ID: 2404.00091

Non-Abelian braiding of Fibonacci anyons with a superconducting processor

March 29, 2024

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Demonstrating anyonic non-Abelian statistics with a minimal $d = 6$ qudit lattice

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Lucy Byles, Ewan Forbes, Jiannis K. Pachos
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Quantum double models provide a natural framework for realising anyons by manipulating a lattice of qudits, which can be directly encoded in quantum simulators. In this work, we consider a lattice of $d=6$ qudits that give rise to $\mathbf{D}(\mathbf{S}_3)$ non-Abelian anyons. We present a method that demonstrates the non-commutativity of the braiding and fusion evolutions solely by utilising the operators that create and measure anyons. Furthermore, we provide a dense coding...

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String-nets, single and double-stranded quantum loop gases for non-Abelian anyons

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Andrea Velenich, Claudio Chamon, Xiao-Gang Wen
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String-net condensation can give rise to non-Abelian anyons whereas loop condensation usually gives rise to Abelian anyons. It has been proposed that generalized quantum loop gases with non-orthogonal inner products can produce non-Abelian anyons. We detail an exact mapping between the string-net and the generalized loop models and explain how the non-orthogonal products arise. We also introduce a loop model of double-stranded nets where quantum loops with an orthogonal inner...

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Emulating anyonic fractional statistical behavior in a superconducting quantum circuit

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Y. P. Zhong, D. Xu, P. Wang, C. Song, Q. J. Guo, W. X. Liu, K. Xu, B. X. Xia, Chao-Yang Lu, Siyuan Han, ... , Wang Haohua
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Anyons are exotic quasiparticles obeying fractional statistics,whose behavior can be emulated in artificially designed spin systems.Here we present an experimental emulation of creating anyonic excitations in a superconducting circuit that consists of four qubits, achieved by dynamically generating the ground and excited states of the toric code model, i.e., four-qubit Greenberger-Horne-Zeilinger states. The anyonic braiding is implemented via single-qubit rotations: a phase ...

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Fibonacci topological phase in arrays of anyonic chains

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Hiromi Ebisu
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Fibonacci anyon, an exotic quasi-particle excitation, plays a pivotal role in realization of a quantum computer. Starting from a $SU(2)_4$ topological phase, in this paper we demonstrate a way to construct a Fibonacci topological phase which has only one non-trivial excitation described by the Fibonacci anyon. We show that arrays of anyonic chains created by excitations of the $SU(2)_4$ phase leads to the Fibonacci phase. We further demonstrate that our theoretical propositio...

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Dyck Paths and Topological Quantum Computation

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Vivek Kumar Singh, Akash Sinha, ... , Jana Indrajit
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The fusion basis of Fibonacci anyons supports unitary braid representations that can be utilized for universal quantum computation. We show a mapping between the fusion basis of three Fibonacci anyons, $\{|1\rangle, |\tau\rangle\}$, and the two length 4 Dyck paths via an isomorphism between the two dimensional braid group representations on the fusion basis and the braid group representation built on the standard $(2,2)$ Young diagrams using the Jones construction. This corre...

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How quickly can anyons be braided? Or: How I learned to stop worrying about diabatic errors and love the anyon

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Christina Knapp, Michael Zaletel, Dong E. Liu, Meng Cheng, ... , Nayak Chetan
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Topological phases of matter are a potential platform for the storage and processing of quantum information with intrinsic error rates that decrease exponentially with inverse temperature and with the length scales of the system, such as the distance between quasiparticles. However, it is less well-understood how error rates depend on the speed with which non-Abelian quasiparticles are braided. In general, diabatic corrections to the holonomy or Berry's matrix vanish at least...

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James R. Wootton, Jan Burri, ... , Loss Daniel
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The possibility of quantum computation using non-Abelian anyons has been considered for over a decade. However the question of how to obtain and process information about what errors have occurred in order to negate their effects has not yet been considered. This is in stark contrast with quantum computation proposals for Abelian anyons, for which decoding algorithms have been tailor-made for many topological error-correcting codes and error models. Here we address this issue...

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Systematic Computation of Braid Generator Matrix in Topological Quantum Computing

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Abdellah Tounsi, Nacer Eddine Belaloui, Mohamed Messaoud Louamri, Amani Mimoun, ... , Rouabah Mohamed Taha
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We present a systematic numerical method to compute the elementary braiding operations for topological quantum computation (TQC). Braiding non-Abelian anyons is a crucial technique in TQC, offering a topologically protected implementation of quantum gates. However, obtaining matrix representations for braid generators can be challenging, especially for systems with numerous anyons or complex fusion patterns. Our proposed method addresses this challenge, allowing for the inclu...

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Why should anyone care about computing with anyons?

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Gavin K. Brennen, Jiannis K. Pachos
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In this article we present a pedagogical introduction of the main ideas and recent advances in the area of topological quantum computation. We give an overview of the concept of anyons and their exotic statistics, present various models that exhibit topological behavior, and we establish their relation to quantum computation. Possible directions for the physical realization of topological systems and the detection of anyonic behavior are elaborated.

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Quantum Field Theories, Topological Materials, and Topological Quantum Computing

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Muhammad Ilyas
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A quantum computer can perform exponentially faster than its classical counterpart. It works on the principle of superposition. But due to the decoherence effect, the superposition of a quantum state gets destroyed by the interaction with the environment. It is a real challenge to completely isolate a quantum system to make it free of decoherence. This problem can be circumvented by the use of topological quantum phases of matter. These phases have quasiparticles excitations ...

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