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In the present case the size of the ensemble is chosen between 500Â K and 10Â M, depending on different ellipticities, which is large enough to get a statistically reliable double ionization subensemble. In the calculations the phase Ï• is set randomly within the interval (0, 2Ï€) for each ensemble member to mimic the phase of a real laser pulse, and at the end of the laser pulse, the positions and momenta of the two electrons are recorded.
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