Realization of three-qubit quantum error correction with superconducting circuits
By M. Reed, Leonardo DiCarlo, S. Nigg, Luyan Sun, Luigi Frunzio, Steven M. Girvin, Robert J. Schoelkopf. Nature, 2011
586 citations recorded by the source corpus.
Quantum computers could be used to solve certain problems exponentially faster than classical computers, but are challenging to build because of their increased susceptibility to errors. However, it is possible to detect and correct errors without destroying coherence, by using quantum error correcting codes. The simplest of these are three-quantum-bit (three-qubit) codes, which map a one-qubit state to an entangled three-qubit state; they can correct any single phase-flip or bit-flip error on one of the three qubits, depending on the code used. Here we demonstrate such phase- and bit-flip error correcting codes in a superconducting circuit. We encode a quantum state, induce errors on the qubits and decode the error syndrome—a quantum state indicating which error has occurred—by reversing the encoding process. This syndrome is then used as the input to a three-qubit gate that corrects the primary qubit if it was flipped. As the code can recover from a single error on any qubit, the fidelity of this process should decrease only quadratically with error probability. We implement the correcting three-qubit gate (known as a conditional-conditional NOT, or Toffoli, gate) in 63 nanoseconds, using an interaction with the third excited state of a single qubit. We find 85 ± 1 per cent fidelity to the expected classical action of this gate, and 78 ± 1 per cent fidelity to the ideal quantum process matrix. Using this gate, we perform a single pass of both quantum bit- and phase-flip error correction and demonstrate the predicted first-order insensitivity to errors. Concatenation of these two codes in a nine-qubit device would correct arbitrary single-qubit errors. In combination with recent advances in superconducting qubit coherence times, this could lead to scalable quantum technology.
Subfields: Artificial Intelligence, Computational Theory and Mathematics
View Paper: https://www.semanticscholar.org/paper/14df5da28c3c056db2124222e6c327e6f5159daa
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In Artificial Intelligence
- Göran Wendin
- Steven M. Girvin
- Ryan Babbush
- Alexandre Blais
- Jarrod R. McClean
- Robert J. Schoelkopf
- Franco Nori
- William D. Oliver
In Computational Theory and Mathematics
- Göran Wendin
- Craig Gidney
- Daniel Loss
- T. O’Brien
- Masoud Mohseni
- William J. Huggins
- Alexei Y. Kitaev
- Jarrod R. McClean
Citations in the corpus
- Exponential suppression of bit or phase errors with cyclic error correction (2021, background): “[33] 2012 Repetition Code [3,1,3] 3 single shot Superconducting”
- Entanglement in a Quantum Annealing Processor (2014, background): “[3] M.”
- 1 / f noise: Implications for solid-state quantum information (2013, background): “…oscillations in superconducting charge qubits (Pashkin et al., 2003), several benchmarking results have been reached in different labs (Di Carlo et al., 2010; Fedorov et al., 2012; Lucero et al., 2012; Mariantoni et al., 2011; Neeley et al., 2010; Palacios-Laloy et al., 2010; Reed et al., 2012).”
- Quantum memories at finite temperature (2014, background): “…protocols present an uphill technical challenge for both engineering complex entangled error-correcting codes, and for reducing incident laboratory noise below a threshold value when compared with current experimental achievements (Barends et al., 2014; Nigg et al., 2014; Reed et al., 2012).”
- Quantum information processing with superconducting circuits: a review (2016, methodology): “These can be implemented in several ways: (i) sequentially, by series of 1q and 2q gates to yield CCNOT (Toffoli) or CCZ [120, 272, 273]; (ii) by a ‘singleshot’ optim ised pulse sequence [274, 275]; or (iii) by singleshot collec tive excitation via bus dynamics.”
- Quantum trajectories and open many-body quantum systems (2014, background): “Quantum coherence has been observed, and decoherence studies performed in atomic systems including photon modes in cavities [11–15]; single trapped atoms [16], ions [8, 17–21], and molecules [22, 23]; and in solid state systems [9, 24] including superconducting junctions [25], and spin systems inclu”
- Circuit QED: Superconducting Qubits Coupled to Microwave Photons (2015, methodology): “…al., 2011a; Wang et al., 2011), entangle two (Ansmann et al., 2009; Chow et al., 2010) and three qubits (Neeley et al., 2010; DiCarlo et al., 2010), run simple quantum algorithms (DiCarlo et al., 2009; Mariantoni et al., 2011b) and perform rudimentary quantum error correction (Reed et al., 2012).”
- Widely Tunable On-Chip Microwave Circulator for Superconducting Quantum Circuits (2017, background): “Demonstrations of this third stage have been made with trapped-ions [40], Rydberg atoms [41], Nitrogen vacancy centers [42], and superconducting qubits [43, 44, 45].”