Dynamic Bragg microcavities in collisions of unipolar light pulses of unusual shape in two- and three-level medium

• URL: http://arxiv.org/abs/2503.08243v1
• Date: Tue, 11 Mar 2025 10:07:05 GMT
• Title: Dynamic Bragg microcavities in collisions of unipolar light pulses of unusual shape in two- and three-level medium
• Authors: Rostislav Arkhipov, Mikhail Arkhipov, Nikolay Rosanov,
• Abstract summary: Unipolar light pulses with a non-zero electric area can be used for ultrafast control of quantum systems.<n>To control atomic properties in an efficient way, it is necessary to vary the temporal shape of the pulses used.<n>New phenomena, not possible with conventional multi-cycle pulses, were discovered by analyzing the interaction of such unipolar pulses with matter.
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• License: http://creativecommons.org/licenses/by/4.0/
• Abstract: Unipolar light pulses with a non-zero electric area due to the unidirectional action on charged particles can be used for the ultrafast control of the properties of quantum systems. To control atomic properties in an efficient way, it is necessary to vary the temporal shape of the pulses used. This has led to the problem of obtaining pulses of an unusual shape, such as a rectangular one. A number of new phenomena, not possible with conventional multi-cycle pulses, were discovered by analyzing the interaction of such unipolar pulses with matter. These include the formation of dynamic microcavities at each resonant transition of a multilevel medium when such pulses collide with the medium. In this work, we compare the behavior of dynamic microcavities in a two-level and a three-level medium when unipolar pulses of unusual shape (rectangular) are collided with the medium. We do this on the basis of the numerical solution of the system for the density matrix of the medium and the wave equation for the electric field. Medium parameters correspond to atomic hydrogen. It is shown that for rectangular pulses in a three-level medium, the dynamics of the cavities can be very different from the two-level model, as opposed to pulses of other shapes (e.g. Gaussian shape). When the third level of the medium is taken into account, the self-induced transparency-like regime disappears. Differences in the dynamics of resonators in a three-level medium are revealed when the pulses behave like 2{\pi} pulses of self-induced transparency.

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