1987
DOI: 10.1070/pu1987v030n06abeh002865
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Quantum electrodynamics of strong fields

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Cited by 261 publications
(483 citation statements)
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“…The study of this effect began in connection with the so-called Klein [1] paradox, and was continued by Schwinger [2], who calculated the vacuum-to-vacuum transition probability in a constant electric field. A complete study of particle creation from vacuum by a constant electric field is represented in [3,4]. It should be mentioned that the effect can actually be observed as soon as the external field strength approaches the characteristic value (critical field) E c = m 2 c 3 /|e| ≃ 1, 3 · 10 16 V /cm.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…The study of this effect began in connection with the so-called Klein [1] paradox, and was continued by Schwinger [2], who calculated the vacuum-to-vacuum transition probability in a constant electric field. A complete study of particle creation from vacuum by a constant electric field is represented in [3,4]. It should be mentioned that the effect can actually be observed as soon as the external field strength approaches the characteristic value (critical field) E c = m 2 c 3 /|e| ≃ 1, 3 · 10 16 V /cm.…”
Section: Introductionmentioning
confidence: 99%
“…Considerable attention has been recently focused on a non-perturbative parton production from vacuum by a classical chromoelectric field of SU(3) [12,13] and SU (2) [14] in the framework of a modern version of the known chromoelectric flux tube model [15], the latter being an effective model for the confinement of quarks in QCD (previously the pair creation by a constant field has been calculated for SU (2) in [16] and for SU (3) in [17]). The model ensures a very good description of the phenomenology of hadron jets in high-energy e + − e − and p −p collision experiments (for further development of the basic model and phenomenological applications, see, e.g., review [18]).…”
Section: Introductionmentioning
confidence: 99%
“…The HE γ-rays interact with the low energy photons of the EBL via the pair-production process leaving an energy dependent attenuation signature in the spectra (Nikishov 1962;Gould & Schréder 1967). The strength of this attenuation and its spectral behavior depends on the properties of the EBL (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…Therefore physics in the presence of such ultra-strong fields is now coming upon a focus of attention. One of the most striking effects in this area is electron-positron pair creation from vacuum [5][6][7][8][9]. However, according to recent calculations [9], spontaneous pair creation from vacuum would require an optical laser of the power above 500 PW, still far from the experimental possibilities of the nearest future.…”
Section: Introductionmentioning
confidence: 99%