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I.B.5: intercept-resend information and disturbance

Proved
QAlgorithms.Papers.Independent.Gap48.P25.interceptResend

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

prove2quantum

Let Alice's BB84 bit and all basis choices be uniform and independent. Eve independently intercepts a fraction p∈[0,1]p\in[0,1]p∈[0,1] of signals, measures in a random BB84 basis and resends her outcome. After sifting, the joint distribution is the Born transition law specified by these operations. Its error rate QQQ and both classical mutual informations, in bits, satisfy

Q=p/4,I(A:E)=I(B:E)=p/2=2Q.Q=p/4,\qquad I(A:E)=I(B:E)=p/2=2Q.Q=p/4,I(A:E)=I(B:E)=p/2=2Q.

The joint law is nonnegative and normalized. This evaluates this particular attack; the illustrative approximate 17 percent threshold is not asserted as an unconditional security threshold.

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)

/-- I.B.5, PDF p.5: evaluation of the specified uniform-basis intercept/resend
attack after sifting, without interpreting its error rate as a security threshold. -/
theorem interceptResend (p : ℝ) (hp : p ∈ Set.Icc (0 : ℝ) 1) :
    (∀ a b e, 0 ≤ irLaw p a b e) ∧
    (∑ a : Bool, ∑ b : Bool, ∑ e : IRRecord, irLaw p a b e) = 1 ∧
    irError p = p/4 ∧ classicalMI (irAE p) = p/2 ∧
    classicalMI (irBE p) = p/2 ∧ p/2 = 2*irError p := by sorry

end QAlgorithms.Papers.Independent.Gap48.P25

end
Source
The Security of Practical Quantum Key Distribution, arXiv:0802.4155v3, PDF p. 5, I.B.5: intercept-resend information and disturbance
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every real ppp with 0≤p≤10\le p\le10≤p≤1, let E\mathcal EE consist of a distinguished record ∅\varnothing∅ and the four records (r,e)(r,e)(r,e) with r,e∈{false,true}r,e\in\{\mathrm{false},\mathrm{true}\}r,e∈{false,true}. Define Jp(a,b,∅)=(1−p)/2J_p(a,b,\varnothing)=(1-p)/2Jp​(a,b,∅)=(1−p)/2 if a=ba=ba=b and 000 otherwise; define Jp(a,b,(true,e))=p/4J_p(a,b,(\mathrm{true},e))=p/4Jp​(a,b,(true,e))=p/4 if a=b=ea=b=ea=b=e and 000 otherwise; and define Jp(a,b,(false,e))=p/16J_p(a,b,(\mathrm{false},e))=p/16Jp​(a,b,(false,e))=p/16 for every a,b,ea,b,ea,b,e. The assertion is that all these values are nonnegative and ∑a,b,EJp(a,b,E)=1\sum_{a,b,E}J_p(a,b,E)=1∑a,b,E​Jp​(a,b,E)=1. Writing Err(p)=∑a≠b,EJp(a,b,E)\mathrm{Err}(p)=\sum_{a\ne b,E}J_p(a,b,E)Err(p)=∑a=b,E​Jp​(a,b,E), PAE(a,E)=∑bJp(a,b,E)P_{AE}(a,E)=\sum_bJ_p(a,b,E)PAE​(a,E)=∑b​Jp​(a,b,E), and PBE(b,E)=∑aJp(a,b,E)P_{BE}(b,E)=\sum_aJ_p(a,b,E)PBE​(b,E)=∑a​Jp​(a,b,E), it further asserts

Err(p)=p4,I(PAE)=p2,I(PBE)=p2,p2=2 Err(p).\mathrm{Err}(p)=\frac p4,\qquad I(P_{AE})=\frac p2,\qquad I(P_{BE})=\frac p2,\qquad \frac p2=2\,\mathrm{Err}(p).Err(p)=4p​,I(PAE​)=2p​,I(PBE​)=2p​,2p​=2Err(p).

Here I(P)=H(P1)+H(P2)−H(P)I(P)=H(P_1)+H(P_2)-H(P)I(P)=H(P1​)+H(P2​)−H(P), with P1,P2P_1,P_2P1​,P2​ the two marginals and HHH the base-two Shannon entropy, using zero contribution for zero masses. Both endpoints p=0p=0p=0 and p=1p=1p=1 are included.

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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