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Geometric support ensures exact Majorana-ring correction

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QAlgorithms.Papers.Independent.Intakethird100.P44.majorana_ring_geometric_correction

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

prove2quantum

All Hilbert spaces are finite dimensional and nonzero, and every channel is completely positive and trace preserving on the full matrix algebra. Consider 2n2n2n Majorana operators wa=wa†w_a=w_a^\daggerwa​=wa†​ on the 2n2^n2n-dimensional Fock space, satisfying {wa,wb}=2δabI\{w_a,w_b\}=2\delta_{ab}I{wa​,wb​}=2δab​I. There are 2k>02k>02k>0 free modes in cyclic order, with even-length intervals IjI_jIj​ of nearest-neighbor paired modes between consecutive free modes. The isometry WWW encodes all 2k2^k2k free-mode states and initializes each paired fermion in its specified vacuum; its range projector is the product of the paired-mode vacuum projectors. Write CCC for total parity and P(X)=(X+CXC)/2\mathcal P(X)=(X+CXC)/2P(X)=(X+CXC)/2. Let d=min⁡j∣Ij∣d=\min_j|I_j|d=minj​∣Ij​∣. Let N(X)=∑iEiXEi†\mathcal N(X)=\sum_iE_iXE_i^\daggerN(X)=∑i​Ei​XEi†​ have a normalized finite Kraus family. Suppose each whole EiE_iEi​ is an even Majorana polynomial supported on some cyclic interval of length ℓi\ell_iℓi​ with 2ℓi≤d2\ell_i\le d2ℓi​≤d. The intervals may differ with iii. Then, writing P±=(I±C)/2P_\pm=(I\pm C)/2P±​=(I±C)/2, there is one complex array λijs\lambda_{ijs}λijs​ such that

W†Ei†Ej(PsBPs)W=λijsW†(PsBPs)WW^\dagger E_i^\dagger E_j(P_sBP_s)W=\lambda_{ijs}W^\dagger(P_sBP_s)WW†Ei†​Ej​(Ps​BPs​)W=λijs​W†(Ps​BPs​)W

for every i,j,si,j,si,j,s and every BBB commuting with the whole-chain even algebra. Moreover a CPTP recovery strongly local to that algebra exactly recovers P\mathcal PP on the code. If d=0d=0d=0, only scalar Kraus operators meet the support condition.

This is finite exact correction under geometric support, without a common support region for the channel or a standard full-code Knill–Laflamme assertion.

Preamble
import Definitions.Def_QAlgorithms_Papers_Independent_Intakethird100_P44
Formal statement
noncomputable section

namespace QAlgorithms.Papers.Independent.Intakethird100.P44

open scoped Matrix ComplexConjugate ComplexOrder

open QAlgorithms.Papers.Independent.Information100.P60 (Mat)

open QAlgorithms.Papers.Independent.Information100.P67 (mapFirst)

open QAlgorithms.Papers.Independent.Claimed50.P48 (operatorTraceDual)

open QAlgorithms.Papers.Independent.Renew46.P43 (purification)

variable {H K L J E F B : Type*}

variable [Fintype H] [DecidableEq H] [Fintype K] [DecidableEq K]

variable [Fintype L] [DecidableEq L] [Fintype J] [DecidableEq J]

variable [Fintype E] [DecidableEq E] [Fintype F] [DecidableEq F]

variable [Fintype B] [DecidableEq B]

/-- PDF pp.10--11, Section IV F: each even Kraus operator may have its OWN
geometric interval, of length at most half the shortest paired interval.
Conclusion is Eq.(54) and exact strong-local physical correction; the disputed
whole-code standard-KL reduction is not used or asserted. 
Parity correction, PDF p.2 Eq.(1): printed i^(|omega|-1) for Majorana labels;
changed to i^m on 2m ordered modes. Why: the printed four-mode value is
anti-Hermitian with square -I, whereas the source requires parity sectors of
a Hermitian involution. Only this normalization (up to sign) is corrected. -/
theorem majorana_ring_geometric_correction {n k : ℕ}
    (f : Fermions n) (r : RingLayout n k) (code : RingCode f r)
    (noise : J → Mat (Fin (2 ^ n))) (hnoise : IsKrausFamily noise)
    (hsupport : ∀ j, ∃ length : ℕ, 2 * length ≤ minimumGap r ∧
      HasIntervalSupport f (noise j) length) :
    RegionalCoefficients (evenRegion f Finset.univ : Set _) (totalParity f)
      noise code.W ∧
    StrongCorrectable (evenRegion f Finset.univ : Set _) (totalParity f)
      (krausApply noise) code.W := by sorry

end QAlgorithms.Papers.Independent.Intakethird100.P44

end
Source
Approximate recovery with locality and symmetry constraints, arXiv:1806.10324v2, PDF p. 10, §IV F: geometric support implies exact correction on the Majorana ring
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What the Lean code literally says, in plain math · gpt-6.1-sol

For all natural numbers n,kn,kn,k, let w0,…,w2n−1w_0,\ldots,w_{2n-1}w0​,…,w2n−1​ be Hermitian complex 2n×2n2^n\times2^n2n×2n matrices satisfying wiwj+wjwi=2δijIw_iw_j+w_jw_i=2\delta_{ij}Iwi​wj​+wj​wi​=2δij​I, and let a ring layout specify n,k>0n,k>0n,k>0 and strictly increasing free indices u0,…,u2k−1u_0,\ldots,u_{2k-1}u0​,…,u2k−1​ with even cyclic gaps gj=(u(j+1) mod 2k+2n−uj−1) mod 2ng_j=(u_{(j+1)\bmod 2k}+2n-u_j-1)\bmod 2ngj​=(u(j+1)mod2k​+2n−uj​−1)mod2n. Let WWW be a complex 2n×2k2^n\times2^k2n×2k matrix with W†W=IW^\dagger W=IW†W=I and

WW†=∏j=02k−1 ∏t=0gj/2−112(I−i w(uj+1+2t) mod 2n w(uj+2+2t) mod 2n),WW^\dagger= \prod_{j=0}^{2k-1}\ \prod_{t=0}^{g_j/2-1} \frac12\left(I-\mathrm i\, w_{(u_j+1+2t)\bmod 2n}\, w_{(u_j+2+2t)\bmod 2n}\right),WW†=j=0∏2k−1​ t=0∏gj​/2−1​21​(I−iw(uj​+1+2t)mod2n​w(uj​+2+2t)mod2n​),

ordered by increasing jjj and then increasing ttt, with empty products equal to III. For a finite index type JJJ, let AjA_jAj​ be complex 2n×2n2^n\times2^n2n×2n matrices satisfying ∑j∈JAj†Aj=I\sum_{j\in J}A_j^\dagger A_j=I∑j∈J​Aj†​Aj​=I. Suppose that for each j∈Jj\in Jj∈J there exist a natural number ℓj\ell_jℓj​ and a starting index sj<2ns_j<2nsj​<2n such that 2ℓj≤min⁡(2n,g0,…,g2k−1)2\ell_j\le\min(2n,g_0,\ldots,g_{2k-1})2ℓj​≤min(2n,g0​,…,g2k−1​) and AjA_jAj​ belongs to the complex linear span of even-length products of matrices waw_awa​ whose indices satisfy (a+2n−sj) mod 2n<ℓj(a+2n-s_j)\bmod 2n<\ell_j(a+2n−sj​)mod2n<ℓj​; repetitions, arbitrary ordering, and empty products are allowed. In particular, ℓj=0\ell_j=0ℓj​=0 is permitted and then AjA_jAj​ is a scalar multiple of III; an empty JJJ cannot satisfy the normalization above. Write A\mathcal AA for the complex linear span of all even-length products of the waw_awa​, set C=inw0⋯w2n−1C=\mathrm i^n w_0\cdots w_{2n-1}C=inw0​⋯w2n−1​, and put Pb=12(I+(−1)bC)P_b=\frac12(I+(-1)^bC)Pb​=21​(I+(−1)bC) for b∈{0,1}b\in\{0,1\}b∈{0,1}. The first conclusion is that there exist complex coefficients λijb\lambda_{ijb}λijb​ such that, for every i,j∈Ji,j\in Ji,j∈J, every b∈{0,1}b\in\{0,1\}b∈{0,1}, and every matrix YYY commuting with every element of A\mathcal AA,

W†Ai†Aj(PbYPb)W=λijb W†(PbYPb)W.W^\dagger A_i^\dagger A_j(P_bYP_b)W =\lambda_{ijb}\,W^\dagger(P_bYP_b)W.W†Ai†​Aj​(Pb​YPb​)W=λijb​W†(Pb​YPb​)W.

The second conclusion is that there exists a channel R\mathcal RR, admitting a finite Kraus representation with Kraus operators KaK_aKa​ satisfying ∑aKa†Ka=I\sum_aK_a^\dagger K_a=I∑a​Ka†​Ka​=I, whose trace dual R∨(Y)ab=tr⁡(R(Eba)Y)\mathcal R^\vee(Y)_{ab}=\operatorname{tr}(\mathcal R(E_{ba})Y)R∨(Y)ab​=tr(R(Eba​)Y) sends every element of A\mathcal AA into A\mathcal AA and fixes every matrix commuting with A\mathcal AA, and such that

R(∑j∈JAjWZW†Aj†)=12(WZW†+CWZW†C)\mathcal R\left(\sum_{j\in J}A_jWZW^\dagger A_j^\dagger\right) =\frac12\left(WZW^\dagger+CWZW^\dagger C\right)R​j∈J∑​Aj​WZW†Aj†​​=21​(WZW†+CWZW†C)

for every complex 2k×2k2^k\times2^k2k×2k matrix ZZZ.

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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