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Both limiting fractions of polarized split channels

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QAlgorithms.Papers.Independent.Intakethird100.P14.channel_polarization

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

prove2quantum

Let WWW be any binary-input classical–quantum channel with normalized density outputs on a common complex Hilbert space. Its information I(W)I(W)I(W) uses a uniform binary input and base-two logarithms. For N=2nN=2^nN=2n, let WN(i)W_N^{(i)}WN(i)​ be the actual split channels obtained by encoding with GNG_NGN​, exposing the previous bits as a classical register, and averaging the later bits uniformly. For every real δ∈(0,1)\delta\in(0,1)δ∈(0,1),

∣{i:I(WN(i))∈(1−δ,1]}∣N⟶I(W),∣{i:I(WN(i))∈[0,δ)}∣N⟶1−I(W).\frac{\bigl|\{i:I(W_N^{(i)})\in(1-\delta,1]\}\bigr|}{N}\longrightarrow I(W),\qquad \frac{\bigl|\{i:I(W_N^{(i)})\in[0,\delta)\}\bigr|}{N}\longrightarrow1-I(W).N​{i:I(WN(i)​)∈(1−δ,1]}​​⟶I(W),N​{i:I(WN(i)​)∈[0,δ)}​​⟶1−I(W).

Both limits are taken as n→∞n\to\inftyn→∞. No symmetry, purity, finite-dimensionality, or strict inequality 0<I(W)<10<I(W)<10<I(W)<1 is assumed. These fractions quantify the information carried by the polarized good and bad channels.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P14
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P14

open Filter MeasureTheory

open scoped ENNReal NNReal ComplexOrder BigOperators

open QAlgorithms.RealRegisters (Hilbert)

open QAlgorithms.Papers.Independent.Dependency50.P33 (IsDensity)

open QAlgorithms.Papers.Independent.Dependency50.P13 (compression)

open QAlgorithms.Papers.Independent.Renew46.P44 (wordOutput)

attribute [local instance] Classical.propDecidable Classical.decEq

/-- Theorem 2, PDF p.4; proof p.8. Both endpoint fractions, with exactly the
source's open and closed interval endpoints, converge along N=2^n. -/
theorem channel_polarization {I : Type} (W : Bit → OutputCoefficients I) (hW : IsBinaryCqChannel W)
    (delta : ℝ) (hd0 : 0 < delta) (hd1 : delta < 1) :
    Tendsto (fun n =>
      ((Finset.univ.filter (fun i : PolarWire n =>
        ENNReal.ofReal (1 - delta) < symmetricInformation (splitChannel W n i) ∧
        symmetricInformation (splitChannel W n i) ≤ 1)).card : ℝ≥0∞) / (2 ^ n : ℕ))
      atTop (nhds (symmetricInformation W)) ∧
    Tendsto (fun n =>
      ((Finset.univ.filter (fun i : PolarWire n =>
        0 ≤ symmetricInformation (splitChannel W n i) ∧
        symmetricInformation (splitChannel W n i) < ENNReal.ofReal delta)).card : ℝ≥0∞) /
          (2 ^ n : ℕ)) atTop (nhds (1 - symmetricInformation W)) := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P14

end
Source
Polar codes for classical-quantum channels, arXiv:1109.2591v3, PDF p. 4, Theorem 2 (Channel Polarization)
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What the Lean code literally says, in plain math · gpt-6.1-sol

For any type III, let W:Z2→CI×IW:\mathbb Z_2\to\mathbb C^{I\times I}W:Z2​→CI×I have density arrays as outputs: each admits a countable expansion W(b)ij=∑r′ur(i)vr(j)‾W(b)_{ij}=\sum'_r u_r(i)\overline{v_r(j)}W(b)ij​=∑r′​ur​(i)vr​(j)​, with ur,vr∈ℓ2(I;C)u_r,v_r\in\ell^2(I;\mathbb C)ur​,vr​∈ℓ2(I;C) and summable products ∥ur∥∥vr∥\|u_r\|\|v_r\|∥ur​∥∥vr​∥; all its finite quadratic forms are real and nonnegative; and its real diagonal is summable with sum one. For any real 0<δ<10<\delta<10<δ<1, the assertion concerns the following split arrays. Put N=2nN=2^nN=2n, let bk(r)b_k(r)bk​(r) denote bit kkk, define rev⁡n(r)=(∑k<nbk(r)2n−1−k) mod N\operatorname{rev}_n(r)=(\sum_{k<n}b_k(r)2^{n-1-k})\bmod Nrevn​(r)=(∑k<n​bk​(r)2n−1−k)modN, and put Grt=∏k<nK(bk(rev⁡n(r)),bk(t))G_{rt}=\prod_{k<n}K(b_k(\operatorname{rev}_n(r)),b_k(t))Grt​=∏k<n​K(bk​(revn​(r)),bk​(t)), with K(a,0)=1, K(a,1)=aK(a,0)=1,\ K(a,1)=aK(a,0)=1, K(a,1)=a, over Z2\mathbb Z_2Z2​. For i<Ni<Ni<N, define arrays on Z2i×IN\mathbb Z_2^i\times I^NZ2i​×IN by

Vi(n)(b)(h,x),(h′,y)={2−(N−1)∑u∈Z2Nu<i=h, ui=b∏t<NW((uG)t)xt,yt,h=h′,0,h≠h′.V_i^{(n)}(b)_{(h,x),(h',y)} =\begin{cases} 2^{-(N-1)} \displaystyle\sum_{\substack{u\in\mathbb Z_2^N\\u_{<i}=h,\ u_i=b}} \prod_{t<N}W((uG)_t)_{x_t,y_t},&h=h',\\ 0,&h\ne h'. \end{cases}Vi(n)​(b)(h,x),(h′,y)​=⎩⎨⎧​2−(N−1)u∈Z2N​u<i​=h, ui​=b​∑​t<N∏​W((uG)t​)xt​,yt​​,0,​h=h′,h=h′.​

For any binary array VVV, set V‾=(V(0)+V(1))/2\overline V=(V(0)+V(1))/2V=(V(0)+V(1))/2 and I(V)=(D2(V(0)∥V‾)+D2(V(1)∥V‾))/2\mathcal I(V)=(D_2(V(0)\Vert\overline V)+D_2(V(1)\Vert\overline V))/2I(V)=(D2​(V(0)∥V)+D2​(V(1)∥V))/2, where D2(X∥Y)D_2(X\Vert Y)D2​(X∥Y) is the supremum over every finite orthonormal family of the quantity

{max⁡ ⁣{0,Re⁡tr⁡(f(A)−Alog⁡C−A+C)log⁡2},ker⁡C⊆ker⁡A,∞,otherwise.\begin{cases} \displaystyle\max\!\left\{0, \frac{\operatorname{Re}\operatorname{tr}(f(A)-A\log C-A+C)}{\log2}\right\}, &\ker C\subseteq\ker A,\\ \infty,&\text{otherwise}. \end{cases}⎩⎨⎧​max{0,log2Retr(f(A)−AlogC−A+C)​},∞,​kerC⊆kerA,otherwise.​

Here A,CA,CA,C are the compressions of OX,OYO_X,O_YOX​,OY​ to that family, f(t)=tlog⁡tf(t)=t\log tf(t)=tlogt, matrix functions use continuous functional calculus, and OXO_XOX​ is a chosen bounded operator on the relevant complex ℓ2\ell^2ℓ2 space with coefficients XXX, or zero if none exists. Then, in [0,∞][0,\infty][0,∞],

#{i<2n:1−δ<I(Vi(n))≤1}2n⟶I(W),#{i<2n:0≤I(Vi(n))<δ}2n⟶1−I(W).\frac{\#\{i<2^n:1-\delta<\mathcal I(V_i^{(n)})\le1\}}{2^n} \longrightarrow\mathcal I(W), \qquad \frac{\#\{i<2^n:0\le\mathcal I(V_i^{(n)})<\delta\}}{2^n} \longrightarrow 1-\mathcal I(W).2n#{i<2n:1−δ<I(Vi(n)​)≤1}​⟶I(W),2n#{i<2n:0≤I(Vi(n)​)<δ}​⟶1−I(W).

The subtraction in the second limit is truncated subtraction in [0,∞][0,\infty][0,∞]. The threshold inequalities are exactly the strict and non-strict inequalities displayed. The sequence includes n=0n=0n=0, and no countability assumption on III is imposed; empty III makes the density hypothesis impossible.

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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