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arXiv:2610.37552

Meet-in-the-Middle Compilation of the $[\mathrm{CNOT}]$ Class with Fibonacci Anyons

Matvei Fedin, Andrey Morozov

quant-phhep-thSubmitted Oct 27, 2026• Announced Oct 28, 2026• 0 citations
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Abstract

Compilation of two-qubit Fibonacci anyon gates is complicated by leakage ($\ell$) from the four-dimensional computational sector to the fifth state of the fusion space. We construct a GPU pipeline to find low-leakage representatives of the $[\text{CNOT}]$ class on different subsets of the braid group. We exhaustively explore the full positive five-generator alphabet up to $L=21$ with minimal leakage $\ell\sim10^{-3}$ and error $d_{[\text{CNOT}]}\sim 10^{-8}$ on it. To reach larger lengths, the search space is successively narrowed to three-generator, boundary-$σ_3$, and palindromic braids, and by considering only the Garside left normal form. These optimizations allow us to reach $L=72$. For $L=69$, a braid with $\ell\sim10^{-10}$ and $d_{[\text{CNOT}]}\sim 10^{-10}$ is found. In addition to directly enumerating optimal braids, we proved that $\ell\in\mathbb Z[\varphi]$, and any nonzero leakage obeys an exponential lower bound in the braid length, and obtained the limit laws $F_{3,\infty}(\ell)=\ell^2$ and $F_{5,\infty}(\ell)=\ell^4$ for our sets. Using asymptotics for the distribution function $F$, we showed that for sufficiently long braids, the asymptotics of exhaustive search are better than the asymptotics of random sampling for finding low-leakage braids.

AI Summary

The paper studies compilation of two-qubit gates locally equivalent to CNOT in the six-Fibonacci-anyon encoding, where a fifth fusion-space state causes leakage. It searches positive braid words, optimizing leakage $\ell=1-|U_{00}|^2$ together with a Makhlin-invariant deviation $d_{[\mathrm{CNOT}]}$. A GPU pipeline splits words into halves and evaluates the leakage-determining amplitude using batched row–column products; full computational blocks and invariants are reconstructed only for filtered candidates. This retains exponential enumeration time rather than providing a collision-based meet-in-the-middle speedup. Full five-generator enumeration reaches $L=21$, yielding $\ell=3.946\times10^{-3}$ and $d=7.779\times10^{-9}$ for the composite-score optimum. Successively restricting to three generators, fixed boundary generators, and palindromes, then removing duplicate halves using Garside normal forms, extends searches to $L=72$. At $L=69$, a candidate has $\ell=8.784\times10^{-11}$ and $d=4.26\times10^{-10}$; candidate leakage values are verified algebraically. The paper proves $\ell\in\mathbb Z[\varphi]$ and, for nonzero leakage at length $L$, $\ell\ge(1+C^{2L})^{-1}$ with $C\approx2.8901$. Projective braid-image density, compact-group random-walk convergence, and Haar matrix-element statistics establish fixed-threshold limiting leakage CDFs $F_{3,\infty}(\ell)=\ell^2$ and $F_{5,\infty}(\ell)=\ell^4$. Optimality claims apply only within the specified search families and objectives; alphabet and palindrome restrictions are empirically motivated, not proved lossless. The claimed asymptotic advantage over random sampling additionally uses an empirical record-leakage scaling and lacks mixing estimates for jointly increasing length and decreasing threshold. Exactly leakage-free entangling braids remain unresolved.

Little sign of AI-generated textIncrementalOverclaimsPossible error

Central claim may not hold: The abstract describes the L=21 result as minimum leakage, although the reported exhaustive-search guarantee concerns the composite objective d+4ℓ rather than leakage under a specified CNOT-class tolerance. The claimed asymptotic exhaustive-search advantage relies on extrapolating an empirical leakage-versus-length fit without proving its asymptotic validity. The sampling comparison incorrectly applies fixed-threshold Haar convergence to exponentially shrinking thresholds, where the finite-length probability of zero-leakage words already contradicts the assumed leakage-only sampling scaling.

Written by gpt-6.1-sol from the paper's full text. Automated: it can be wrong.

Comments
30 pages, 5 figures

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Meet-in-the-Middle Compilation of the [CNOT][\mathrm{CNOT}][CNOT] Class with Fibonacci Anyons
Compilation of two-qubit Fibonacci anyon gates is complicated by leakage (ℓ\ellℓ) from the four-dimensional computational sector to the fifth state of the fusion space. We construct a GPU pipeline to find low-leakage representatives of the [CNOT][\text{CNOT}][CNOT] class on different subsets of the braid group.
We exhaustively explore the full positive five-generator alphabet up to L=21L=21L=21 with minimal leakage ℓ∼10−3\ell\sim10^{-3}ℓ∼10−3 and error d[CNOT]∼10−8d_{[\text{CNOT}]}\sim 10^{-8}d[CNOT]​∼10−8 on it. To reach larger lengths, the search space is successively narrowed to three-generator, boundary-σ3σ_3σ3​, and palindromic braids, and by considering only the Garside left normal form. These optimizations allow us to reach L=72L=72L=72. For L=69L=69L=69, a braid with ℓ∼10−10\ell\sim10^{-10}ℓ∼10−10 and d[CNOT]∼10−10d_{[\text{CNOT}]}\sim 10^{-10}d[CNOT]​∼10−10 is found.
In addition to directly enumerating optimal braids, we proved that ℓ∈Z[φ]\ell\in\mathbb Z[\varphi]ℓ∈Z[φ], and any nonzero leakage obeys an exponential lower bound in the braid length, and obtained the limit laws F3,∞(ℓ)=ℓ2F_{3,\infty}(\ell)=\ell^2F3,∞​(ℓ)=ℓ2 and F5,∞(ℓ)=ℓ4F_{5,\infty}(\ell)=\ell^4F5,∞​(ℓ)=ℓ4 for our sets. Using asymptotics for the distribution function FFF, we showed that for sufficiently long braids, the asymptotics of exhaustive search are better than the asymptotics of random sampling for finding low-leakage braids.
The paper studies compilation of two-qubit gates locally equivalent to CNOT in the six-Fibonacci-anyon encoding, where a fifth fusion-space state causes leakage. It searches positive braid words, optimizing leakage ℓ=1−∣U00∣2\ell=1-|U_{00}|^2ℓ=1−∣U00​∣2 together with a Makhlin-invariant deviation d[CNOT]d_{[\mathrm{CNOT}]}d[CNOT]​.
A GPU pipeline splits words into halves and evaluates the leakage-determining amplitude using batched row–column products; full computational blocks and invariants are reconstructed only for filtered candidates. This retains exponential enumeration time rather than providing a collision-based meet-in-the-middle speedup. Full five-generator enumeration reaches L=21L=21L=21, yielding ℓ=3.946×10−3\ell=3.946\times10^{-3}ℓ=3.946×10−3 and d=7.779×10−9d=7.779\times10^{-9}d=7.779×10−9 for the composite-score optimum. Successively restricting to three generators, fixed boundary generators, and palindromes, then removing duplicate halves using Garside normal forms, extends searches to L=72L=72L=72. At L=69L=69L=69, a candidate has ℓ=8.784×10−11\ell=8.784\times10^{-11}ℓ=8.784×10−11 and d=4.26×10−10d=4.26\times10^{-10}d=4.26×10−10; candidate leakage values are verified algebraically.
The paper proves ℓ∈Z[φ]\ell\in\mathbb Z[\varphi]ℓ∈Z[φ] and, for nonzero leakage at length LLL, ℓ≥(1+C2L)−1\ell\ge(1+C^{2L})^{-1}ℓ≥(1+C2L)−1 with C≈2.8901C\approx2.8901C≈2.8901. Projective braid-image density, compact-group random-walk convergence, and Haar matrix-element statistics establish fixed-threshold limiting leakage CDFs F3,∞(ℓ)=ℓ2F_{3,\infty}(\ell)=\ell^2F3,∞​(ℓ)=ℓ2 and F5,∞(ℓ)=ℓ4F_{5,\infty}(\ell)=\ell^4F5,∞​(ℓ)=ℓ4.
Optimality claims apply only within the specified search families and objectives; alphabet and palindrome restrictions are empirically motivated, not proved lossless. The claimed asymptotic advantage over random sampling additionally uses an empirical record-leakage scaling and lacks mixing estimates for jointly increasing length and decreasing threshold. Exactly leakage-free entangling braids remain unresolved.
We investigate the topological quantum compilation of two-qubit operations within a system of Fibonacci anyons. Our primary goal is to generate gates that are approximately leakage-free and equivalent to the controlled-not (cnot) gate up to single-qubit operations. These gates belong to the local equivalence class [cnot]. Additionally, we explore which local equivalence classes of two-qubit operations can be naturally generated by braiding Fibonacci anyons. We discovered that most of the generated classes are located near the edges of the Weyl chamber representation of two-qubit gates, specifically between the local equivalence classes of the identity [1][\mathbb{1}][1] and [cnot], swap and between those of the double-controlled-not [dcnot] and [swap]. Furthermore, we found a numerically exact implementation of a local equivalent of the swap gate using a sequence of only nine elements from the Fibonacci braiding gate set.
We discuss how to significantly reduce leakage errors in topological quantum computation by introducing an irrelevant error in phase, using the construction of a controlled-NOT (CNOT) gate in the Fibonacci anyon model as a concrete example. To be specific, we construct a functional braid in a six-anyon Hilbert space that exchanges two neighboring anyons while conserving the encoded quantum information. The leakage error is $\ensuremath{\sim}{10}^{\ensuremath{-}10}$ for a braid of $\ensuremath{\sim}100$ interchanges of anyons. Applying the braid greatly reduces the leakage error in the construction of generic controlled-rotation gates.
Topological quantum computing holding global anti-interference ability is realized by braiding some anyons, such as well-known Fibonacci anyons. Here, based on $SO(3)_2 $ theory we obtain a total of 6 anyon models utilizing \textit{F}-matrices, \textit{R}-symbols, and fusion rules of metaplectic anyon.We obtain the elementary braiding matrices (EBMs) by means of unconventional encoding. After braiding \textit{X} and X′X^\primeX′, we insert a pair of \textit{Z} anyons into them to ensure that the initial order of anyons remains unchanged. In this process only fusion is required, and measurement is not necessary. Three of them {V3113,V3131,V1133}\{V^{113}_3,V^{131}_3,V^{133}_1\}{V3113​,V3131​,V1133​} are studied in detail. We study systematically the compilation of these three models through EBMs obtained analytically. For one-qubit case, the classical \textit{H}- and \textit{T}-gate can be well constructed using the genetic algorithm enhanced Solovay-Kitaev algorithm (GA-enhanced SKA) by {V3113,V3131,V1133}\{V^{113}_3,V^{131}_3,V^{133}_1\}{V3113​,V3131​,V1133​}. The obtained accuracy of the \textit{H}/\textit{T}-gate by {V3113,V1133}\{V^{113}_3,V^{133}_1\}{V3113​,V1133​} is slightly inferior to the corresponding gates of the Fibonacci anyon model, but it also can meet the requirements of fault-tolerant quantum computing, V3131V^{131}_3V3131​ giving the best performance of these four models. For the two-qubit case, we use the exhaustive method for short lengths and the GA for long lengths to obtain braidword for {V3113,V3131,V1133}\{V^{113}_3,V^{131}_3,V^{133}_1\}{V3113​,V3131​,V1133​} models. The resulting matrices can well approximate the local equivalence class of the CNOT-gate, while demonstrating a much smaller error than the Fibonacci model, especially for the V3113V^{113}_3V3113​.The braiding processes of conventional encoding (using identical anyons) and unconventional encoding (using distinct anyons) are compared. Finally, we attempt to generalize the model to the \textit{N}-qubit case.
Abstract Topological quantum computation is an implementation of a quantum computer in a way that radically reduces decoherence. Topological qubits are encoded in the topological evolution of two-dimensional quasi-particles called anyons and universal set of quantum gates can be constructed by braiding these anyons yielding to a topologically protected circuit model. In the present study we remind the basics of this emerging quantum computation scheme and illustrate how a topological qubit built with three Fibonacci anyons might be adopted to achieve leakage free braiding gate by exchanging the anyons composing it. A single-qubit braiding gate that approximates the Hadamard quantum gate to a certain accuracy is numerically implemented using a brute force search method. The algorithms utilized for that purpose are explained and the numerical programs are publicly shared for reproduction and further use.
We address the problem of compiling quantum operations into braid representations for non-Abelian quasiparticles described by the Fibonacci anyon model. We classify the single-qubit unitaries that can be represented exactly by Fibonacci anyon braids and use the classification to develop a probabilistically polynomial algorithm that approximates any given single-qubit unitary to a desired precision by an asymptotically depth-optimal braid pattern. We extend our algorithm in two directions: to produce braids that allow only single-strand movement, called weaves, and to produce depth-optimal approximations of two-qubit gates. Our compiled braid patterns have depths that are 20 to 1000 times shorter than those output by prior state-of-the-art methods, for precisions ranging between 10(-10) and 10(-30).
FINDING: Topological quantum computation via non-Abelian anyon braiding, specifically Fibonacci anyons, encodes qubits in degenerate state spaces where braid operations generate the Fibonacci fusion rules and yield universal quantum gates. | MATH: Fibonacci anyon fusion rule: τ ⊗ τ = 1 ⊕ τ (golden anyon). Dimension of Hilbert space for n anyons grows as Fibonacci numbers: dim(H_n) = F_{n-1} (with F_0=0, F_1=1). Braid generators σ_i satisfy Yang-Baxter: σ_i σ_{i+1} σ_i = σ_{i+1} σ_i σ_{i+1}, and σ_i σ_j = σ_j σ_i for |i-j|≥2. Single-qubit braiding gates compiled via brute-force optimization (arXiv:2008.03542) — the key constant is the golden ratio φ = (1+√5)/2 ≈ 1.618, which appears as the quantum dimension d_τ = φ. | CONNECTION: Direct geometric harmony: Fibonacci anyons have quantum dimension exactly φ = 1.618 (and its inverse 0.618 = 1/φ). The fusion space dimension sequence (1,1,2,3,5,8,...) is the Fibonacci sequence — the same ratio governing pentagonal symmetry (5-fold crystallogr Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com