2004
DOI: 10.1021/jp049153p
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Optimal Control of Ionization Processes in NaK:  Comparison between Theory and Experiment

Abstract: We report a good agreement between the shapes of tailored pulses obtained theoretically and experimentally by using the optimal-control theory and the closed-loop learning technique to maximize the ionization yield in NaK. The theoretical pulse shapes are found to be robust regarding the choice of the initial guess. We assign the leading features of the pulse shapes to processes underlying the optimal control and reveal the mechanism which involves an electronic transition followed by a direct two-photon proce… Show more

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Cited by 53 publications
(50 citation statements)
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“…Among others a very important experimental work was conducted in the group of Wçste, in which they tried to optimize the photoionization yield from NaK with use of the genetic algorithm. [40] This was soon followed by a theoretical analysis by the group of Bonačić-Koutecký, [41] which clarified that the optimized process has been achieved in the series of resonant electronic excitation from the ground state (1 1 S + ) to intermediate excited states sequentially (!2 1 S + !3 1 P) and finally leading to the ionized state NaK + (1 2 S + ). Besides, in each intermediate electronic state the nuclear wavepacket running on it takes some time to move to a position where the succeeding electronic excitation has a large quantum mechanical probability.…”
Section: Introductionmentioning
confidence: 99%
“…Among others a very important experimental work was conducted in the group of Wçste, in which they tried to optimize the photoionization yield from NaK with use of the genetic algorithm. [40] This was soon followed by a theoretical analysis by the group of Bonačić-Koutecký, [41] which clarified that the optimized process has been achieved in the series of resonant electronic excitation from the ground state (1 1 S + ) to intermediate excited states sequentially (!2 1 S + !3 1 P) and finally leading to the ionized state NaK + (1 2 S + ). Besides, in each intermediate electronic state the nuclear wavepacket running on it takes some time to move to a position where the succeeding electronic excitation has a large quantum mechanical probability.…”
Section: Introductionmentioning
confidence: 99%
“…Most of the subpulses can be assigned to multiples of 1 / 2·T osc of the wave packet in the first excited ⌺ state, which is about 220 fs. As observed before, 27 stepwise excitation is likely to yield more efficient production of NaK ions than just a single or double pulse. This assertion is true even if the respective pulse peak intensities are lower.…”
Section: Resultsmentioning
confidence: 58%
“…Assuming the ansatz of controllability, i.e. the probability that a control target can be achieved with a laser controller [21], this allows, on the one hand, calculating optimal energy delivery [22,23] in the time domain for given objectives and, on the other hand, investigating active control knobs from temporal electric field distributions.…”
Section: Introductionmentioning
confidence: 99%