2018
DOI: 10.1007/s11128-018-1835-8
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Efficient experimental design of high-fidelity three-qubit quantum gates via genetic programming

Abstract: We have designed efficient quantum circuits for the three-qubit Toffoli (controlled-controlled NOT) and the Fredkin (controlled-SWAP) gate, optimized via genetic programming methods. The gates thus obtained were experimentally implemented on a three-qubit NMR quantum information processor, with a high fidelity. Toffoli and Fredkin gates in conjunction with the single-qubit Hadamard gates form a universal gate set for quantum computing, and are an essential component of several quantum algorithms. Genetic algor… Show more

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Cited by 16 publications
(4 citation statements)
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“…Table 5 shows the theoretical and experimental results of the relaxation times for this molecule. The experimental values were taken from [53]. For F1-F3 atoms, the differences between theoretical and experimental values were: for T 1 , 0.08 s, and for T 2 , 0.05 s. For the F1-F2 atoms, the differences between theoretical and experimental values were 0.31 s for T 1 and 0.03 s for T 2 .…”
Section: Validation Of the Theoretical Methodologymentioning
confidence: 99%
“…Table 5 shows the theoretical and experimental results of the relaxation times for this molecule. The experimental values were taken from [53]. For F1-F3 atoms, the differences between theoretical and experimental values were: for T 1 , 0.08 s, and for T 2 , 0.05 s. For the F1-F2 atoms, the differences between theoretical and experimental values were 0.31 s for T 1 and 0.03 s for T 2 .…”
Section: Validation Of the Theoretical Methodologymentioning
confidence: 99%
“…The deviations in the simulated process matrix from the desired process matrix arises due to experimental errors in state preparation, implementa-tion of unitary dilation operators and inevitable systematic errors. These errors can be reduced using appropriate optimization protocols [41]. Particularly for the MFGP process, the experimental implementation of all four unitary dilation operators requires 9 CNOT gates (i.e.9 CNOT gates × 4 Kraus operators = 36 CNOT gates in total to simulate the MFGP process), while for the phase damping channel, the experimental implementation of the unitary dilation operator U A1 , U A2 , U A3 and U A4 requires 8, 3, 3 and 0 CNOT gates, respectively (i.e.14 CNOT gates in total to simulate the phase damping channel).…”
Section: B Simulating a Two-qubit Phase Damping Channelmentioning
confidence: 99%
“…Efficient quantum circuits for a 3-qubit NMR (nuclear magnetic resonance) quantum processor [67] can be obtained by GP algorithms as introduced in [22]. By using GP generated circuits for Toffoli and Fredkin gates, solutions that are robust against decoherence errors can be obtained.…”
Section: B Genetic Programmingmentioning
confidence: 99%