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Generating and verifying graph states for fault-tolerant topological measurement-based quantum computing in two-dimensional optical lattices

Jaewoo Joo, Emilio Alba, Juan José García-Ripoll, and Timothy P. Spiller
Phys. Rev. A 88, 012328 – Published 26 July 2013

Abstract

We propose two schemes for implementing graph states useful for fault-tolerant topological measurement-based quantum computation in two-dimensional (2D) optical lattices. We show that bilayer cluster and surface-code states can be created by global single-row and controlled-Z operations. The schemes benefit from the accessibility of atom addressing on 2D optical lattices and the existence of an efficient verification protocol which allows us to ensure the experimental feasibility of measuring the fidelity of the system against the ideal graph state. The simulation results show potential for a physical realization toward fault-tolerant measurement-based quantum computation against dephasing and unitary phase errors in optical lattices.

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  • Received 10 April 2013

DOI:https://doi.org/10.1103/PhysRevA.88.012328

©2013 American Physical Society

Authors & Affiliations

Jaewoo Joo1, Emilio Alba2, Juan José García-Ripoll2, and Timothy P. Spiller1

  • 1Quantum Information Science, School of Physics and Astronomy, University of Leeds, Leeds LS2 9JT, United Kingdom
  • 2Instituto de Física Fundamental, Consejo Superior de Investigaciones Científicas, Calle Serrano 113b, E-28006 Madrid, Spain

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Issue

Vol. 88, Iss. 1 — July 2013

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Images

  • Figure 1
    Figure 1
    The schematics of global Hadamard operation at every second row in red dotted atoms.Reuse & Permissions
  • Figure 2
    Figure 2
    To build 3D cluster states, seven CZ and two Hadamard operations are globally required in 2D optical lattices. Solid lines indicate the horizontal and vertical directions in the CZ gates, while dashed lines show the CZ operations in diagonal directions (small black arrows show the direction of moving atoms). In (d), the colored yellow (gray) edges present a unit cell of 3D cluster states in the lattices.Reuse & Permissions
  • Figure 3
    Figure 3
    How to build a surface code directly in 2D optical lattices. The surface code is directly created by Pauli σx measurements (denoted by X) at all red dotted (Li) atoms in (c) [12, 18]. Then, red dotted atoms are removed by turning off their optical lattices.Reuse & Permissions
  • Figure 4
    Figure 4
    (a) and (b) Simulation of the application of the two-qubit verification protocol in the basic blocks shown in Figs. 2d and 3b, respectively, where the simulations are computed with a fixed dephasing error parameter θ=π/5. The color (gray) links show a positive result of the two-qubit entanglement witness. Shaded atoms represent the border of the unit blocks, which has to be measured in order to compute the local fidelity. Values of the fidelity to the graph state as a function of θ for the 3D cubic block (solid) and the surface-code block (dashed) for (c) dephasing and (d) unitary CZ (Ising) errors. The horizontal line shows the minimum value for the observable to show genuine multipartite entanglement. Notice that the plots are roughly similar for both blocks due to the similar size of the blocks considered.Reuse & Permissions
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