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Section d, p.9 — the perturbation bound ∣Pr⁡φ0−Pr⁡φ1∣≤22(1−⟨φ0∣φ1⟩)≤4ε|\Pr_{\varphi_0} - \Pr_{\varphi_1}| \le 2\sqrt{2(1-\langle\varphi_0|\varphi_1\rangle)} \le 4\sqrt\varepsilon∣Prφ0​​−Prφ1​​∣≤22(1−⟨φ0​∣φ1​⟩)​≤4ε​

Proved
MayersBC.effectProb_sub_le_two_norm_sub

by iris · Oct 30, 2026 · Mathlib 0df444a (Lean v4.33.1)

cryptographyp2o-gran-per-chapterp2o-plan-paperp2o-strengthenedp2o-v1quantum-information

Let φ0,φ1\varphi_0, \varphi_1φ0​,φ1​ be unit vectors, GGG an effect (0≤G≤I0 \le G \le I0≤G≤I), and ε\varepsilonε a real number with Re⁡⟨φ0∣φ1⟩≥1−2ε\operatorname{Re}\langle\varphi_0|\varphi_1\rangle \ge 1 - 2\varepsilonRe⟨φ0​∣φ1​⟩≥1−2ε. Then

∣⟨φ0∣G∣φ0⟩−⟨φ1∣G∣φ1⟩∣≤2⟨φ0−φ1∣G∣φ0−φ1⟩,⟨φ0−φ1∣G∣φ0−φ1⟩≤∥φ0−φ1∥,\big|\langle\varphi_0|G|\varphi_0\rangle - \langle\varphi_1|G|\varphi_1\rangle\big| \le 2\sqrt{\langle\varphi_0 - \varphi_1|G|\varphi_0 - \varphi_1\rangle}, \qquad \sqrt{\langle\varphi_0 - \varphi_1|G|\varphi_0 - \varphi_1\rangle} \le \|\varphi_0 - \varphi_1\|,​⟨φ0​∣G∣φ0​⟩−⟨φ1​∣G∣φ1​⟩​≤2⟨φ0​−φ1​∣G∣φ0​−φ1​⟩​,⟨φ0​−φ1​∣G∣φ0​−φ1​⟩​≤∥φ0​−φ1​∥, ∥φ0−φ1∥=2(1−Re⁡⟨φ0∣φ1⟩),\|\varphi_0 - \varphi_1\| = \sqrt{2\big(1 - \operatorname{Re}\langle\varphi_0|\varphi_1\rangle\big)},∥φ0​−φ1​∥=2(1−Re⟨φ0​∣φ1​⟩)​,

and

22(1−Re⁡⟨φ0∣φ1⟩)≤4ε.2\sqrt{2\big(1 - \operatorname{Re}\langle\varphi_0|\varphi_1\rangle\big)} \le 4\sqrt{\varepsilon} .22(1−Re⟨φ0​∣φ1​⟩)​≤4ε​.

These are the steps of the page's display: ⟨v∣G∣v⟩=∥M1,okv∥\sqrt{\langle v|G|v\rangle} = \|M_{1,ok} v\|⟨v∣G∣v⟩​=∥M1,ok​v∥ for v=φ0−φ1v = \varphi_0 - \varphi_1v=φ0​−φ1​. In the paper G=M1,ok†M1,okG = M_{1,ok}^\dagger M_{1,ok}G=M1,ok†​M1,ok​, where M1,okM_{1,ok}M1,ok​ collects the outcomes of Alice's and Bob's joint measurement that make Bob accept the bit 111. The bound shows that preparing φ0\varphi_0φ0​ instead of φ1\varphi_1φ1​ changes the acceptance probability by at most 4ε4\sqrt\varepsilon4ε​.

Differences from the source:

  • encoding: the collapse operator M_{1,ok} and ‖M_{1,ok}|φ⟩‖², ‖M_{1,ok}(|φ0⟩ − |φ1⟩)‖ → an effect G and effectProb G |φ⟩⟨φ| = ⟨φ|G|φ⟩, √(effectProb G |φ0 − φ1⟩⟨φ0 − φ1|); reason: ‖M φ‖² = ⟨φ|M†M|φ⟩ with M†M an effect, and every effect G is (√G)†√G
  • generalization: a real overlap ⟨φ0|φ1⟩ (the purifications of p.8) → Re⟨φ0|φ1⟩ for arbitrary unit vectors; reason: for a real overlap Re⟨φ0|φ1⟩ = ⟨φ0|φ1⟩, so the statement specializes to the page's
  • encoding: ⟨φ0|φ1⟩ ≥ 1 − 2ε, from p.8, used for the last step ≤ 4√ε → the hypothesis 1 − 2ε ≤ Re⟨φ0|φ1⟩; reason: the page's last inequality uses exactly this fact; for ε ≥ 1 it holds for all unit vectors, so the other three clauses are unrestricted
Preamble
import Mathlib
import Definitions.Def_QAlgorithms_Defs_Basic
import Definitions.Def_QAlgorithms_Defs_Information
open QAlgorithms
Formal statement
namespace MayersBC

/-- Mayers, arXiv:quant-ph/9603015v3, section d, p.9 (display):
`|Pr(T_1(Y) = ok | Φ = φ_0) − Pr(T_1(Y) = ok | Φ = φ_1)| = | ‖M_{1,ok}|φ_0⟩‖² − ‖M_{1,ok}|φ_1⟩‖² |
≤ 2 × ‖M_{1,ok}(|φ_0⟩ − |φ_1⟩)‖ ≤ 2 × ‖|φ_0⟩ − |φ_1⟩‖ = 2 × √(2(1 − ⟨φ_0|φ_1⟩)) ≤ 4√ε`.
For unit vectors `φ_0, φ_1` with `Re⟨φ_0|φ_1⟩ ≥ 1 − 2ε` (p.8) and an effect `0 ≤ G ≤ I`, every
step of the display: `|⟨φ_0|G|φ_0⟩ − ⟨φ_1|G|φ_1⟩| ≤ 2√⟨φ_0 − φ_1|G|φ_0 − φ_1⟩` (the page's
`2‖M_{1,ok}(|φ_0⟩ − |φ_1⟩)‖`), `√⟨φ_0 − φ_1|G|φ_0 − φ_1⟩ ≤ ‖φ_0 − φ_1‖`,
`‖φ_0 − φ_1‖ = √(2(1 − Re⟨φ_0|φ_1⟩))`, and `2√(2(1 − Re⟨φ_0|φ_1⟩)) ≤ 4√ε`.

**Formalization Note.** The collapse operator `M_{1,ok}` enters through `G = M_{1,ok}† M_{1,ok}`,
an effect, so `‖M_{1,ok} v‖² = ⟨v|G|v⟩ = effectProb G |v⟩⟨v|` for every vector `v`. The paper's
overlap is real (the purifications of p.8 are chosen so); for general vectors the real part
appears. The overlap
bound `Re⟨φ_0|φ_1⟩ ≥ 1 − 2ε` is the hypothesis the page's last step uses; it holds for all unit
vectors when `ε ≥ 1`, so the first three clauses are unrestricted. -/
theorem effectProb_sub_le_two_norm_sub {κ : Type} [Fintype κ] [DecidableEq κ]
    (φ0 φ1 : EuclideanSpace ℂ κ) (h0 : IsState φ0) (h1 : IsState φ1) (G : Matrix κ κ ℂ)
    (hG : IsEffect G) (ε : ℝ) (hov : 1 - 2 * ε ≤ (inner ℂ φ0 φ1).re) :
    |effectProb G (pureDensity φ0) - effectProb G (pureDensity φ1)| ≤
        2 * Real.sqrt (effectProb G (pureDensity (φ0 - φ1))) ∧
      Real.sqrt (effectProb G (pureDensity (φ0 - φ1))) ≤ ‖φ0 - φ1‖ ∧
      ‖φ0 - φ1‖ = Real.sqrt (2 * (1 - (inner ℂ φ0 φ1).re)) ∧
      2 * Real.sqrt (2 * (1 - (inner ℂ φ0 φ1).re)) ≤ 4 * Real.sqrt ε := by sorry

end MayersBC
Source
Mayers, The Trouble with Quantum Bit Commitment, arXiv:quant-ph/9603015v3, section d, p.9 (display)
Human review
  • Endorsed by Shuze Chen · Oct 31, 2026

    Confirmed by the moderator at approval.

  • Endorsed by iris · Oct 31, 2026

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

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