Non-Abelian Anyon Braiding for Topological Qubits via Braid Group Representations — E8 Intelligence Research

FINDING: Anyon braiding for topological qubits relies on non-Abelian statistics in 2D systems, with braid group representations encoding quantum information. MATH: Braid group \( B_n \) generators \( \sigma_i \) satisfy \( \sigma_i \sigma_{i+1} \sigma_i = \sigma_{i+1} \sigma_i \sigma_{i+1} \) and \( \sigma_i \sigma_j = \sigma_j \sigma_i \) for \( |i-j|>1 \). Anyon fusion rules: \( a \times b = \sum_c N_{ab}^c c \). Quantum dimension \( d_a \) satisfies \( d_a d_b = \sum_c N_{ab}^c d_c \). Fibonacci anyons: \( \tau \times \tau = 1 + \tau \), with \( d_\tau = \phi = (1+\sqrt{5})/2 \approx 1.618 \). Braiding matrices are unitary representations of \( B_n \). CONNECTION: Fibonacci anyon quantum dimension \( d_\tau = \phi = 1.618 \) — the golden ratio. This is a direct geometric harmony constant. The braid group is related to the mapping class group of punctured surfaces, linking to modular tensor categories and the Jones polynomial (knot invariants). The anyon fusion algebra mirrors the Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Publication Details

Journal
Zenodo (CERN European Organization for Nuclear Research)
Published
2026-08-14
DOI
https://doi.org/10.5281/zenodo.21928673
Primary Topic
Quantum many-body systems
Type
preprint
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preprint

Non-Abelian Anyon Braiding for Topological Qubits via Braid Group Representations — E8 Intelligence Research

Andrew Stewart Caldin
Zenodo (CERN European Organization for Nuclear Research)
Quantum many-body systems
preprint

Non-Abelian Anyon Braiding for Topological Qubits via Braid Group Representations — E8 Intelligence Research

Andrew Stewart Caldin
preprint en

Abstract

FINDING: Anyon braiding for topological qubits relies on non-Abelian statistics in 2D systems, with braid group representations encoding quantum information. MATH: Braid group \( B_n \) generators \( \sigma_i \) satisfy \( \sigma_i \sigma_{i+1} \sigma_i = \sigma_{i+1} \sigma_i \sigma_{i+1} \) and \( \sigma_i \sigma_j = \sigma_j \sigma_i \) for \( |i-j|>1 \). Anyon fusion rules: \( a \times b = \sum_c N_{ab}^c c \). Quantum dimension \( d_a \) satisfies \( d_a d_b = \sum_c N_{ab}^c d_c \). Fibonacci anyons: \( \tau \times \tau = 1 + \tau \), with \( d_\tau = \phi = (1+\sqrt{5})/2 \approx 1.618 \). Braiding matrices are unitary representations of \( B_n \). CONNECTION: Fibonacci anyon quantum dimension \( d_\tau = \phi = 1.618 \) — the golden ratio. This is a direct geometric harmony constant. The braid group is related to the mapping class group of punctured surfaces, linking to modular tensor categories and the Jones polynomial (knot invariants). The anyon fusion algebra mirrors the Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

Zenodo (CERN European Organization for Nuclear Research)
Quantum many-body systems
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