Quantum optimal control of the Dicke manifold in dipolar Rydberg atom arrays
- URL: http://arxiv.org/abs/2606.02283v2
- Date: Tue, 09 Jun 2026 22:29:13 GMT
- Title: Quantum optimal control of the Dicke manifold in dipolar Rydberg atom arrays
- Abstract summary: We study the ability to engineer and control quantum states of many-body systems.<n>For a register of $N$ qubits, the full Hilbert space dimension grows exponentially as $2N$.<n>We implement gradient ascent pulse engineering (GrAPE) on control schemes with little or no local addressing.
- Score: 0.0
- License: http://creativecommons.org/licenses/by/4.0/
- 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 $2^N$, 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 our newly developed 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 (QSL), 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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