Symmetrized Characterization of Noisy Quantum Processes
Joseph Emerson1,2,
Marcus Silva2,3,
Osama Moussa2,3,
Colm Ryan2,3,
Martin Laforest2,3,
Jonathan Baugh2,
David G. Cory4 and
Raymond Laflamme2,3,5
1 Department of Applied Math, University of Waterloo, Waterloo, ON N2L 3G1, Canada.
2 Institute for Quantum Computing, University of Waterloo, Waterloo, ON N2L 3G1, Canada.
3 Department of Physics and Astronomy, University of Waterloo, Waterloo, ON N2L 3G1, Canada.
4 Department of Nuclear Science and Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA.
5 Perimeter Institute for Theoretical Physics, Waterloo, ON N2L 2Y5, Canada.
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Fig. 1. Schematic of coarse-graining by symmetrization. Averaging the noise by twirling under a symmetry group yields an effective noise process that has a reduced number of independent parameters. Distinct symmetrization groups [represented by (a) red and (b) blue] uniformize different subsets of parameters.
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Fig. 2. Quantum circuit. One experimental run consists of a conjugation of the noise process . The standard protocol requires conjugation only by an element Ci, whereas the ensemble protocol requires conjugating also by a permutation s of the qubits. The standard protocol requires only one input state , whereas the ensemble protocol requires n distinct input operators w.
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Fig. 3. Results for pw from experiments 5 and 6 in Table 1. Shown are projections of the four-dimensional likelihood function onto various probability planes. The asymmetry seen in some of the confidence areas is a result of this projection. The results for one cycle with 10 µs pulse spacing (experiment 5) are in red, and the results for two cycles with 5 µs spacing (experiment 6) are in blue.
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