2012
DOI: 10.1134/s1054660x12100209
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Nonresonant quantum electrodynamics processes in a pulsed laser field

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Cited by 60 publications
(98 citation statements)
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“…Here in relations (50) and (53 ) solid angles of positron and electron are denoted by dΩ ± . In expressions (49) and (52) parameters γ p+q− and γ p−q+ are determined by relations (18), (19), where it is necessary to replace: p 1 → p + , p 2 → q − for γ p+q− and p 1 → q + , p 2 → p − for γ p−q+ . Relativistic-invariant parameters u (a) and u (b) equals to:…”
Section: The Resonant Differential Cross Sectionmentioning
confidence: 99%
“…Here in relations (50) and (53 ) solid angles of positron and electron are denoted by dΩ ± . In expressions (49) and (52) parameters γ p+q− and γ p−q+ are determined by relations (18), (19), where it is necessary to replace: p 1 → p + , p 2 → q − for γ p+q− and p 1 → q + , p 2 → p − for γ p−q+ . Relativistic-invariant parameters u (a) and u (b) equals to:…”
Section: The Resonant Differential Cross Sectionmentioning
confidence: 99%
“…Another possible scenario of producing electron-positron pairs is the nonlinear BreitWheeler process, which is the main topic of this paper. For recent reviews concerning electron-positron pair creation, we refer the reader to [12][13][14][15][16].…”
Section: Introductionmentioning
confidence: 99%
“…The resonant behavior of the processes of the second order in the fine-structure constant is one of the fundamental problems of quantum electrodynamics in the presence of an external field, whose analysis was started in the mid-1960s (see, for example, reviews [1][2][3][4][5], monographs [6][7][8], and [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24]). …”
Section: Introductionmentioning
confidence: 99%