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From Majorana Fermions to Topological Order
Quantum Physics · Submitted 18 Jan 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that the fermionic Hamiltonian modeling this system is topologically-ordered in a region of parameter space.
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The abstract, sentence by sentence
We consider a system consisting of a 2D network of links between Majorana fermions on superconducting islands. We show that the fermionic Hamiltonian modeling this system is topologically-ordered in a region of parameter space. In particular we show that Kitaev's toric code emerges in fourth-order perturbation theory. By using a Jordan-Wigner transformation we can map the model onto a family of signed 2D Ising models in a transverse field where the signs (FM or AFM) are determined by additional gauge bits. Our mapping allows an understanding of the non-perturbative regime and the phase transition to a non-topological phase. We discuss the physics behind a possible implementation of this model and argue how it can be used for topological quantum computation by adiabatic changes in the Hamiltonian.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider a system consisting of a 2D network of links between Majorana fermions on superconducting islands. | contribution 0.54 | 0.33 | 0.03 | asserted 0.75 |
| s1 | We show that the fermionic Hamiltonian modeling this system is topologically-ordered in a region of parameter space. | result 0.97 | 0.95 | 0.76 | asserted 1.00 |
| s2 | In particular we show that Kitaev's toric code emerges in fourth-order perturbation theory. | result 0.99 | 0.91 | 0.23 | asserted 1.00 |
| s3 | By using a Jordan-Wigner transformation we can map the model onto a family of signed 2D Ising models in a transverse field where the signs (FM or AFM) are determined by additional gauge bits. | method 0.97 | 0.89 | 0.06 | asserted 0.88 |
| s4 | Our mapping allows an understanding of the non-perturbative regime and the phase transition to a non-topological phase. | interpretation 0.64 | 0.86 | 0.12 | asserted 0.95 |
| s5 | We discuss the physics behind a possible implementation of this model and argue how it can be used for topological quantum computation by adiabatic changes in the Hamiltonian. | interpretation 0.81 | 0.60 | 0.20 | hedged possibility 0.96 |
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The paper
Original abstract
We consider a system consisting of a 2D network of links between Majorana fermions on superconducting islands. We show that the fermionic Hamiltonian modeling this system is topologically-ordered in a region of parameter space. In particular we show that Kitaev's toric code emerges in fourth-order perturbation theory. By using a Jordan-Wigner transformation we can map the model onto a family of signed 2D Ising models in a transverse field where the signs (FM or AFM) are determined by additional gauge bits. Our mapping allows an understanding of the non-perturbative regime and the phase transition to a non-topological phase. We discuss the physics behind a possible implementation of this model and argue how it can be used for topological quantum computation by adiabatic changes in the Hamiltonian.
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How the literature uses it
4 arXiv papers cite this in 22 sentences
Papers citing it · 10 sentences without a confident label
Builds on it 1 paper
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To illustrate the basic premise as it may be applied to architectures with Majorana fermions, we will advance and study a generalization of a model introduced in Ref. [ref] to describe a square lattice array of Josephson-coupled nanowires on superconducting grains.
Arbitrary Dimensional Majorana Dualities and Network Architectures for Topological Matter · Introduction · 1.00
Uses its method or tool 2 papers
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[ref] The bond-algebraic approach, [ref] that we employ to study general exact dualities and fermionization, [ref] allows for the derivation of earlier known dualities as well as a plethora of many new others for rather general networks (or graphs) in arbitrary dimensions and boundary conditions.
Arbitrary Dimensional Majorana Dualities and Network Architectures for Topological Matter · Introduction · 0.96
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The coupling of independent slips is then calculated as the tunnelling amplitude in the cosine potential using semi-classical WKB approximation [ref] , leading to $lnΔ ∝-√(E_J / E_C)$.
Topological ordering in the Majorana Toric Code · Dominant Josephson tunneling rate · 0.95
Compares with it 2 papers
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This latter result was derived, using methods very different to ours, in Ref. [ref] .
Arbitrary Dimensional Majorana Dualities and Network Architectures for Topological Matter · Duality to annealed transverse-field Ising models · 0.81
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These architectures display some similarities to the surface-code setups introduced recently in Refs. [ref] , but seek to leverage the topological quantum information processing afforded by MZMs, rather than pursuing active error correction.
Scalable Designs for Quasiparticle-Poisoning-Protected Topological Quantum Computation with Majorana Zero Modes · Conclusions and Near-term Directions · 1.00
Cites it as background 3 papers
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The phase-diagram (see Fig. [ref]) of the system is rich and has been analyzed [ref] .
Topological ordering in the Majorana Toric Code · The model · 0.92
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[ref] In particular, the possibility of realizing them as zero-energy states localized at the end of one-dimensional systems [so-called Majorana end states (MES)] has been the subject of many recent investigations.
Majorana states in inhomogeneous spin ladders · Introduction · 0.97
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In the Introduction, we succinctly reviewed the effective Hamiltonian for the square lattice array, [ref] depicted in Fig. [ref], of Josephson-coupled granular superconductors carrying each two nanowires.
Arbitrary Dimensional Majorana Dualities and Network Architectures for Topological Matter · Networks of Superconducting Grains and Nanowires · 0.86
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