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arXiv:hep-th/9301100 · Nuclear Physics B

Anyons and quantum groups

Alberto Lerda A, S. Sciuto

Published Jul 1, 1993• 89 citations
arXivHTMLPDF
DOI
10.1016/0550-3213(93)90316-h

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Quantum Mechanics of Anyons

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Fibonacci Anyon Braid Groups Classified by Modular Tensor Categories — E8 Intelligence Research

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FINDING: Fibonacci anyon braid group representations are classified by modular tensor categories (MTCs) with fusion rules derived from the Fibonacci (golden ratio) quantum group \( \text{SU}(2)_3 \), yielding non-Abelian statistics and universal topological quantum computation. MATH: - Fibonacci anyon fusion rule: \( \tau \times \tau = 1 + \tau \) (where \( \tau \) is the non-Abelian anyon, 1 is the vacuum). - Quantum dimension of \( \tau \): \( d_\tau = \phi = (1+\sqrt{5})/2 \approx 1.618 \). - Braid matrix eigenvalues: \( e^{\pm i\pi/5} \) and \( e^{\pm i3\pi/5} \), derived from the \( R \)-matrix of the quantum group \( U_q(\mathfrak{sl}_2) \) at \( q = e^{i\pi/5} \). - Modular \( S \)-matrix for Fibonacci MTC: \[ S = \frac{1}{\sqrt{\phi+2}} \begin{pmatrix} 1 & \phi \\ \phi & -1 \end{pmatrix} \] with \( \phi = 1.618 \). - Central charge \( c = 4/5 \), related to the minimal model \( M(5,4) \) of conformal field theory. CONNECTION: - The golden ratio \( \phi = Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Fibonacci Anyons Enable Universal Quantum Computation via Hexagonal Symmetry — E8 Intelligence Research

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FINDING: Fibonacci anyons realize non-Abelian braiding statistics with quantum dimension φ, enabling universal topological quantum computation via the A₂ root system's hexagonal symmetry. MATH: - Quantum dimension of Fibonacci anyon: \( d = \phi = \frac{1+\sqrt{5}}{2} \approx 1.618 \) - Fusion rule: \( \tau \times \tau = 1 + \tau \) (where τ is the Fibonacci anyon) - Braiding matrices satisfy the Yang–Baxter equation and produce the Fibonacci representation of the braid group \( B_n \) - A₂ root system: 6 roots at 60° angles, hexagonal lattice, Coxeter number 3, Weyl group order 6 CONNECTION: - The quantum dimension φ is exactly the golden ratio, linking anyon statistics to the Fibonacci sequence and pentagonal/quasicrystalline symmetry. - The A₂ root system's hexagonal lattice (crystallographic symmetry) underlies the fusion and braiding structure of Fibonacci anyons; the anyon's fusion algebra corresponds to the representation theory of the quantum group \( U_q(sl_2) Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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Anyons and Deformed Lie Algebras

M. Frau, Alberto Lerda A, S. Sciuto

We discuss the connection between anyons (particles with fractional statistics) and deformed Lie algebras (quantum groups). After a brief review of the main properties of anyons, we present the details of the anyonic realization of all deformed classical Lie algebras in terms of anyonic oscillators. The deformation parameter of the quantum groups is directly related to the statistics parameter of the anyons. Such a realization is a direct generalization of the Schwinger construction in terms of fermions and is based on a sort of bosonization formula which yields the generators of the deformed algebra in terms of the undeformed ones. The entire procedure is well defined on two-dimensional lattices, but it can be consistently reduced also to one-dimensional chains.

arXiv:hep-th/9407161•Jul 25, 1994•2 citations

Physics And Mathematics of Anyons

Shiing-Shen Chern, C. W. Chu, C. S. Ting

•Jun 1, 1991•5 citations
FINDING: Fibonacci anyon braid group representations are classified by modular tensor categories (MTCs) with fusion rules derived from the Fibonacci (golden ratio) quantum group SU(2)3 \text{SU}(2)_3 SU(2)3​, yielding non-Abelian statistics and universal topological quantum computation. MATH: - Fibonacci anyon fusion rule: τ×τ=1+τ \tau \times \tau = 1 + \tau τ×τ=1+τ (where τ \tau τ is the non-Abelian anyon, 1 is the vacuum). - Quantum dimension of τ \tau τ: dτ=ϕ=(1+5)/2≈1.618 d_\tau = \phi = (1+\sqrt{5})/2 \approx 1.618 dτ​=ϕ=(1+5​)/2≈1.618. - Braid matrix eigenvalues: e±iπ/5 e^{\pm i\pi/5} e±iπ/5 and e±i3π/5 e^{\pm i3\pi/5} e±i3π/5, derived from the R R R-matrix of the quantum group Uq(sl2) U_q(\mathfrak{sl}_2) Uq​(sl2​) at q=eiπ/5 q = e^{i\pi/5} q=eiπ/5. - Modular S S S-matrix for Fibonacci MTC: S=1ϕ+2(1ϕϕ−1) S = \frac{1}{\sqrt{\phi+2}} \begin{pmatrix} 1 & \phi \\ \phi & -1 \end{pmatrix} S=ϕ+2​1​(1ϕ​ϕ−1​) with ϕ=1.618 \phi = 1.618 ϕ=1.618. - Central charge c=4/5 c = 4/5 c=4/5, related to the minimal model M(5,4) M(5,4) M(5,4) of conformal field theory. CONNECTION: - The golden ratio \( \phi = Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Fibonacci anyons realize non-Abelian braiding statistics with quantum dimension φ, enabling universal topological quantum computation via the A₂ root system's hexagonal symmetry. MATH: - Quantum dimension of Fibonacci anyon: d=ϕ=1+52≈1.618 d = \phi = \frac{1+\sqrt{5}}{2} \approx 1.618 d=ϕ=21+5​​≈1.618 - Fusion rule: τ×τ=1+τ \tau \times \tau = 1 + \tau τ×τ=1+τ (where τ is the Fibonacci anyon) - Braiding matrices satisfy the Yang–Baxter equation and produce the Fibonacci representation of the braid group Bn B_n Bn​ - A₂ root system: 6 roots at 60° angles, hexagonal lattice, Coxeter number 3, Weyl group order 6 CONNECTION: - The quantum dimension φ is exactly the golden ratio, linking anyon statistics to the Fibonacci sequence and pentagonal/quasicrystalline symmetry. - The A₂ root system's hexagonal lattice (crystallographic symmetry) underlies the fusion and braiding structure of Fibonacci anyons; the anyon's fusion algebra corresponds to the representation theory of the quantum group \( U_q(sl_2) Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
We discuss the connection between anyons (particles with fractional statistics) and deformed Lie algebras (quantum groups). After a brief review of the main properties of anyons, we present the details of the anyonic realization of all deformed classical Lie algebras in terms of anyonic oscillators. The deformation parameter of the quantum groups is directly related to the statistics parameter of the anyons. Such a realization is a direct generalization of the Schwinger construction in terms of fermions and is based on a sort of bosonization formula which yields the generators of the deformed algebra in terms of the undeformed ones. The entire procedure is well defined on two-dimensional lattices, but it can be consistently reduced also to one-dimensional chains.