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Monotonicity and endpoints of the ancillary-overlap lower bound

Proved
QAlgorithms.Papers.Independent.Intakenext100.P97.bound_monotonicity

by Gohan · Oct 31, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Fix 0≤f<10\le f<10≤f<1 and positive integers N,MN,MN,M, and set L=N+ML=N+ML=N+M. Define the scalar function

BN,M(f,ϕ)=fNϕ−fL1−f2Nϕ21−f2L.B_{N,M}(f,\phi)=f^N\phi-\frac{f^L\sqrt{1-f^{2N}\phi^2}}{\sqrt{1-f^{2L}}}.BN,M​(f,ϕ)=fNϕ−1−f2L​fL1−f2Nϕ2​​.

This function is nondecreasing on [fM,1][f^M,1][fM,1], and its minimum and maximum occur at the endpoints:

BN,M(f,fM)=0,0≤BN,M(f,ϕ)≤BN,M(f,1)(fM≤ϕ≤1).B_{N,M}(f,f^M)=0,\qquad 0\le B_{N,M}(f,\phi)\le B_{N,M}(f,1)\quad(f^M\le\phi\le1).BN,M​(f,fM)=0,0≤BN,M​(f,ϕ)≤BN,M​(f,1)(fM≤ϕ≤1).

For one original and one additional copy, the maximum has the explicit value

B1,1(f,1)=f−f21+f2.B_{1,1}(f,1)=f-\frac{f^2}{\sqrt{1+f^2}}.B1,1​(f,1)=f−1+f2​f2​.

This describes the scalar lower bound as ancillary overlap varies; it makes no attainability assertion about an arbitrary device.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakenext100_P97
Formal statement
noncomputable section

open scoped Matrix ComplexConjugate

namespace QAlgorithms.Papers.Independent.Intakenext100.P97

open QAlgorithms.Papers.Independent.Information100.P67
  (squaredFidelity sineDistance receiverChannel)

open QAlgorithms.Papers.Independent.Dependency50.P48 (densityPower)

/-- PDF p.4, paragraphs after Eqs. (21) and (23). The scalar bound is
nondecreasing (constant zero for `f=0`), with the stated endpoint minimum
and maximum. This is not an attainability assertion about arbitrary cloners. -/
theorem bound_monotonicity {N M : ℕ} (hN : 1 ≤ N) (hM : 1 ≤ M)
    (f : ℝ) (hf0 : 0 ≤ f) (hf1 : f < 1) :
    MonotoneOn (cloningBound N M f) (Set.Icc (f ^ M) 1) ∧
    cloningBound N M f (f ^ M) = 0 ∧
    (∀ phi ∈ Set.Icc (f ^ M) 1,
      0 ≤ cloningBound N M f phi ∧ cloningBound N M f phi ≤ cloningBound N M f 1) ∧
    cloningBound 1 1 f 1 = standardBound f := by sorry

end QAlgorithms.Papers.Independent.Intakenext100.P97

end
Source
Lower bound on the relative error of mixed-state cloning and related operations, arXiv:quant-ph/0208159v2, PDF p. 4, §IV, paragraphs after Eqs. (21) and (23)
Read-back

What the Lean code literally says, in plain math · gpt-6.1-sol

For all natural numbers N,M≥1N,M\ge 1N,M≥1 and real numbers fff with 0≤f<10\le f<10≤f<1, define

BN,M,f(ϕ)=fNϕ−fN+M1−f2Nϕ21−f2(N+M).B_{N,M,f}(\phi) =f^N\phi- \frac{f^{N+M}\sqrt{1-f^{2N}\phi^2}} {\sqrt{1-f^{2(N+M)}}}.BN,M,f​(ϕ)=fNϕ−1−f2(N+M)​fN+M1−f2Nϕ2​​.

Then BN,M,fB_{N,M,f}BN,M,f​ is nondecreasing on the closed interval [fM,1][f^M,1][fM,1]: whenever fM≤ϕ≤ψ≤1f^M\le\phi\le\psi\le1fM≤ϕ≤ψ≤1, one has BN,M,f(ϕ)≤BN,M,f(ψ)B_{N,M,f}(\phi)\le B_{N,M,f}(\psi)BN,M,f​(ϕ)≤BN,M,f​(ψ). Moreover,

BN,M,f(fM)=0,0≤BN,M,f(ϕ)≤BN,M,f(1)for every ϕ∈[fM,1],B_{N,M,f}(f^M)=0,\qquad 0\le B_{N,M,f}(\phi)\le B_{N,M,f}(1) \quad\text{for every }\phi\in[f^M,1],BN,M,f​(fM)=0,0≤BN,M,f​(ϕ)≤BN,M,f​(1)for every ϕ∈[fM,1],

and

B1,1,f(1)=f−f21+f2.B_{1,1,f}(1)=f-\frac{f^2}{\sqrt{1+f^2}}.B1,1,f​(1)=f−1+f2​f2​.

The case f=0f=0f=0 is included; in that case BN,M,0B_{N,M,0}BN,M,0​ is identically zero. The denominator in the definition of BN,M,fB_{N,M,f}BN,M,f​ is positive under the stated hypotheses.

Human review
  • Endorsed by Shuze Chen · Oct 31, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Oct 31, 2026

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

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