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§VI: exact noiseless-dimension converse

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QAlgorithms.Papers.Independent.Intakethird100.P65.noiseless_dimension_converse

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

prove2quantum

All systems have finite positive dimension and fixed computational bases. Matrix order is Loewner order and logarithms are base two.

Let N:A→B\mathcal N:A\to BN:A→B be CPTP and let m1,m2≥1m_1,m_2\ge1m1​,m2​≥1 be integers. Suppose N\mathcal NN exactly simulates idm1\mathrm{id}_{m_1}idm1​​ with NS assistance, and idm2\mathrm{id}_{m_2}idm2​​ exactly simulates N\mathcal NN with NS assistance. Then

m1≤m2.m_1\le m_2.m1​≤m2​.

Exact simulation means minimum half-diamond error zero. No nonzero-error version is asserted; this is the noiseless-dimension converse in the discussion.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P65
Formal statement
noncomputable section

open Filter QAlgorithms

open scoped BigOperators Matrix ComplexConjugate ComplexOrder Topology

namespace QAlgorithms.Papers.Independent.Intakethird100.P65

attribute [local instance] Classical.propDecidable Classical.decEq

open QAlgorithms.Papers.Independent.Dependency50.P09 (transposeBob)

open QAlgorithms.Papers.Independent.Dependency50.P35 (maxRelative)

open QAlgorithms.Papers.Independent.Independent2.P01 (dampingKraus damping)

open QAlgorithms.Papers.Independent.Gap48.P33 (phaseFlipChannel)

open QAlgorithms.Papers.Independent.Information100.P06 (Below)

open QAlgorithms.Papers.Independent.Information100.P34 (choi)

open QAlgorithms.Papers.Independent.Information100.P62 (Stochastic)

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

open QAlgorithms.Papers.Independent.Information100.P67 (IsSubnormalized purifiedDistance)

open QAlgorithms.Papers.Independent.Information100.P69 (replacer permute)

open QAlgorithms.Papers.Independent.Information100.P71 (diamond channelPower channelRelative)

open QAlgorithms.Papers.Independent.Support50.P39 (quantumMutualInformation)

variable {A B C D R : Type} [Fintype A] [DecidableEq A]
  [Fintype B] [DecidableEq B] [Fintype C] [DecidableEq C]
  [Fintype D] [DecidableEq D] [Fintype R] [DecidableEq R]

variable [Nonempty A] [Nonempty B] [Nonempty C] [Nonempty D] [Nonempty R]

/-- Section VI, exact noiseless-dimension converse, PDF p.15.
Both simulations use NS assistance and exact error zero. -/
theorem noiseless_dimension_converse (N : Superop A B) (hN : IsChannel N)
    (m1 m2 : ℕ) (h1 : 0 < m1) (h2 : 0 < m2)
    (hforward : minimumError .ns N (fun X : Mat (Fin m1) => X) = 0)
    (hbackward : minimumError .ns (fun X : Mat (Fin m2) => X) N = 0) :
    m1 ≤ m2 := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P65

end
Source
Quantum Channel Simulation and the Channel's Smooth Max-Information, arXiv:1807.05354v2, PDF p. 15, §VI: exact noiseless-dimension converse
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What the Lean code literally says, in plain math · gpt-6.1-sol

For finite index types A,BA,BA,B, equipped with decidable equality, let NNN be a channel from complex matrices on AAA to complex matrices on BBB, meaning that N(X)=∑jKjXKj†N(X)=\sum_jK_jXK_j^\daggerN(X)=∑j​Kj​XKj†​ for every XXX, for some finite Kraus family satisfying ∑jKj†Kj=I\sum_jK_j^\dagger K_j=I∑j​Kj†​Kj​=I. For maps T:I→JT:I\to JT:I→J and V:K→LV:K\to LV:K→L, define ENS(T,V)\mathcal E_{\mathrm{NS}}(T,V)ENS​(T,V) as the real infimum of the errors Δ(WT(Q),V)\Delta(W_T(Q),V)Δ(WT​(Q),V) over all channels Q:K×J→I×LQ:K\times J\to I\times LQ:K×J→I×L for which there exist channels F:K→IF:K\to IF:K→I and G:J→LG:J\to LG:J→L satisfying Tr⁡LQ(X)=F(Tr⁡JX)\operatorname{Tr}_LQ(X)=F(\operatorname{Tr}_JX)TrL​Q(X)=F(TrJ​X) and Tr⁡IQ(X)=G(Tr⁡KX)\operatorname{Tr}_IQ(X)=G(\operatorname{Tr}_KX)TrI​Q(X)=G(TrK​X) for every input matrix XXX, where

WT(Q)(X)ℓ,ℓ′=∑i,i′∈I∑j,j′∈JT(Eii′)j,j′ Q(X⊗Ejj′)(i,ℓ),(i′,ℓ′),Δ(S,V)=12sup⁡∥X∥1≤1∥(id⁡K⊗(S−V))(X)∥1.W_T(Q)(X)_{\ell,\ell'}= \sum_{i,i'\in I}\sum_{j,j'\in J} T(E_{ii'})_{j,j'}\,Q(X\otimes E_{jj'})_{(i,\ell),(i',\ell')}, \qquad \Delta(S,V)=\frac12\sup_{\|X\|_1\le1} \bigl\|(\operatorname{id}_K\otimes(S-V))(X)\bigr\|_1.WT​(Q)(X)ℓ,ℓ′​=i,i′∈I∑​j,j′∈J∑​T(Eii′​)j,j′​Q(X⊗Ejj′​)(i,ℓ),(i′,ℓ′)​,Δ(S,V)=21​∥X∥1​≤1sup​​(idK​⊗(S−V))(X)​1​.

Here the supremum ranges over all complex matrices XXX on K×KK\times KK×K, without positivity or trace-one requirements; the amplified map applies S−VS-VS−V to each block indexed by the reference register KKK, and ∥X∥1=Re⁡Tr⁡X†X\|X\|_1=\operatorname{Re}\operatorname{Tr}\sqrt{X^\dagger X}∥X∥1​=ReTrX†X​. For every pair of positive natural numbers m1,m2m_1,m_2m1​,m2​, including dimension one, if

ENS(N,id⁡m1)=0andENS(id⁡m2,N)=0,\mathcal E_{\mathrm{NS}}(N,\operatorname{id}_{m_1})=0 \quad\text{and}\quad \mathcal E_{\mathrm{NS}}(\operatorname{id}_{m_2},N)=0,ENS​(N,idm1​​)=0andENS​(idm2​​,N)=0,

where id⁡m\operatorname{id}_midm​ is the identity map on m×mm\times mm×m complex matrices, then m1≤m2m_1\le m_2m1​≤m2​. The two hypotheses assert that these infima equal zero; they do not explicitly require an admissible operation attaining zero error.

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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