A flat-top beam profile created via analytical superposition of Gaussian modes provides spatial selectivity for Rydberg excitation, confirmed by differing Rabi oscillation visibilities between targeted and neighboring atoms in experiment.
[18]), the required input is not the de- sired field profileE(x)itself but its Fourier transform[39] F[E(x)](t) = 1√ 2π ∫∞ −∞E(x) exp(ixt)dx
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Addressable Rydberg excitation in arrays of single neutral atoms with a strongly focused flat-top beam
A flat-top beam profile created via analytical superposition of Gaussian modes provides spatial selectivity for Rydberg excitation, confirmed by differing Rabi oscillation visibilities between targeted and neighboring atoms in experiment.