2010
DOI: 10.1016/j.physletb.2010.07.044
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Finite size effects in stimulated laser pair production

Abstract: We consider stimulated pair production employing strong-field QED in a high-intensity laser background. In an infinite plane wave, we show that light-cone quasi-momentum can only be transferred to the created pair as a multiple of the laser frequency, i.e.\ by a higher harmonic. This translates into discrete resonance conditions providing the support of the pair creation probability which becomes a delta-comb. These findings corroborate the usual interpretation of multi-photon production of pairs with an effec… Show more

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Cited by 176 publications
(199 citation statements)
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“…In particular, one may study the effects of the laser induced mass shift [32,33] without having to worry about contaminations due to discretisation errors. This requires an appropriate (possibly numerical) definition for proper time averages in pulses to continue the study of finite size effects on processes such as nonlinear Thomson/Compton scattering [34,35] or laser induced pair production [36].…”
Section: Discussionmentioning
confidence: 99%
“…In particular, one may study the effects of the laser induced mass shift [32,33] without having to worry about contaminations due to discretisation errors. This requires an appropriate (possibly numerical) definition for proper time averages in pulses to continue the study of finite size effects on processes such as nonlinear Thomson/Compton scattering [34,35] or laser induced pair production [36].…”
Section: Discussionmentioning
confidence: 99%
“…3 we compare (41) with the exact polarisation flip probability (40). For our plots, here and in subsequent examples, we use the following background field profile:…”
Section: A Helicity Flip: Behaviour As a Function Of Energymentioning
confidence: 99%
“…see Bulanov et al (2015) and literature cited therein). These effects manifest themselves through multi-photon Compton and Breit-Wheeler effects (Nikishov & Ritus 1964a,b;Ritus 1985) (see Narozhnyi & Fofanov (1996), Boca & Florescu (2009), Ehlotzky, Krajewska & Kamiśki (2009), Heinzl, Ilderton & Marklund (2010a), Heinzl, Seipt & Kämpfer (2010b, Mackenroth & Di Piazza (2011), Krajewska & Kamiński (2012), Titov et al (2012), Harvey, Heinzl & Ilderton (2009) for recent studies), i.e. through either photon emission by an electron or positron, or electron-positron pair production by a high energy photon, respectively.…”
Section: S V Bulanov and Othersmentioning
confidence: 99%