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.
This implies thatcn = 0for odd nandd kE(0)/dxk = 0for oddk
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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.