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Creation of electron-positron plasma with superstrong laser field

期刊

EUROPEAN PHYSICAL JOURNAL-SPECIAL TOPICS
卷 223, 期 6, 页码 1083-1092

出版社

SPRINGER HEIDELBERG
DOI: 10.1140/epjst/e2014-02159-1

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资金

  1. Russian Fund for Basic Research [11-02-12148ofi-m, 13-02-00372]
  2. RF Ministry of Science and Education [14.A18.21.0773]
  3. RF President programs for support of young Russian scientists and the leading research schools [MD-5838.2013.2]

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We present a short review of recent progress in studying QED effects within the interaction of ultra-relativistic laser pulses with vacuum and e (-) e (+) plasma. Current development in laser technologies promises very rapid growth of laser intensities in the near future. Two exawatt class facilities (ELI and XCELS, Russia) in Europe are already in the planning stage. Realization of these projects will make available a laser intensity of similar to 10(26) W/cm(2) or even higher. Therefore, discussion of nonlinear optical effects in vacuum are becoming compelling for experimentalists and are currently gaining much attention. We show that, in spite of the fact that the expected field strength is still essentially less than E (S) = m (2) c (3)/ea = 1.32 center dot 10(16) V/cm, the nonlinear vacuum effects will be accessible for observation at the ELI and XCELS facilities. The most promissory effect for observation is pair creation by a laser pulse in vacuum. It is shown, that at intensities similar to 5 center dot 10(25) W/cm(2), creation even of a single pair is accompanied by the development of an avalanche QED cascade. There exists a distinctive feature of the laser-induced cascades, as compared with the air showers arising due primarily to cosmic rays entering the atmosphere. In our case the laser field plays not only the role of a target (similar to a nucleus in the case of air showers) but is also responsible for the acceleration of slow particles. It is shown that the effect of pair creation imposes a natural limit for the attainable laser intensity and, apparently, the field strength E similar to E (S) is not accessible for a pair-creating electromagnetic field at all.

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