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    Quantum optimal control of the Dicke manifold in dipolar Rydberg atom arrays

    Ivy Pannier-Günther1,2,*, Vikas Buchemmavari1,2, Pablo M. Poggi3,1, and Ivan H. Deutsch1,2

    • *Contact author: igunther@unm.edu

    Phys. Rev. A 114, 032412 – Published 8 September, 2026

    DOI: https://doi.org/10.1103/y9rl-cjym

    Abstract

    The ability to engineer and control quantum states of many-body systems is a central challenge in quantum information science. For a register of N qubits, the full Hilbert space dimension grows exponentially as 2N, rendering generic state preparation and control infeasible without exploiting structure or symmetry. A particularly important and physically motivated restriction is to the fully symmetric subspace, spanned by the Dicke states, which are simultaneous eigenstates of collective spin J=N/2. Ensembles of Rydberg atoms interacting via electric dipoles in two-dimensional tweezer arrays form a promising platform for achieving such control. However, the finite range of dipole-dipole interactions poses a challenge to generating and controlling the Dicke manifold because the Hamiltonian incurs leakage from the computational subspace. To counteract this leakage, we perform quantum optimal control algorithms on a truncated Hilbert space according to the method of “irrep distillation” (IRD), which captures the process by which the symmetric subspace couples to leakage error-spaces, using only linear-scaling Hilbert dimension. We implement gradient ascent pulse engineering (GrAPE) on control schemes with little or no local addressing, to generate resourceful states like Greenberger-Horne-Zeilinger, Dicke, and extremal quantum states. We benchmark each scheme of IRD-GrAPE for its quantum speed limit, as well as exactly testing pulse fidelities on small system sizes and predicting fidelities using higher-order IRD on larger systems.

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