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This research presents a mean-field approximation model to overcome computational barriers in controlling arrays of interacting Rydberg atoms for quantum simulation. By adapting pulses designed for non-interacting systems, the method maintains high fidelity with less than 1% error even as system size increases beyond standard numerical limits. This advancement is critical for scaling up neutral-atom quantum processors where interatomic interactions are a dominant factor in state preparation and gate operations.
Mean-field Pulse Adaptation for the Circulatization of Interacting Rydberg Atoms
arXiv:2607.26978v1 Announce Type: new Abstract: Arrays of circular Rydberg atoms provide a promising platform for quantum simulation and computation; however, their preparation in the presence of interatomic interactions remains a major challenge. While optimal control methods have enabled the design of fast and accurate radio-frequency pulses for the circularization of a single atom and of an atom pair, the extension to more atoms is fundamentally limited by the exponential growth of the Hilbert space, which renders numerical simulations computationally infeasible. Here, we introduce an effective model that treats interactions within a mean-field approximation, thereby enabling the simulation of large atomic systems. Our model further enables the adaptation of pulses optimized for non-interacting atoms to interacting systems, based on the computation of a single time evolution. For two interacting $^{87}\mathrm{Rb}$ atoms, we demonstrate that the error of our method remains below $1 \, \%$ and that our adapted pulses recover the initial performance of optimal pulses in the regime of weak to moderate interaction strengths.
Abstract:Arrays of circular Rydberg atoms provide a promising platform for quantum simulation and computation; however, their preparation in the presence of interatomic interactions remains a major challenge. While optimal control methods have enabled the design of fast and accurate radio-frequency pulses for the circularization of a single atom and of an atom pair, the extension to more atoms is fundamentally limited by the exponential growth of the Hilbert space, which renders numerical simulations computationally infeasible. Here, we introduce an effective model that treats interactions within a mean-field approximation, thereby enabling the simulation of large atomic systems. Our model further enables the adaptation of pulses optimized for non-interacting atoms to interacting systems, based on the computation of a single time evolution. For two interacting $^{87}\mathrm{Rb}$ atoms, we demonstrate that the error of our method remains below $1 \, \%$ and that our adapted pulses recover the initial performance of optimal pulses in the regime of weak to moderate interaction strengths.
Quantum Physics (quant-ph); Atomic Physics (physics.atom-ph)
arXiv:2607.26978 [quant-ph]
(or arXiv:2607.26978v1 [quant-ph] for this version)
https://doi.org/10.48550/arXiv.2607.26978 Focus to learn more arXiv-issued DOI via DataCite (pending registration)
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