Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Six Majorana Zero Modes Braid into a Three-Qubit Clifford Group — E8 Intelligence Research

Andrew Stewart Caldin

Published Oct 30, 2026• 0 citations
Publisher

Abstract

FINDING: Six Majorana zero modes (MZMs) form three qubit pairs whose braiding generates a finite Clifford-group representation — the minimal non-Abelian platform for universal-adjacent topological quantum computation. | MATH: 2n MZMs → n qubits; 6 MZMs → 3 qubits → Hilbert space dim 2³ = 8. Braid group B₆ (or its image) maps to Clifford group C₃ ⊂ U(8). Ising anyon σ braiding: γᵢ → γⱼ, γⱼ → −γᵢ (i≠j), γₖ → γₖ. Majorana algebra {γᵢ,γⱼ} = 2δᵢⱼ. Fusion: σ×σ = 1 + ψ. Braid generator eigenvalues e^{±iπ/8} (topological phase, related to ν=5/2). | CONNECTION: Clifford group order for n qubits = 2^{n²+2n}·∏(4ᵏ−1); for n=3: 2^{15}·(4−1)(16−1)(64−1) = 32768·3·15·63 = 92,897,280. Braid group B₆ has 6 generators σ₁…σ₅ with relations σᵢσᵢ₊₁σᵢ = σᵢ₊₁σᵢσᵢ₊₁ (Yang–Baxter / braid relation) — a cubic algebraic relation, echoing the 3-fold symmetry of A₂ root system and the 2π/3 rotation in SU(3). The 6 MZMs sit at vertices of an octahedron (6 vertices, 8 faces = 2³ Hilbert states); braiding = SO(6) rota Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

DOI
10.5281/zenodo.23796671

Related papers

Spin(6)≅SU(4) Links 6 Majorana Modes to Clifford Universality — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Spin(6)≅SU(4) is the Lie-algebraic backbone linking 6 Majorana zero modes to Clifford gate universality via SO(6) vector representation and su(4) Cartan decomposition | MATH: Spin(6)≅SU(4), rank 3; 6 MZMs ↔ 6 generators of SO(6) vector rep; su(4) has dim 15 = 6 (Cartan/complex) + 9 (non-Cartan); Cartan subalgebra dim = rank = 3; Clifford group over n qubits ↔ symplectic group Sp(2n, F₂), order 2^(n²+2n)∏(2^(2k)−1) | CONNECTION: su(4)≅so(6) root system A₃; 6 roots = 6 MZMs; Weyl group S₄ order 24 = 4!; crystallographic A₃ lattice (fcc-derived); 6 = 2×3, base-60 divisibility; braiding phases e^(iπ/4) = √2/2 ≈ 0.707 (near 0.786 within Fibonacci anyon error) | DEPTH: 8 FINDING: Braiding MZMs in spin space (worldribbon) realizes non-Abelian statistics without spatial transport — adiabatic spin reversal generates the braid | MATH: Braid operator B_ij = exp(π γ_i γ_j /4); γ_i γ_j = −γ_j γ_i (Clifford algebra Cl(0,6)); spin reversal = SO(6) rotation by π; two MZMs → SU(2) subspace; b Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Oct 30, 2026•0 citations

Majorana 1's Ising Anyons: Clifford-Only Braiding, Magic States Needed — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Microsoft's Majorana 1 chip claims topological qubits using Majorana zero modes, but the mathematical core is the non-Abelian braiding statistics of Ising anyons — not yet peer-verified; the arXiv paper is a software framework, not the hardware breakthrough. | MATH: Ising anyon braid group yields Clifford gates only (not universal); to reach universality, one must inject a non-Clifford gate (e.g., π/8 phase) via magic state distillation — requiring ratios of rotation angles: π/4, π/8, π/16. The topological protection relies on the fusion rules: σ × σ = 1 + ψ (where σ = Majorana, ψ = fermion), and the braid matrix eigenvalues are e^{±iπ/8} — note the 1/8 fractional phase, which is *not* a golden-ratio harmonic but a root-of-unity order 16. The qubit encoding uses parity: two Majoranas form a fermion with occupation 0 or 1, giving the computational basis. | CONNECTION: The braid group B_n acts on the Ising anyon Hilbert space of dimension 2^{(n-1)/2}; this is deeply tied to the Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Oct 25, 2026•0 citations

Topological Qubits via Non-Abelian Anyons: Majorana Braiding and Microsoft's Majorana 1 — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Topological quantum computing leverages non-Abelian anyons (Majorana zero modes) for fault-tolerant braiding operations, with Microsoft's Majorana 1 chip claiming topological qubit hardware. | MATH: Braid group B_n generators σ_i satisfy σ_i σ_{i+1} σ_i = σ_{i+1} σ_i σ_{i+1} (Yang–Baxter); Majorana operators γ_i obey {γ_i, γ_j} = 2δ_ij; topological qubit encoded in parity iγ_1γ_2 = ±1; non-Abelian anyon exchange yields unitary matrices U(σ_i) = exp(θ σ_i) with θ = π/4 for Ising anyons (Fibonacci anyons: θ = 2π/5). | CONNECTION: Braid group relations are the algebraic shadow of the Yang–Baxter equation — the same structure underlying 2D crystallographic root systems (A_n, B_n, D_n) and the golden ratio appears in Fibonacci anyons: quantum dimension φ = (1+√5)/2 ≈ 1.618, with fusion rules τ⊗τ = 1⊕τ giving dimension φ² = φ+1. | DEPTH: 8 --- **Detailed analysis:** 1. **Key mathematical insight:** The core discovery is that topological phases of matter host quasiparticles (anyon Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Aug 24, 2026•0 citations

Topological Qubits via Non-Abelian Anyons: Braid Group and Majorana Modes — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Topological quantum computing leverages non-Abelian anyons (Majorana zero modes) for fault-tolerant braiding operations, with Microsoft's Majorana 1 chip claiming topological qubit hardware. | MATH: Braid group B_n generators σ_i satisfy 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; non-Abelian anyons yield unitary representations U(σ_i) with U(σ_i)U(σ_{i+1})U(σ_i) ≠ U(σ_{i+1})U(σ_i)U(σ_{i+1}); Majorana zero modes obey γ_i† = γ_i, {γ_i, γ_j} = 2δ_ij; topological qubit encoded in parity (−1)^{n} = i^{2n} γ_1 γ_2 … γ_{2n}; Fibonacci anyons have quantum dimension φ = (1+√5)/2 ≈ 1.618, fusion rules τ×τ = 1 + τ. | CONNECTION: Fibonacci anyons directly encode the golden ratio φ in their quantum dimension — braiding statistics are governed by the golden ratio; the braid group B_n is isomorphic to the mapping class group of the punctured disk, whose moduli space relates to the modular group PSL(2,ℤ) (base-60 heritage); Majorana zero modes on a 1D nanowire fo Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Sep 4, 2026•0 citations

Topological Quantum Computing: Braid Groups, Majorana Modes, and Microsoft's Majorana 1 Chip — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Topological quantum computing leverages non-Abelian anyons (Majorana zero modes) for fault-tolerant braid-based computation, with Microsoft's Majorana 1 chip claiming hardware realization. | MATH: Braid group B_n generators σ_i satisfy σ_iσ_{i+1}σ_i = σ_{i+1}σ_iσ_{i+1} and σ_iσ_j = σ_jσ_i for |i−j|≥2; Fibonacci anyons yield fusion space dimension φ (golden ratio) via F-matrix with entries involving φ^{-1/2}; Majorana modes obey γ_i†=γ_i, {γ_i,γ_j}=2δ_ij; topological charge conservation enforces fusion rules; Jones polynomial evaluated at q=e^{2πi/5} (or e^{2πi/k} for SU(2)_k Chern-Simons) encodes braid invariants. | CONNECTION: Fibonacci anyon model has quantum dimension d = φ = (1+√5)/2 ≈ 1.618, with F-matrix elements ∝ 1/φ ≈ 0.618; braid group representations correspond to Temperley-Lieb algebra with loop value δ = φ+φ^{-1} = √5 ≈ 2.236; SU(2)_k level k=3 gives φ; crystallographic root system A_2 (hexagonal lattice) underlies SU(3) anyons; base-60 appears in modular data S,T Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Sep 10, 2026•0 citations

Microsoft's Majorana 1: Topological Qubit Claims Without Demonstrated Logical Qubits — E8 Intelligence Research

Andrew Stewart Caldin

FINDING: Microsoft's Majorana 1 claims a topological qubit platform based on Majorana zero modes (MZMs) in InAs/Al heterostructures — a materials/physics claim, not yet a demonstrated logical qubit. | MATH: MZM operators satisfy γ_i = γ_i† and {γ_i, γ_j} = 2δ_ij (Clifford algebra Cl(R^n)); braiding implements non-Abelian SU(2) transformations via R = exp(iπ/4 · γ_iγ_j). Topological protection gap Δ ~ 1 K scale; error suppression scales as exp(−Δ/k_BT). | CONNECTION: Braiding group B_n (Artin braid group) maps to Clifford/Pauli group; Fibonacci anyons would yield golden-ratio quantum dimensions d = φ = 1.618 (not claimed here — Majorana/Ising anyons have d = √2). | DEPTH: 6 FINDING: Topological quantum computing's core promise is error suppression by topology, not redundancy — the "unbreakable" framing. | MATH: Degeneracy of 2n MZMs = 2^(n−1); ground-state manifold dimension = 2^(n−1). Braiding = unitary rep of B_n; Ising anyons generate only Clifford gates (need magic-state injection Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

•Oct 27, 2026•0 citations
FINDING: Six Majorana zero modes (MZMs) form three qubit pairs whose braiding generates a finite Clifford-group representation — the minimal non-Abelian platform for universal-adjacent topological quantum computation. | MATH: 2n MZMs → n qubits; 6 MZMs → 3 qubits → Hilbert space dim 2³ = 8. Braid group B₆ (or its image) maps to Clifford group C₃ ⊂ U(8). Ising anyon σ braiding: γᵢ → γⱼ, γⱼ → −γᵢ (i≠j), γₖ → γₖ. Majorana algebra {γᵢ,γⱼ} = 2δᵢⱼ. Fusion: σ×σ = 1 + ψ. Braid generator eigenvalues e^{±iπ/8} (topological phase, related to ν=5/2). | CONNECTION: Clifford group order for n qubits = 2^{n²+2n}·∏(4ᵏ−1); for n=3: 2^{15}·(4−1)(16−1)(64−1) = 32768·3·15·63 = 92,897,280. Braid group B₆ has 6 generators σ₁…σ₅ with relations σᵢσᵢ₊₁σᵢ = σᵢ₊₁σᵢσᵢ₊₁ (Yang–Baxter / braid relation) — a cubic algebraic relation, echoing the 3-fold symmetry of A₂ root system and the 2π/3 rotation in SU(3). The 6 MZMs sit at vertices of an octahedron (6 vertices, 8 faces = 2³ Hilbert states); braiding = SO(6) rota Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Spin(6)≅SU(4) is the Lie-algebraic backbone linking 6 Majorana zero modes to Clifford gate universality via SO(6) vector representation and su(4) Cartan decomposition | MATH: Spin(6)≅SU(4), rank 3; 6 MZMs ↔ 6 generators of SO(6) vector rep; su(4) has dim 15 = 6 (Cartan/complex) + 9 (non-Cartan); Cartan subalgebra dim = rank = 3; Clifford group over n qubits ↔ symplectic group Sp(2n, F₂), order 2^(n²+2n)∏(2^(2k)−1) | CONNECTION: su(4)≅so(6) root system A₃; 6 roots = 6 MZMs; Weyl group S₄ order 24 = 4!; crystallographic A₃ lattice (fcc-derived); 6 = 2×3, base-60 divisibility; braiding phases e^(iπ/4) = √2/2 ≈ 0.707 (near 0.786 within Fibonacci anyon error) | DEPTH: 8 FINDING: Braiding MZMs in spin space (worldribbon) realizes non-Abelian statistics without spatial transport — adiabatic spin reversal generates the braid | MATH: Braid operator B_ij = exp(π γ_i γ_j /4); γ_i γ_j = −γ_j γ_i (Clifford algebra Cl(0,6)); spin reversal = SO(6) rotation by π; two MZMs → SU(2) subspace; b Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Microsoft's Majorana 1 chip claims topological qubits using Majorana zero modes, but the mathematical core is the non-Abelian braiding statistics of Ising anyons — not yet peer-verified; the arXiv paper is a software framework, not the hardware breakthrough. | MATH: Ising anyon braid group yields Clifford gates only (not universal); to reach universality, one must inject a non-Clifford gate (e.g., π/8 phase) via magic state distillation — requiring ratios of rotation angles: π/4, π/8, π/16. The topological protection relies on the fusion rules: σ × σ = 1 + ψ (where σ = Majorana, ψ = fermion), and the braid matrix eigenvalues are e^{±iπ/8} — note the 1/8 fractional phase, which is *not* a golden-ratio harmonic but a root-of-unity order 16. The qubit encoding uses parity: two Majoranas form a fermion with occupation 0 or 1, giving the computational basis. | CONNECTION: The braid group B_n acts on the Ising anyon Hilbert space of dimension 2^{(n-1)/2}; this is deeply tied to the Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Topological quantum computing leverages non-Abelian anyons (Majorana zero modes) for fault-tolerant braiding operations, with Microsoft's Majorana 1 chip claiming topological qubit hardware. | MATH: Braid group B_n generators σ_i satisfy σ_i σ_{i+1} σ_i = σ_{i+1} σ_i σ_{i+1} (Yang–Baxter); Majorana operators γ_i obey {γ_i, γ_j} = 2δ_ij; topological qubit encoded in parity iγ_1γ_2 = ±1; non-Abelian anyon exchange yields unitary matrices U(σ_i) = exp(θ σ_i) with θ = π/4 for Ising anyons (Fibonacci anyons: θ = 2π/5). | CONNECTION: Braid group relations are the algebraic shadow of the Yang–Baxter equation — the same structure underlying 2D crystallographic root systems (A_n, B_n, D_n) and the golden ratio appears in Fibonacci anyons: quantum dimension φ = (1+√5)/2 ≈ 1.618, with fusion rules τ⊗τ = 1⊕τ giving dimension φ² = φ+1. | DEPTH: 8 --- **Detailed analysis:** 1. **Key mathematical insight:** The core discovery is that topological phases of matter host quasiparticles (anyon Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Topological quantum computing leverages non-Abelian anyons (Majorana zero modes) for fault-tolerant braiding operations, with Microsoft's Majorana 1 chip claiming topological qubit hardware. | MATH: Braid group B_n generators σ_i satisfy 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; non-Abelian anyons yield unitary representations U(σ_i) with U(σ_i)U(σ_{i+1})U(σ_i) ≠ U(σ_{i+1})U(σ_i)U(σ_{i+1}); Majorana zero modes obey γ_i† = γ_i, {γ_i, γ_j} = 2δ_ij; topological qubit encoded in parity (−1)^{n} = i^{2n} γ_1 γ_2 … γ_{2n}; Fibonacci anyons have quantum dimension φ = (1+√5)/2 ≈ 1.618, fusion rules τ×τ = 1 + τ. | CONNECTION: Fibonacci anyons directly encode the golden ratio φ in their quantum dimension — braiding statistics are governed by the golden ratio; the braid group B_n is isomorphic to the mapping class group of the punctured disk, whose moduli space relates to the modular group PSL(2,ℤ) (base-60 heritage); Majorana zero modes on a 1D nanowire fo Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Topological quantum computing leverages non-Abelian anyons (Majorana zero modes) for fault-tolerant braid-based computation, with Microsoft's Majorana 1 chip claiming hardware realization. | MATH: Braid group B_n generators σ_i satisfy σ_iσ_{i+1}σ_i = σ_{i+1}σ_iσ_{i+1} and σ_iσ_j = σ_jσ_i for |i−j|≥2; Fibonacci anyons yield fusion space dimension φ (golden ratio) via F-matrix with entries involving φ^{-1/2}; Majorana modes obey γ_i†=γ_i, {γ_i,γ_j}=2δ_ij; topological charge conservation enforces fusion rules; Jones polynomial evaluated at q=e^{2πi/5} (or e^{2πi/k} for SU(2)_k Chern-Simons) encodes braid invariants. | CONNECTION: Fibonacci anyon model has quantum dimension d = φ = (1+√5)/2 ≈ 1.618, with F-matrix elements ∝ 1/φ ≈ 0.618; braid group representations correspond to Temperley-Lieb algebra with loop value δ = φ+φ^{-1} = √5 ≈ 2.236; SU(2)_k level k=3 gives φ; crystallographic root system A_2 (hexagonal lattice) underlies SU(3) anyons; base-60 appears in modular data S,T Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
FINDING: Microsoft's Majorana 1 claims a topological qubit platform based on Majorana zero modes (MZMs) in InAs/Al heterostructures — a materials/physics claim, not yet a demonstrated logical qubit. | MATH: MZM operators satisfy γ_i = γ_i† and {γ_i, γ_j} = 2δ_ij (Clifford algebra Cl(R^n)); braiding implements non-Abelian SU(2) transformations via R = exp(iπ/4 · γ_iγ_j). Topological protection gap Δ ~ 1 K scale; error suppression scales as exp(−Δ/k_BT). | CONNECTION: Braiding group B_n (Artin braid group) maps to Clifford/Pauli group; Fibonacci anyons would yield golden-ratio quantum dimensions d = φ = 1.618 (not claimed here — Majorana/Ising anyons have d = √2). | DEPTH: 6 FINDING: Topological quantum computing's core promise is error suppression by topology, not redundancy — the "unbreakable" framing. | MATH: Degeneracy of 2n MZMs = 2^(n−1); ground-state manifold dimension = 2^(n−1). Braiding = unitary rep of B_n; Ising anyons generate only Clifford gates (need magic-state injection Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com