How statement and proof provenance work
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These labels describe origin, not correctness: citations and verification chips remain separate evidence.
B6 exact rank certificates and encoded leakage budget
Example
The exact B6 certificates have determinants and modulo for the selected and Lie-word minors. In the total-charge- six-anyon space there are two natural four-dimensional code choices: a pair-charge code and the triple code of Six-anyon triple-encoded subspace and leakage complement. The density argument applies to either chosen subspace; the two definitions use different fusion trees, and no equality of their projectors is asserted. For a circuit with ideal one-qubit or adjacent two-qubit gates, assigning gives total logical block error and leakage at most .
Facts & Assumptions
Given: The fixed Fibonacci fusion rule, the pair and triple fusion trees, the exact finite-field certificates, and .
The normalized B6 image in has closure containing , and the image in has closure containing . Exact five-dimensional Fibonacci B6 density Exact eight-dimensional Fibonacci B6 density
The simultaneous B6 closure contains . Joint SU(5)×SU(8) closure from B6 path blocks
Per-gate full-space errors add; exact logical-block equality for an ambient unitary forces zero leakage. Logical error and leakage add under code-preserving gate approximation Exact logical-block correctness forces zero leakage
Reduction of coefficients through the stated specialization sends a zero algebraic determinant to zero. Fibonacci coefficient ring and its exact mod-31 specialization
The six-anyon triple code has dimension in both total-charge blocks; in total charge , the ambient dimension is . Six-anyon triple-encoded subspace and leakage complement
Every admissible fusion tree has its orthonormal path basis, and a unitary associator composite changes between the pair, triple, and left-associated trees. Multiplicity-aware fusion-tree basis Fusion-tree basis and dimension recursion Unitary fusion category Gauge covariance of fusion-space braid actions
A full-space approximation by to a code-preserving unitary target bounds both logical block error and leakage by . Block-target approximation bounds logical error and leakage
The categorical braid is the normalized braid multiplied by the same scalar in both total-charge blocks. This phase must be tracked under coherent control. The braid phase is a common scalar character
Assume . The Axiom of Countable Choice ()
Use the Fibonacci fusion rules and the triple-code path convention stated in Six-anyon triple-encoded subspace and leakage complement. The pair-charge code below is a distinct subspace in the same total-charge block; no equality of the two code projectors is assumed.
Verification
In the pairwise tree , let label the charge or of pair , respectively. Fusion to total charge allows exactly the strings For , the intermediate charge after the first two pair outputs is . For , it is uniquely , respectively; each then fuses with the last pair output to total charge . A string with exactly one has total charge and is inadmissible. Thus the four even strings span a four-dimensional pair-charge code , and the all- string spans its one-dimensional complement. Fix a unitary associator composite from to the left-associated B6 tree. The triple code in [F6] is transported to that same tree by its own fixed associator composite. Both are four-dimensional subspaces of the five-dimensional total-charge- fusion space. The argument below treats them as independent code choices and makes no projector-equality claim.
Let be any four-dimensional subspace of the five-dimensional total-charge- fusion space, including either or , and let . Its orthogonal complement is one-dimensional. Define on ; this is unitary with determinant one, so . By [F1], every operator-norm neighborhood of contains a normalized B6 word. Applying [F8] to a word within of gives logical block error and leakage at most for the selected code. Therefore the pair-charge and triple codes each admit the same density guarantee without identifying their subspaces.
The five-dimensional certificate runs research/scaffold-audit-2026-10-16/topological-quantum-computing/b6-lie-rank-certificate.py and returns the exact minor determinant in . The eight-dimensional deterministic selection runs research/scaffold-audit-2026-10-16/topological-quantum-computing/b6-su8-lie-rank-certificate.py and returns determinant . Both scripts use integer arithmetic only; [F4] proves that these nonzero reductions imply nonzero exact complex determinants.
Fix either selected charge- code or . For use the ordered transported even paths of step 1.1 as the computational basis; for use the ordered triple paths in [F6]. In the charge- block use the triple code with its ordered basis from [F6]. Each code is thereby identified with . Write each ideal circuit gate as : a one-qubit gate A is or , and an adjacent two-qubit gate is its full matrix. In each sector take the orthonormal complementary paths in the corresponding grouped fusion tree and transport them by the same unitary associator. These complements have dimensions and . With , define ambient code-preserving targets, in these code/complement coordinates, by Each complement action is unitary because , and . Transporting these targets to the fixed left-associated ambient bases preserves determinant and norm. Thus they are actual elements of and and preserve the selected code in each sector. For the pair-charge choice, the charge- target just uses the separately specified triple code; no equality of pair and triple projectors is used.
Let , take target accuracy , and set for . The product of the open operator-norm -balls around meets the normalized simultaneous B6 image by [F2]. Choose one word in this product, giving These are ambient bounds on the entire five- and eight-dimensional sectors for every gate, including the one-qubit factors. The choices for the two sectors are the same braid word.
For either , the normalized ambient matrices and the code-preserving ideal matrices satisfy every hypothesis of [F3] by step 2.1, step 3.1. Its finite telescoping estimate therefore gives The ideal product restricts to on the selected code. Apply [F8] to this ambient bound: total logical block error and leakage are both at most . For a concrete distinction between these measurements, take , code , target , and The compressed block is , so its logical error is , while the leakage amplitude is . It has the correct one-dimensional logical direction with reduced amplitude, not an exactly correct block. Conversely, exact block equality forces zero leakage by [F3].
The bounds in step 4.1 concern normalized braid matrices, or equivalently categorical matrices compared to targets with the common phase matched. By [F9], the concatenated categorical braid has the common factor in both sectors. Multiplication by that unit scalar leaves leakage unchanged and yields the corresponding single projective logical phase; it cannot be independently discarded in different sectors or under coherent control. This existence proof assigns no braid-length, search-time or physical-preparation bound.
Depends on
- Exact five-dimensional Fibonacci B6 density
- Exact eight-dimensional Fibonacci B6 density
- Joint SU(5)×SU(8) closure from B6 path blocks
- The braid phase is a common scalar character
- Fibonacci B6 approximates one logical two-qubit gate in both charge blocks
- Logical error and leakage add under code-preserving gate approximation
- Exact logical-block correctness forces zero leakage
- Fibonacci single-qubit projective density
- Six-anyon triple-encoded subspace and leakage complement
- Multiplicity-aware fusion-tree basis
- Fusion-tree basis and dimension recursion
- Unitary fusion category
- Gauge covariance of fusion-space braid actions
- Block-target approximation bounds logical error and leakage
- Fibonacci coefficient ring and its exact mod-31 specialization
- The Axiom of Countable Choice ($\mathrm{AC}_\omega$)
Used by
Nothing in the library uses this result yet.
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Sources
- Michael H. Freedman, Michael J. Larsen, and Zhenghan Wang, A Modular Functor Which Is Universal for Quantum Computation (standard reference, not scraped)
- Chetan Nayak, Steven H. Simon, Ady Stern, Michael Freedman, and Sankar Das Sarma, Non-Abelian Anyons and Topological Quantum Computation (standard reference, not scraped)
- Ronald de Wolf, Quantum Computing: Lecture Notes (standard reference, not scraped)