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Long-term cyclotron dynamics of relativistic wave packets: Spontaneous collapse and revival

In this work we study the effects of collapse and revival, as well as the zitterbewegung (ZB) phenomenon, for the relativistic electron wave packets, which are a superposition of the states with quantum numbers sharply peaked around some Landau level n sub(0) of the order of few tens. The probabilit...

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Published in:Physical review. A, Atomic, molecular, and optical physics Atomic, molecular, and optical physics, 2012-02, Vol.85 (2), Article 022105
Main Authors: Demikhovskii, V. Ya, Maksimova, G. M., Perov, A. A., Telezhnikov, A. V.
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container_title Physical review. A, Atomic, molecular, and optical physics
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description In this work we study the effects of collapse and revival, as well as the zitterbewegung (ZB) phenomenon, for the relativistic electron wave packets, which are a superposition of the states with quantum numbers sharply peaked around some Landau level n sub(0) of the order of few tens. The probability densities as well as average velocities of the packet center and the average spin components were calculated analytically and their evolution is visualized. Our computations demonstrate that due to the dephasing of the states for times larger than the cyclotron period the initial wave packet (which includes the states with the positive energy only) loses the spatial localization so that the evolution can no longer be described classically. However, at the half-revival time t=T sub(R)/2 its reshaping takes place first. It is shown that the behavior of the wave packet containing the states of both energy bands (with E sub(n)>0 and E sub(n)0 only. The obtained results can be useful for the description of electromagnetic radiation and absorption in relativistic plasma on astrophysics objects, where superhigh magnetic field has a value of the order 10 super(8)-10 super(9)T, as well as for interpretation of experiments with trapped ions.
doi_str_mv 10.1103/PhysRevA.85.022105
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However, at the half-revival time t=T sub(R)/2 its reshaping takes place first. It is shown that the behavior of the wave packet containing the states of both energy bands (with E sub(n)&gt;0 and E sub(n)&lt;0) is more complicated. At short times of a few classical periods such a packet splits into two parts, which rotate with cyclotron frequency in the opposite directions and meet each other every one-half of the cyclotron period. At these moments their wave functions have a significant overlap that leads to ZB, and at the time of fractional revival each of two subpackets is decomposed into few packet fractions. However, at t=T sub(R) each of the two subpackets (with positive or negative energy) restores at various points of the cyclotron orbit, which makes reshaping of the initial wave packet impossible, entirely unlike the wave packet which consists of states with energies E sub(n)&gt;0 only. 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source American Physical Society:Jisc Collections:APS Read and Publish 2023-2025 (reading list)
subjects Collapse
Cyclotrons
Density
Evolution
Mathematical analysis
Position (location)
Relativistic plasmas
Wave packets
title Long-term cyclotron dynamics of relativistic wave packets: Spontaneous collapse and revival
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