2015
DOI: 10.1103/physrevx.5.041040
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Parafermions in a Kagome Lattice of Qubits for Topological Quantum Computation

Abstract: Engineering complex non-Abelian anyon models with simple physical systems is crucial for topological quantum computation. Unfortunately, the simplest systems are typically restricted to Majorana zero modes (Ising anyons). Here we go beyond this barrier, showing that the Z4 parafermion model of non-Abelian anyons can be realized on a qubit lattice. Our system additionally contains the Abelian D(Z4) anyons as low-energetic excitations. We show that braiding of these parafermions with each other and with the D(Z4… Show more

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Cited by 19 publications
(26 citation statements)
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“…Exchange and transverse-field clock-model couplings take on a particular simple form in this language: (35) and then introduce spinful fermions d a,α via a Bogoliubov transformation:…”
Section: E Spin-1/2 Representation and Alternative Fermionization Scmentioning
confidence: 99%
See 1 more Smart Citation
“…Exchange and transverse-field clock-model couplings take on a particular simple form in this language: (35) and then introduce spinful fermions d a,α via a Bogoliubov transformation:…”
Section: E Spin-1/2 Representation and Alternative Fermionization Scmentioning
confidence: 99%
“…Finally, parafermion chains are related to bosonic clock models (for any Z N ) [15,32]-a relation that we will frequently exploit. In the Z 4 limit, one can decompose clock spins into two sets of Pauli matrices [33][34][35] that can be fermionized by standard methods [36]. We will later draw further connections to all of these works, particularly the results for quantum-spin-Hall systems.…”
Section: Introductionmentioning
confidence: 99%
“…Unfortunately, many proposals to physically realize parafermions concern the case where d is even [7,[10][11][12]23,25]. On the other hand, Z 3 parafermions can, for example, emerge in interacting nanowires [17,19,20]; see also Ref.…”
Section: Discussionmentioning
confidence: 99%
“…This includes the case d = 2, i.e., Majorana fermions in a qubit toric code. Reference [25] describes in detail how this can be achieved for d = 4, and the generalization to arbitrary d is straightforward.…”
Section: Discussionmentioning
confidence: 99%
“…Alternatively, braiding can be done using either interaction-based proposals [31,32] or a measurement-only approach [33][34][35] without physically moving anyons. These two approaches are shown to be equivalent [36] and they can avoid diabatic errors associated with moving anyons.…”
Section: Introductionmentioning
confidence: 99%