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Lemma 1, Eqs.(8)–(10): PBT diamond error

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QAlgorithms.Papers.Independent.Intakethird100.P49.pbt_diamond_error

by Gohan · Nov 1, 2026 · Mathlib 0df444a (Lean v4.33.1)

prove2quantum

Let d≥2d\ge2d≥2 and let Γd,M\Gamma_{d,M}Γd,M​ be the deterministic PBT channel using integer M≥2M\ge2M≥2, MMM normalized Bell pairs, the standard square-root measurement, classical communication of its outcome, and port selection. Let fe=⟨Φd∣(id⊗Γd,M)(Φd)∣Φd⟩f_e=\langle\Phi_d|(\mathrm{id}\otimes\Gamma_{d,M})(\Phi_d)|\Phi_d\ranglefe​=⟨Φd​∣(id⊗Γd,M​)(Φd​)∣Φd​⟩, with normalized ∣Φd⟩=d−1/2∑j∣j,j⟩|\Phi_d\rangle=d^{-1/2}\sum_j|j,j\rangle∣Φd​⟩=d−1/2∑j​∣j,j⟩. The channel is CPTP and depolarizing: Γ(X)=(1−ξd,M)X+ξd,Mtr⁡(X)I/d\Gamma(X)=(1-\xi_{d,M})X+\xi_{d,M}\operatorname{tr}(X)I/dΓ(X)=(1−ξd,M​)X+ξd,M​tr(X)I/d. Its actual unhalved diamond error satisfies

δd,M=2(1−fe)=2(d2−1)d2ξd,M≤2d(d−1)M.\delta_{d,M}=2(1-f_e)=\frac{2(d^2-1)}{d^2}\xi_{d,M}\le\frac{2d(d-1)}M.δd,M​=2(1−fe​)=d22(d2−1)​ξd,M​≤M2d(d−1)​.

Moreover δd,M→0\delta_{d,M}\to0δd,M​→0 as integer M→∞M\to\inftyM→∞. These identities relate the operational PBT construction to its depolarizing probability and give uniform convergence, including reference-entangled inputs.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P49
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P49

open QAlgorithms Filter

open scoped Matrix ComplexConjugate ComplexOrder BigOperators

attribute [local instance] Classical.propDecidable Classical.decEq

open QAlgorithms.Papers.Independent.Information100.P63 (Mat tensorPower)

open QAlgorithms.Papers.Independent.Dependency50.P18 (bipartiteTensor)

open QAlgorithms.Papers.Independent.Information100.P71 (diamond AdaptiveTest adaptiveInput adaptiveAccept)

open QAlgorithms.Papers.Independent.Bridge50.P25
  (LOCCOn normalizedChannelChoi TwoWayGenerationCode TwoWayChannelProtocol
   generationCodeError twoWayGenerationCapacity sendChannelRegister StateFunctional
   IsDimensionChangingLOCCMonotone privateStateInPartyOrder)

open QAlgorithms.Papers.Independent.Support50.P07 (amplitudeDampingChannel)

/-- Lemma 1, PDF p.3, (8)--(10), Methods pp.7--8: actual SRM PBT is
CPTP and depolarizing; full diamond error equals twice Bell infidelity.
The error bound is uniform over all inputs, including entangled references. -/
theorem pbt_diamond_error (d : ℕ) [NeZero d] (hd : 2 ≤ d) :
    (∀ M : ℕ, 2 ≤ M →
      IsChannel (pbtChannel d M) ∧
      (∀ X, pbtChannel d M X = ((1-pbtNumber d M : ℝ) : ℂ) • X +
        ((pbtNumber d M / d : ℝ) : ℂ) • (X.trace • (1 : Mat (Fin d)))) ∧
      pbtError d M = 2 * (1-pbtEntanglementFidelity d M) ∧
      pbtError d M = 2 * ((d : ℝ)^2-1) / (d : ℝ)^2 * pbtNumber d M ∧
      pbtError d M ≤ 2 * (d : ℝ) * (d-1 : ℝ) / M) ∧
    Tendsto (pbtError d) atTop (nhds 0) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P49

end
Source
Fundamental limits to quantum channel discrimination, arXiv:1803.02834v4, PDF p. 3, Lemma 1, Eqs.(8)–(10): PBT diamond error
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What the Lean code literally says, in plain math · gpt-6.1-sol

For every natural number ddd, equipped with the assumption d≠0d\ne0d=0, and satisfying d≥2d\ge2d≥2, the following holds. To specify the quantities involved, write Pd,M\mathcal P_{d,M}Pd,M​ for the map constructed as follows: on an input register and MMM ports, each of dimension ddd, define

Si[(x,a),(y,b)]={1/d,x=ai, y=bi, and aj=bj for every j≠i,0,otherwise,S=∑i=0M−1Si,R=f(S),f(t)=(t)−1,S_i[(x,a),(y,b)] =\begin{cases} 1/d,&x=a_i,\ y=b_i,\ \text{and }a_j=b_j\text{ for every }j\ne i,\\ 0,&\text{otherwise}, \end{cases} \quad S=\sum_{i=0}^{M-1}S_i,\quad R=f(S),\quad f(t)=(\sqrt t)^{-1},Si​[(x,a),(y,b)]={1/d,0,​x=ai​, y=bi​, and aj​=bj​ for every j=i,otherwise,​S=i=0∑M−1​Si​,R=f(S),f(t)=(t​)−1,

where f(S)f(S)f(S) uses continuous functional calculus and f(0)=0f(0)=0f(0)=0, and put

Qi=RSiR+1M(I−RSR).Q_i=RS_iR+\frac1M(I-RSR).Qi​=RSi​R+M1​(I−RSR).

For ports of output dimension eee, define the selection map by

Td,e,M(Z)u,v=∑i, p,q, b,cbi=u, ci=vbj=cj (j≠i)(Qi)q,p Z(p,b),(q,c),\mathcal T_{d,e,M}(Z)_{u,v} =\sum_{\substack{i,\ p,q,\ b,c\\ b_i=u,\ c_i=v\\ b_j=c_j\ (j\ne i)}} (Q_i)_{q,p}\,Z_{(p,b),(q,c)},Td,e,M​(Z)u,v​=i, p,q, b,cbi​=u, ci​=vbj​=cj​ (j=i)​∑​(Qi​)q,p​Z(p,b),(q,c)​,

where p,qp,qp,q index the input register together with its ddd-dimensional ports, and b,cb,cb,c index the eee-dimensional ports; the singleton output register is suppressed. With Φd=d−1∑x,y∣x,x⟩⟨y,y∣\Phi_d=d^{-1}\sum_{x,y}|x,x\rangle\langle y,y|Φd​=d−1∑x,y​∣x,x⟩⟨y,y∣, set Pd,M(X)=Td,d,M(X⊗Φd⊗M)\mathcal P_{d,M}(X)=\mathcal T_{d,d,M}(X\otimes\Phi_d^{\otimes M})Pd,M​(X)=Td,d,M​(X⊗Φd⊗M​). For any matrix XXX, let ∥X∥1=Re⁡tr⁡X†X\|X\|_1=\operatorname{Re}\operatorname{tr}\sqrt{X^\dagger X}∥X∥1​=RetrX†X​, and for a map F\mathcal FF with input dimension ddd, let

Δd(F)=sup⁡∥X∥1≤1∥(id⁡d⊗F)(X)∥1,\Delta_d(\mathcal F) =\sup_{\|X\|_1\le1}\|(\operatorname{id}_d\otimes\mathcal F)(X)\|_1,Δd​(F)=∥X∥1​≤1sup​∥(idd​⊗F)(X)∥1​,

where XXX ranges over all complex matrices on the two ddd-dimensional registers. Define

νd,M=1−Re⁡(Pd,M(∣0⟩⟨1∣)0,1),εd,M=Δd(id⁡−Pd,M),\nu_{d,M}=1-\operatorname{Re}\bigl(\mathcal P_{d,M}(|0\rangle\langle1|)_{0,1}\bigr),\quad \varepsilon_{d,M}=\Delta_d(\operatorname{id}-\mathcal P_{d,M}),νd,M​=1−Re(Pd,M​(∣0⟩⟨1∣)0,1​),εd,M​=Δd​(id−Pd,M​),

and

Fd,M=Re⁡⟨Ωd∣(id⁡d⊗Pd,M)(Φd)∣Ωd⟩,∣Ωd⟩=d−1/2∑x∣x,x⟩.F_{d,M} =\operatorname{Re}\langle\Omega_d| (\operatorname{id}_d\otimes\mathcal P_{d,M})(\Phi_d) |\Omega_d\rangle,\qquad |\Omega_d\rangle=d^{-1/2}\sum_x|x,x\rangle.Fd,M​=Re⟨Ωd​∣(idd​⊗Pd,M​)(Φd​)∣Ωd​⟩,∣Ωd​⟩=d−1/2x∑​∣x,x⟩.

For every natural number M≥2M\ge2M≥2, Pd,M\mathcal P_{d,M}Pd,M​ has a finite Kraus representation X↦∑jKjXKj†X\mapsto\sum_jK_jXK_j^\daggerX↦∑j​Kj​XKj†​ with ∑jKj†Kj=I\sum_jK_j^\dagger K_j=I∑j​Kj†​Kj​=I, and, for every complex d×dd\times dd×d matrix XXX,

Pd,M(X)=(1−νd,M)X+νd,Md tr⁡(X)I.\mathcal P_{d,M}(X) =(1-\nu_{d,M})X+\frac{\nu_{d,M}}d\,\operatorname{tr}(X)I.Pd,M​(X)=(1−νd,M​)X+dνd,M​​tr(X)I.

Moreover,

εd,M=2(1−Fd,M)=2(d2−1)d2νd,M≤2d(d−1)M,lim⁡M→∞εd,M=0.\varepsilon_{d,M} =2(1-F_{d,M}) =\frac{2(d^2-1)}{d^2}\nu_{d,M} \le\frac{2d(d-1)}M, \qquad \lim_{M\to\infty}\varepsilon_{d,M}=0.εd,M​=2(1−Fd,M​)=d22(d2−1)​νd,M​≤M2d(d−1)​,M→∞lim​εd,M​=0.

The finite-MMM assertions require M≥2M\ge2M≥2; the convergence assertion concerns the entire naturally indexed sequence.

Human review
  • Endorsed by Shuze Chen · Nov 1, 2026

    Confirmed by the moderator at approval.

  • Endorsed by Gohan · Nov 1, 2026

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

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