IV.B.4: weak-laser, zero-error quadratic approximation
ProvedQAlgorithms.Papers.Independent.Gap48.P25.zeroErrorOptimumprove2quantum
Write for the total transmission. In the zero-error weak-pulse truncation with negligible higher photons and dark counts and perfect error correction, the normalized rate proxy is for . It has the unique maximum
Consequently, for with other transmission factors fixed, the optimized proxy equals . The source's photon-number approximations define this quadratic proxy; no exact Poisson optimization is asserted.
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)
/-- IV.B.4, PDF p.29: exact optimization of the zero-error weak-pulse proxy. -/
theorem zeroErrorOptimum (s : ℝ) (hs : 0 < s) (hs1 : s ≤ 1) :
zeroProxy s s = s^2/2 ∧
(∀ mu : ℝ, 0 ≤ mu → zeroProxy s mu ≤ s^2/2) ∧
(∀ mu : ℝ, 0 ≤ mu → (zeroProxy s mu = s^2/2 ↔ mu = s)) ∧
(∀ t b : ℝ, (t*b)^2/2 = t^2*(b^2/2)) := by sorry
end QAlgorithms.Papers.Independent.Gap48.P25
end
Source
The Security of Practical Quantum Key Distribution, arXiv:0802.4155v3, PDF p. 29, IV.B.4: weak-laser, zero-error quadratic approximation
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What the Lean code literally says, in plain math · gpt-6.1-sol
For every real with , define . Then ; for every real , , with equality if and only if . The range of has no upper bound. In addition, for all real , without sign or size restrictions,
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