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Accepted Hardy settings agree

Proved
QAlgorithms.Papers.Independent.Intakethird100.P47.accepted_settings_agree

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

prove2quantum

Let p(a,b∣A,B)p(a,b\mid A,B)p(a,b∣A,B) be a nonnegative binary conditional distribution normalized for each pair of settings, and let w(A,B)w(A,B)w(A,B) be a nonnegative normalized input law. The joint law is w(A,B)p(a,b∣A,B)w(A,B)p(a,b\mid A,B)w(A,B)p(a,b∣A,B). Set S={a=b=0}S=\{a=b=0\}S={a=b=0}, s=∑A,Bw(A,B)p(00∣A,B)s=\sum_{A,B}w(A,B)p(00\mid A,B)s=∑A,B​w(A,B)p(00∣A,B), and, when s>0s>0s>0, let J(A,B)=w(A,B)p(00∣A,B)/sJ(A,B)=w(A,B)p(00\mid A,B)/sJ(A,B)=w(A,B)p(00∣A,B)/s be the accepted setting law.

Assume s>0s>0s>0 and the two cross-setting zero constraints p(00∣10)=p(00∣01)=0p(00\mid10)=p(00\mid01)=0p(00∣10)=p(00∣01)=0. Every unequal setting pair has zero joint acceptance mass, and

Pr⁡[A=B∣S]=∑A=BJ(A,B)=1.\Pr[A=B\mid S]=\sum_{A=B}J(A,B)=1.Pr[A=B∣S]=A=B∑​J(A,B)=1.

This gives perfect agreement of the raw setting bits under the ideal cross-setting constraints.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P47
Formal statement
namespace QAlgorithms.Papers.Independent.Intakethird100.P47

open scoped ComplexConjugate

open scoped BigOperators

/-- II B, PDF p.3, using (1) on p.2: accepted settings agree with probability one.
No restriction to qubits, uniform inputs or a claim of secrecy is involved. -/
theorem accepted_settings_agree (p : Behavior) (w : PairLaw)
    (hp : IsBehavior p) (hw : IsPairLaw w)
    (h10 : p true false false false = 0) (h01 : p false true false false = 0)
    (hs : 0 < siftingProbability p w) :
    (∀ A B, A ≠ B → acceptedMass p w A B = 0) ∧
    (∑ A, ∑ B, if A = B then acceptedLaw p w A B else 0) = 1 := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P47
Source
Device-independent quantum key distribution based on measurement inputs, arXiv:1308.6447v3, PDF p. 3, II B: perfect correlation of accepted settings
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every function p:{0,1}4→Rp:\{0,1\}^4\to\mathbb Rp:{0,1}4→R and function w:{0,1}2→Rw:\{0,1\}^2\to\mathbb Rw:{0,1}2→R, where 000 denotes false and 111 true, assume p(A,B,a,b)≥0p(A,B,a,b)\ge0p(A,B,a,b)≥0 for every choice of its four arguments and ∑a,bp(A,B,a,b)=1\sum_{a,b}p(A,B,a,b)=1∑a,b​p(A,B,a,b)=1 for every A,BA,BA,B; assume also w(A,B)≥0w(A,B)\ge0w(A,B)≥0 for every pair and ∑A,Bw(A,B)=1\sum_{A,B}w(A,B)=1∑A,B​w(A,B)=1. If p(1,0,0,0)=0p(1,0,0,0)=0p(1,0,0,0)=0, p(0,1,0,0)=0p(0,1,0,0)=0p(0,1,0,0)=0, and

S=∑A,Bw(A,B)p(A,B,0,0)>0,S=\sum_{A,B}w(A,B)p(A,B,0,0)>0,S=A,B∑​w(A,B)p(A,B,0,0)>0,

then w(A,B)p(A,B,0,0)=0w(A,B)p(A,B,0,0)=0w(A,B)p(A,B,0,0)=0 for every A≠BA\ne BA=B, and

∑A,B{w(A,B)p(A,B,0,0)/S,A=B,0,A≠B=1.\sum_{A,B} \begin{cases} w(A,B)p(A,B,0,0)/S,&A=B,\\ 0,&A\ne B \end{cases} =1.A,B∑​{w(A,B)p(A,B,0,0)/S,0,​A=B,A=B​=1.
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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