4.6 Article

Speed limits for two-qubit gates with weakly anharmonic qubits

Journal

PHYSICAL REVIEW A
Volume 105, Issue 4, Pages -

Publisher

AMER PHYSICAL SOC
DOI: 10.1103/PhysRevA.105.042614

Keywords

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Funding

  1. MEXT Quantum Leap Flagship Program [JPMXS0120319794]
  2. Japan Science and Technology Agency Core Research for Evolutionary Science and Technology [JPMJCR1775]
  3. National Sciences and Engineering Council of Canada (NSERC)

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This study examines the implementation of two-qubit gates in the presence of additional quantum states in the accessible energy range. The results show that the coupling between higher energy levels can increase the gate speed, while weak anharmonicity constrains the system's control speed. By modifying the pulse optimization algorithm, the impact of higher levels can be minimized. Furthermore, the optimal-control gate speeds are compared with those obtained using other protocols.
We consider the implementation of two-qubit gates when the physical systems used to realize the qubits possess additional quantum states in the accessible energy range. We use optimal control theory to determine the maximum achievable gate speed for two-qubit gates in the qubit subspace of the many-level Hilbert space, and we analyze the effect of the additional quantum states on the gate speed. We identify two competing mechanisms. On one hand, higher energy levels are generally more strongly coupled to each other. Under suitable conditions, this stronger coupling can be utilized to make two-qubit gates significantly faster than the reference value based on simple qubits. On the other hand, a weak anharmonicity constrains the speed at which the system can be adequately controlled: according to the intuitive picture, faster operations require stronger control fields, which are more likely to excite higher levels in a weakly anharmonic system, which in turn leads to faster decoherence and uncontrolled leakage outside the qubit space. To account for this constraint, we modify the pulse optimization algorithm to avoid pulses that lead to appreciable population of the higher levels. In this case, we find that the presence of the higher levels can lead to a significant reduction in the maximum achievable gate speed. We also compare the optimal-control gate speeds with those obtained using the cross-resonance or selectivedarkening gate protocol. We find that this protocol, with some parameter optimization, can be used to achieve a relatively fast implementation of the controlled-NOT gate. These results can help the search for optimized gate implementations in realistic quantum computing architectures, such as those based on superconducting circuits. They also provide guidelines for desirable conditions on anharmonicity that would allow optimal utilization of the higher levels to achieve fast quantum gates.

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