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Proof of Theorem 19, p. 23 — Tr⁡(Piσi)=1/2+3ε\operatorname{Tr}(\mathbb P_i\sigma_i) = 1/2 + 3\varepsilonTr(Pi​σi​)=1/2+3ε

Proved
ShadowTomography.QuantumLB.trace_sigma_self

by mikedeng1 · Oct 5, 2026 · Mathlib 0df444a (Lean v4.33.1)

p2o-batch-pfp1bp2o-gran-per-chapterp2o-plan-paperp2o-v1quantum-measurementshadow-tomography

Let N≥1N\ge 1N≥1, let P\mathbb PP be the orthogonal projection onto an N/2N/2N/2-dimensional subspace of CN\mathbb C^NCN, let ε∈R\varepsilon\in\mathbb Rε∈R, and let

σ:=(1−6ε)IN+6ε⋅2NP.\sigma := (1-6\varepsilon)\frac{\mathbb I}{N} + 6\varepsilon\cdot\frac2N\mathbb P .σ:=(1−6ε)NI​+6ε⋅N2​P.

Then the measurement P\mathbb PP accepts σ\sigmaσ with probability

Tr⁡(Pσ)=12+3ε.\operatorname{Tr}(\mathbb P\sigma) = \frac12 + 3\varepsilon .Tr(Pσ)=21​+3ε.

So the designated measurement Pi\mathbb P_iPi​ is biased by 3ε3\varepsilon3ε towards accepting its own hard state σi\sigma_iσi​.

Formalization Note No sign condition on ε\varepsilonε is needed. The hypothesis N≥1N\ge1N≥1 excludes the empty matrix, whose trace is 000.

Preamble
import Mathlib
import Definitions.Def_ShadowTomography_QuantumLB_IsHalfProjector
import Definitions.Def_ShadowTomography_QuantumLB_sigmaState
Formal statement
namespace ShadowTomography.QuantumLB

/-- Proof of Theorem 19, p. 23: `Tr(ℙ σ) = 1/2 + 3ε` for `σ = (1 − 6ε) 𝕀/N + 6ε (2/N) ℙ`. -/
theorem trace_sigma_self {N : ℕ} (hN : 1 ≤ N) (P : Matrix (Fin N) (Fin N) ℂ)
    (hP : IsHalfProjector P) (ε : ℝ) :
    (P * sigmaState P ε).trace.re = 1 / 2 + 3 * ε := by sorry

end ShadowTomography.QuantumLB
Source
Aaronson, Shadow Tomography of Quantum States, arXiv:1711.01053v2, p. 23, proof of Theorem 19, display for Tr(ℙ_iσ_i)
Human review
  • Endorsed by Shuze Chen · Oct 5, 2026

    Confirmed by the moderator at approval.

  • Endorsed by mikedeng1 · Oct 5, 2026

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

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