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Shared and private random data can be fixed

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QAlgorithms.Papers.Independent.Intakethird100.P11.randomness_canBeFixed

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

prove2quantum

Fix a finite normalized pure ensemble E={pi,∣vi⟩AB}\mathcal E=\{p_i,|v_i\rangle_{AB}\}E={pi​,∣vi​⟩AB​} in finite-dimensional complex Hilbert spaces, a positive blocklength nnn, and positive compressed dimensions dA,dBd_A,d_BdA​,dB​. Let (Ω,μ)(\Omega,\mu)(Ω,μ) be a probability space for all input-independent random data, including the decoder's random data. For each seed s∈Ωs\in\Omegas∈Ω, let csc_scs​ consist of independent local CPTP encoders with these same output dimensions and a joint CPTP decoder. Define its ensemble-average squared fidelity by

F(cs)=∑in(∏t=1npit)⟨vin∣cs(∣vin⟩⟨vin∣)∣vin⟩,∣vin⟩=⨂t=1n∣vit⟩.F(c_s)=\sum_{i^n}\Bigl(\prod_{t=1}^np_{i_t}\Bigr) \langle v_{i^n}|c_s(|v_{i^n}\rangle\langle v_{i^n}|)|v_{i^n}\rangle, \qquad |v_{i^n}\rangle=\bigotimes_{t=1}^n|v_{i_t}\rangle.F(cs​)=in∑​(t=1∏n​pit​​)⟨vin​∣cs​(∣vin​⟩⟨vin​∣)∣vin​⟩,∣vin​⟩=t=1⨂n​∣vit​​⟩.

If s↦F(cs)s\mapsto F(c_s)s↦F(cs​) is measurable, it is integrable and there is a seed s0s_0s0​ such that

F(cs0)≥∫ΩF(cs) dμ(s).F(c_{s_0})\ge\int_\Omega F(c_s)\,d\mu(s).F(cs0​​)≥∫Ω​F(cs​)dμ(s).

Thus fixing all random data preserves the dimension budgets without reducing the randomized average fidelity. Applied at each blocklength, this removes shared or private randomness from the achievable-rate criterion.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P11
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P11

open MeasureTheory Filter

open scoped BigOperators ComplexConjugate Matrix

open QAlgorithms.Papers.Independent.Dependency50.P19 (both)

open QAlgorithms.Papers.Independent.Information100.P27 (shannon)

attribute [local instance] Classical.propDecidable Classical.decEq

/-- PDF p.3, Section II: fixing every party's random data yields a valid deterministic
code with the same dimension budgets and fidelity at least its randomized average.
Measurability plus the normalized-source/channel bounds ensures genuine integrability. -/
theorem randomness_canBeFixed {I A B Omega : Type*}
    [Fintype I] [Fintype A] [Fintype B] [DecidableEq A] [DecidableEq B]
    [MeasurableSpace Omega] (mu : Measure Omega) [IsProbabilityMeasure mu]
    (p : I → ℝ) (hp : ∀ i, 0 ≤ p i) (htotal : ∑ i, p i = 1)
    (v : I → EuclideanSpace ℂ (A × B)) (hv : ∀ i, IsState (v i))
    (n da db : ℕ) (codes : Omega → DistributedBlockCode A B n da db)
    (hmeas : Measurable (fun seed => finiteFidelity p v (codes seed))) :
    Integrable (fun seed => finiteFidelity p v (codes seed)) mu ∧
      ∃ seed, (∫ s, finiteFidelity p v (codes s) ∂mu) ≤ finiteFidelity p v (codes seed) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P11

end
Source
On the distributed compression of quantum information, arXiv:quant-ph/0403042v3, PDF p. 3, Section II: shared and private randomness can be fixed
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What the Lean code literally says, in plain math · gpt-6.1-sol

Let I,A,BI,A,BI,A,B be finite types, with decidable equality on A,BA,BA,B, and let Ω\OmegaΩ be a measurable space equipped with a probability measure μ\muμ. Let p:I→Rp:I\to\mathbb Rp:I→R satisfy pi≥0p_i\ge0pi​≥0 for every iii and ∑ipi=1\sum_i p_i=1∑i​pi​=1, and let vi∈CA×Bv_i\in\mathbb C^{A\times B}vi​∈CA×B have Euclidean norm 111 for every iii, including labels of weight zero. Fix natural numbers n,dA,dBn,d_A,d_Bn,dA​,dB​ and, for every seed s∈Ωs\in\Omegas∈Ω, a distributed block code CsC_sCs​. Each code includes the requirements n,dA,dB>0n,d_A,d_B>0n,dA​,dB​>0, encoding channels EA,sE_{A,s}EA,s​ and EB,sE_{B,s}EB,s​ from the respective nnn-letter registers to dimensions dA,dBd_A,d_BdA​,dB​, and a decoding channel DsD_sDs​ back to the two nnn-letter registers. Here a channel is a map admitting a finite representation X↦∑jKjXKj†X\mapsto\sum_j K_jXK_j^\daggerX↦∑j​Kj​XKj†​ with ∑jKj†Kj=1\sum_jK_j^\dagger K_j=1∑j​Kj†​Kj​=1. Write Cs=Ds∘(EA,s⊗EB,s)\mathcal C_s=D_s\circ(E_{A,s}\otimes E_{B,s})Cs​=Ds​∘(EA,s​⊗EB,s​), where the two encoders act separately on their registers. For w:{0,…,n−1}→Iw:\{0,\ldots,n-1\}\to Iw:{0,…,n−1}→I, define Vw(a,b)=∏t=0n−1vw(t)(at,bt)V_w(a,b)=\prod_{t=0}^{n-1}v_{w(t)}(a_t,b_t)Vw​(a,b)=∏t=0n−1​vw(t)​(at​,bt​), Pw=VwVw†P_w=V_wV_w^\daggerPw​=Vw​Vw†​, and

F(s)=∑w(∏t=0n−1pw(t))Re⁡tr⁡ ⁣(Pw Cs(Pw)).F(s)=\sum_w\left(\prod_{t=0}^{n-1}p_{w(t)}\right) \operatorname{Re}\operatorname{tr}\!\left(P_w\,\mathcal C_s(P_w)\right).F(s)=w∑​(t=0∏n−1​pw(t)​)Retr(Pw​Cs​(Pw​)).

If the real function FFF is measurable, then it is integrable with respect to μ\muμ, and there exists a seed s∈Ωs\in\Omegas∈Ω such that ∫ΩF dμ≤F(s)\int_\Omega F\,d\mu\le F(s)∫Ω​Fdμ≤F(s). The normalization assumptions exclude empty I,A,BI,A,BI,A,B; no measurability of the code assignment itself is assumed beyond measurability of FFF.

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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