Single temporal-pulse-modulated parameterized controlled-phase gate for Rydberg atoms
arXiv:2201.05994 · doi:10.1103/PhysRevApplied.18.044042
Abstract
We propose an adiabatic protocol for implementing a controlled-phase gate CZ with continuous of neutral atoms through a symmetrical two-photon excitation process via the second resonance line, in Rb, with a single-temporal-modulation-coupling of the ground state and intermediate state. Relying on different adiabatic paths, the phase factor of CZ gate can be accumulated on the logic qubit state alone by calibrating the shape of the temporal pulse where strict zero amplitudes at the start and end of the pulse are not needed. For a wide range of , we can obtain the fidelity of CZ gate over in less than s, in the presence of spontaneous emission from intermediate and Rydberg states. And in particular for , we benchmark the performance of the CZ gate by taking into account various experimental imperfections, such as Doppler shifts, fluctuation of Rydberg-Rydberg interaction strength, inhomogeneous Rabi frequency, and noise of driving fields, etc, and show that the predicted fidelity is able to maintain at about after correcting the measurement error. This gate protocol provides a robustness against the fluctuation of pulse amplitude and a flexible way for adjusting the entangling phase, which may contribute to the experimental implementation of near-term noisy intermediate-scale quantum (NISQ) computation and algorithm with neutral-atom systems.
15 pages, 12 figures, accepted by Phys. Rev. Applied
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- Simulation of a feedback-based algorithm for quantum optimization for a realistic neutral atom system with an optimized small-angle controlled-phase gate
- Holonomic swap and controlled-swap gates of neutral atoms via selective Rydberg pumping
- Fast nuclear-spin entangling gates compatible with large-scale atomic arrays
- Inertial geometric quantum logic gates
- Symmetric gate for ultracold neutral atoms based on counterdiabatic driving at Rydberg excitation
- Engineering the non-Hermitian Su-Schrieffer-Heeger model with skin effects in Rydberg atom arrays