Fast, Accurate, and Realizable Two-Qubit Entangling Gates by Quantum Interference in Detuned Rabi Cycles of Rydberg Atoms

TL;DR

This paper introduces a practical scheme for high-fidelity, fast, and robust two-qubit entangling gates using quantum interference in detuned Rabi cycles of Rydberg atoms, addressing motion-induced dephasing issues.

Contribution

The authors propose a novel interference-based method for implementing accurate Rydberg entangling gates with minimal dephasing and high speed, improving scalability for neutral atom quantum computing.

Findings

Gate fidelity limited only by rotation error and Rydberg decay

Motion-induced dephasing minimized due to no population in Rydberg states during operation

Scheme is resilient to variations in Rydberg interaction strength V

Abstract

High-fidelity entangling quantum gates based on Rydberg interactions are required for scalable quantum computing with neutral atoms. Their realization, however, meets a major stumbling block -- the motion-induced dephasing of the transition between the ground and Rydberg states. By using quantum interference between different detuned Rabi oscillations, we propose a practical scheme to realize a class of accurate entangling Rydberg quantum gates subject to a minimal dephasing error. We show two types of such gates, $U_{1}$ and $U_{2}$, in the form of $\text{diag}\{1, e^{i\alpha}, e^{i\gamma}, e^{i\beta}\}$, where $\alpha, \gamma$, and $\beta$ are determined by the parameters of lasers and the Rydberg blockade $V$. $U_{1}$ is realized by sending to the two qubits a single off-resonant laser pulse, while $U_{2}$ is realized by individually applying one pulse of detuned laser to each qubit. Our method has several advantages. First, the gates are accurate because the fidelity of $U_k$ is limited only by a rotation error below $10^{-5}$ and the Rydberg-state decay. Decay error on the order of $10^{-5}$ can be easily obtained because all transitions are detuned, resulting in small population in Rydberg state. Second, the motion-induced dephasing is minimized because there is no gap time in which a population is left in the Rydberg shelving states of either qubit. Third, the gate is resilient to the variation of $V$. This is because among the three phases $\alpha,\gamma$, and $\beta$, only the last has a (partial) dependence on $V$. Fourth, the Rabi frequency and $V$ in our scheme are of similar magnitude, which permits a fast implementation of the gate when both of them are of the feasible magnitude of several megahertz. The rapidity, accuracy, and feasibility of this interference method can lay the foundation for entangling gates in universal quantum computing with neutral atoms.