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Scalable, local control over gate operations is an outstanding challenge in the field of quantum computing and programmable quantum simulation with Rydberg atom arrays.
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This is the total scattering rate including both Raman and Rayleigh scattering, but we treat it as Raman scattering when Δ < Δ f \displaystyle\Delta<\Delta_{f} , the fine structure splitting Cline et al. 1994 . Given the required value of Δ \displaystyle\Delta derived below, this is self-consistent for gate errors ϵ ≳ 10 − 4 \displaystyle\epsilon\gtrsim 10^{-4} in Rb and Cs, given Δ r / Γ ≈ 10 6 \displaystyle\Delta_{r}/\Gamma\approx 10^{6} in these atoms
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