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Breakdown of sequential tunnel ionization in ultrashort electromagnetic pulses
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We consider double ionization of negative bromine ion in intense low-frequency electromagnetic fields. By solving numerically the two-electron time-dependent Schr{\" o}dinger equation we demonstrate that while for pulses of a few tens of femtoseconds duration and longer the sequential single-electron approximation perfectly describes the ionization dynamics, for pulses as short as a few femtoseconds this picture breaks down entirely, and the electron-electron interaction suppresses the rate of ionization by roughly one order of magnitude. We also show clear signatures of the collective tunneling effect in the photoelectron density distribution. This counter-intuitive channel of ionization opens up due to the electron-electron repulsion in the direction lateral to the applied electric field.
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Collective tunnel ionization in atomic systems
Two electrons can escape an atom simultaneously through a collective tunneling channel, with the electron-electron repulsion shaping the escape path and leaving a measurable lateral momentum signature.
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