“…In the case of neutral atoms, the requirement that the gate operation time is short compared to the typical time of decoherence mechanisms, including spontaneous emission, collisions, ionization of the Rydberg states, transitions induced by black body radiation, or motional excitation of the atoms trapped in an optical lattice, leads to the search of state-selective Rydberg excitation schemes using femtosecond pulses. Despite the fact that excitation to a single n-Rydberg level requires nanosecond or cw lasers with a narrow bandwidth, coherent control tools as control algorithms to optimally shape femtosecond laser pulses have been successfully used to address a single transition [6,7], as well as multipulse schemes using 150 fs pulses, which alone would populate about ten n-Rydberg levels, have shown the ability to selectively populate a single or a few levels [8,9]. These different schemes address the excitation of relatively high Rydberg levels, typically of principal quantum numbers as n ∼ 30.…”