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arXiv:1210.7929 · Physical Review B

Measurement-only topological quantum computation via tunable interactions

Parsa Bonderson

Published Jan 10, 2013• 61 citations
arXivHTMLPDF

Abstract

I examine, in general, how tunable interactions may be used to perform anyonic teleportation and generate braiding transformations for non-Abelian anyons. I explain how these methods are encompassed by the ``measurement-only'' approach to topological quantum computation. The physically most relevant example of Ising anyons or Majorana zero modes is considered in detail, particularly in the context of Majorana nanowires.

DOI
10.1103/physrevb.87.035113

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Topological Quantum Computing via Non-Abelian Anyon Braiding and Majorana Modes — E8 Intelligence Research

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FINDING: Topological quantum computing uses non-Abelian anyons (Majorana zero modes) for fault-tolerant qubits, with braiding operations encoding quantum gates. | MATH: Braid group \( B_n \) generators satisfy \( \sigma_i \sigma_{i+1} \sigma_i = \sigma_{i+1} \sigma_i \sigma_{i+1} \); Majorana operators \( \gamma_i \) satisfy \( \{\gamma_i, \gamma_j\} = 2\delta_{ij} \); fusion rules for Ising anyons: \( \sigma \times \sigma = 1 + \psi \), \( \sigma \times \psi = \sigma \), \( \psi \times \psi = 1 \). | CONNECTION: Braid group is deeply linked to the golden ratio via the Temperley-Lieb algebra at \( q = e^{i\pi/5} \), where the Jones polynomial yields \( \tau = (1+\sqrt{5})/2 \approx 1.618 \); Fibonacci anyons have fusion rules \( \tau \times \tau = 1 + \tau \), directly encoding the golden ratio. | DEPTH: 9 — Non-Abelian statistics and braiding are foundational to topological quantum computation, with direct geometric harmony in Fibonacci anyon models. Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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FINDING: Topological quantum computing uses non-Abelian anyons (Majorana zero modes) to encode qubits in braiding operations, immune to local decoherence. | MATH: Braid group \( B_n \) generators \( \sigma_i \) satisfy \( \sigma_i \sigma_{i+1} \sigma_i = \sigma_{i+1} \sigma_i \sigma_{i+1} \); anyon fusion rules: \( \sigma \times \sigma = 1 + \psi \) (Ising model); Majorana operators \( \gamma_i \) with \( \{\gamma_i, \gamma_j\} = 2\delta_{ij} \); topological qubit encoded in parity \( i\gamma_1\gamma_2 = \pm 1 \). | CONNECTION: Braid group is related to the Fibonacci sequence via the Burau representation; the golden ratio \( \phi = 1.618 \) appears in the quantum dimension of Fibonacci anyons: \( d_\tau = \phi \). The Ising anyon quantum dimension is \( \sqrt{2} \), linking to \( \sqrt{2} \approx 1.414 \), close to 1.4142 (no direct golden ratio). Crystallographic symmetry: Anyon braiding corresponds to the mapping class group of a punctured surface, related to root systems of Lie alge Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com

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I examine, in general, how tunable interactions may be used to perform anyonic teleportation and generate braiding transformations for non-Abelian anyons. I explain how these methods are encompassed by the ``measurement-only'' approach to topological quantum computation. The physically most relevant example of Ising anyons or Majorana zero modes is considered in detail, particularly in the context of Majorana nanowires.
I will discuss the revolutionary new concept of topological quantum computation, which is fault-tolerant at the hardware level with no need, in principle, of any quantum error correction protocols. Errors simply do not occur since the physical qubits and the computation steps are protected against decoherence by non-local topological correlations in the underlying physical system. The key idea is non-Abelian statistics of the quasiparticles (called 'anyons' as opposed to fermions or bosons), where the space-time braiding of the anyons around each other, i.e. quantum 'knots', form topologically protected quantum gate operations. I will describe in detail the theoretical principles guiding the experimental search for the appropriate topological phases of matter where such non-Abelian anyons, which are low-dimensional solid state versions of the elusive and exotic Majorana fermions hypothesized seventy-five years ago, may exist. I will critically discuss the recent experimental claims of observing the Majorana modes in semiconductor nanowire structures following earlier theoretical proposals, outlining the future developments which would be necessary to eventually build a topological quantum computer.
Topological quantum computation based on anyons is a promising approach to achieve fault-tolerant quantum computing. The Majorana zero modes in the Kitaev chain are an example of non-Abelian anyons where braiding operations can be used to perform quantum gates. Here we perform a quantum simulation of topological quantum computing, by teleporting a qubit encoded in the Majorana zero modes of a Kitaev chain. The quantum simulation is performed by mapping the Kitaev chain to its equivalent spin version and realizing the ground states in a superconducting quantum processor. The teleportation transfers the quantum state encoded in the spin-mapped version of the Majorana zero mode states between two Kitaev chains. The teleportation circuit is realized using only braiding operations and can be achieved despite being restricted to Clifford gates for the Ising anyons. The Majorana encoding is a quantum error detecting code for phase-flip errors, which is used to improve the average fidelity of the teleportation for six distinct states from 70.76±0.35% to 84.60±0.11%, well beyond the classical bound in either case.
FINDING: Topological quantum computing uses non-Abelian anyons (Majorana zero modes) for fault-tolerant qubits, with braiding operations encoding quantum gates. | MATH: Braid group Bn B_n Bn​ generators satisfy σiσi+1σi=σi+1σiσi+1 \sigma_i \sigma_{i+1} \sigma_i = \sigma_{i+1} \sigma_i \sigma_{i+1} σi​σi+1​σi​=σi+1​σi​σi+1​; Majorana operators γi \gamma_i γi​ satisfy {γi,γj}=2δij \{\gamma_i, \gamma_j\} = 2\delta_{ij} {γi​,γj​}=2δij​; fusion rules for Ising anyons: σ×σ=1+ψ \sigma \times \sigma = 1 + \psi σ×σ=1+ψ, σ×ψ=σ \sigma \times \psi = \sigma σ×ψ=σ, ψ×ψ=1 \psi \times \psi = 1 ψ×ψ=1. | CONNECTION: Braid group is deeply linked to the golden ratio via the Temperley-Lieb algebra at q=eiπ/5 q = e^{i\pi/5} q=eiπ/5, where the Jones polynomial yields τ=(1+5)/2≈1.618 \tau = (1+\sqrt{5})/2 \approx 1.618 τ=(1+5​)/2≈1.618; Fibonacci anyons have fusion rules τ×τ=1+τ \tau \times \tau = 1 + \tau τ×τ=1+τ, directly encoding the golden ratio. | DEPTH: 9 — Non-Abelian statistics and braiding are foundational to topological quantum computation, with direct geometric harmony in Fibonacci anyon models. 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) and braid group representations to encode fault-tolerant qubits, with Microsoft's Majorana 1 chip claiming hardware realization. | MATH: Braid group Bn B_n Bn​ generators σi \sigma_i σi​ satisfy σiσi+1σi=σi+1σiσi+1 \sigma_i \sigma_{i+1} \sigma_i = \sigma_{i+1} \sigma_i \sigma_{i+1} σi​σi+1​σi​=σi+1​σi​σi+1​ and σiσj=σjσi \sigma_i \sigma_j = \sigma_j \sigma_i σi​σj​=σj​σi​ for ∣i−j∣>1 |i-j|>1 ∣i−j∣>1. Anyonic exchange yields unitary matrices U(σi) U(\sigma_i) U(σi​) with non-commuting phases eiθ e^{i\theta} eiθ, where θ \theta θ depends on topological charge (e.g., Ising anyons: θ=π/8 \theta = \pi/8 θ=π/8 for σ \sigma σ particles). Fibonacci anyons: dimension d=ϕ=(1+5)/2≈1.618 d = \phi = (1+\sqrt{5})/2 \approx 1.618 d=ϕ=(1+5​)/2≈1.618, with fusion rules τ×τ=1+τ \tau \times \tau = 1 + \tau τ×τ=1+τ. Majorana zero modes: γi†=γi \gamma_i^\dagger = \gamma_i γi†​=γi​, {γi,γj}=2δij \{\gamma_i, \gamma_j\} = 2\delta_{ij} {γi​,γj​}=2δij​, parity P=ik∏γi P = i^k \prod \gamma_i P=ik∏γi​. | CONNECTION: Fibonacci anyon dimension d=ϕ=1.618 d = \phi = 1.618 d=ϕ=1.618 — direct golden ratio e Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com
A paradigm to build a quantum computer, based on topological invariants is highlighted. The identities in the ensemble of knots, links and braids originally discovered in relation to topological quantum field theory are shown: how they define Artin braid group -- the mathematical basis of topological quantum computation (TQC). Vector spaces of TQC correspond to associated strings of particle interactions, and TQC operates its calculations on braided strings of special physical quasiparticles -- anyons -- with non-Abelian statistics. The physical platform of TQC is to use the topological quantum numbers of such small groups of anyons as qubits and to perform operations on these qubits by exchanging the anyons, both within the groups that form the qubits and, for multi-qubit gates, between groups. By braiding two or more anyons, they acquire up a topological phase or Berry phase similar to that found in the Aharonov-Bohm effect. Topological matter such as fractional quantum Hall systems and novel discovered topological insulators open the way to form system of anyons -- Majorana fermions -- with the unique property of encoding and processing quantum information in a naturally fault-tolerant way. In the topological insulators, due to its fundamental attribute of topological surface state occurrence of the bound, Majorana fermions are generated at its heterocontact with superconductors. One of the key operations of TQC -- braiding of non-Abelian anyons: it is illustrated how it can be implemented in one-dimensional topological isolator wire networks.
FINDING: Topological quantum computing uses non-Abelian anyons (Majorana zero modes) to encode qubits in braiding operations, immune to local decoherence. | MATH: Braid group Bn B_n Bn​ generators σi \sigma_i σi​ satisfy σiσi+1σi=σi+1σiσi+1 \sigma_i \sigma_{i+1} \sigma_i = \sigma_{i+1} \sigma_i \sigma_{i+1} σi​σi+1​σi​=σi+1​σi​σi+1​; anyon fusion rules: σ×σ=1+ψ \sigma \times \sigma = 1 + \psi σ×σ=1+ψ (Ising model); Majorana operators γi \gamma_i γi​ with {γi,γj}=2δij \{\gamma_i, \gamma_j\} = 2\delta_{ij} {γi​,γj​}=2δij​; topological qubit encoded in parity iγ1γ2=±1 i\gamma_1\gamma_2 = \pm 1 iγ1​γ2​=±1. | CONNECTION: Braid group is related to the Fibonacci sequence via the Burau representation; the golden ratio ϕ=1.618 \phi = 1.618 ϕ=1.618 appears in the quantum dimension of Fibonacci anyons: dτ=ϕ d_\tau = \phi dτ​=ϕ. The Ising anyon quantum dimension is 2 \sqrt{2} 2​, linking to 2≈1.414 \sqrt{2} \approx 1.414 2​≈1.414, close to 1.4142 (no direct golden ratio). Crystallographic symmetry: Anyon braiding corresponds to the mapping class group of a punctured surface, related to root systems of Lie alge Author: Andrew Stewart Caldin, Independent Researcher, UK. Part of the E8 Intelligence Research series. Platform: e8intelligence.com