s,p). The declaration asserts that s∗∈ΔAs_*\in\Delta_As∗​∈ΔA​, that uuu factors as u(a)=∏i=02ui(ai)u(a)=\prod_{i=0}^2u_i(a_i)u(a)=∏i=02​ui​(ai​) for some probability vectors uiu_iui​ on {0,1}\{0,1\}{0,1}, and that

F=U,U=max⁡{0,12log⁡2(4/3)},inf⁡p∈ΔVK(s∗,p)=C,C=max⁡{0,log⁡2(4/3)}.F=U,\qquad U=\max\{0,\tfrac12\log_2(4/3)\},\qquad \inf_{p\in\Delta_V}K(s_*,p)=C,\qquad C=\max\{0,\log_2(4/3)\}.F=U,U=max{0,21​log2​(4/3)},p∈ΔV​inf​K(s∗​,p)=C,C=max{0,log2​(4/3)}.

It also asserts the existence of p∈ΔVp\in\Delta_Vp∈ΔV​ such that Lp=RL_p=RLp​=R, K(u,p)=FK(u,p)=FK(u,p)=F, and K(s∗,p)=CK(s_*,p)=CK(s∗​,p)=C.

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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