High-On-Off-Ratio Beam-Splitter Interaction for Gates on Bosonically Encoded Qubits

Encoding a qubit in a high-quality superconducting microwave cavity offers the opportunity to perform the first layer of error correction in a single device but presents a challenge: how can quantum oscillators be controlled while introducing a minimal number of additional error channels? We focus o...

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Veröffentlicht in:PRX quantum 2023-06, Vol.4 (2), p.020355, Article 020355
Hauptverfasser: Chapman, Benjamin J., de Graaf, Stijn J., Xue, Sophia H., Zhang, Yaxing, Teoh, James, Curtis, Jacob C., Tsunoda, Takahiro, Eickbusch, Alec, Read, Alexander P., Koottandavida, Akshay, Mundhada, Shantanu O., Frunzio, Luigi, Devoret, M.H., Girvin, S.M., Schoelkopf, R.J.
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Sprache:eng
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Zusammenfassung:Encoding a qubit in a high-quality superconducting microwave cavity offers the opportunity to perform the first layer of error correction in a single device but presents a challenge: how can quantum oscillators be controlled while introducing a minimal number of additional error channels? We focus on the two-qubit portion of this control problem by using a three-wave-mixing coupling element to engineer a programmable beam-splitter interaction between two bosonic modes separated by more than an octave in frequency, without introducing major additional sources of decoherence. Combining this with single-oscillator control provided by a dispersively coupled transmon provides a framework for quantum control of multiple encoded qubits. The beam-splitter interaction g_{bs} is fast relative to the time scale of oscillator decoherence, enabling over 10^{3} beam-splitter operations per coherence time and approaching the typical rate of the dispersive coupling χ used for individual oscillator control. Further, the programmable coupling is engineered without adding unwanted interactions between the oscillators, as evidenced by the high on-off ratio of the operations, which can exceed 10^{5}. We then introduce a new protocol to realize a hybrid controlled-swap operation in the regime g_{bs}≈χ, in which a transmon provides the control bit for the swap of two bosonic modes. Finally, we use this gate in a swap test to project a pair of bosonic qubits into a Bell state with measurement-corrected fidelity of 95.5%±0.2%.
ISSN:2691-3399
2691-3399
DOI:10.1103/PRXQuantum.4.020355