2014
DOI: 10.1017/s0263034613001043
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Numerical study of positron production with short-pulse high-intensity lasers

Abstract: One-dimensional particle-in-cell and Monte-Carlo (FLUKA) simulation methods were used together, in order to investigate the production of positrons in lead targets, illuminated by a short-pulse high-intensity laser. The study is focused on lead targets of 1 mm thickness and more and pulses of intensity in the range 1019–1022 W/cm2. The calculations provided an estimate of an absolute number of positrons and the ratio of electrons and positrons emerging from the target. The thickness of the target is scaled in … Show more

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Cited by 6 publications
(3 citation statements)
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“…Unlike methods used in Refs. [31][32][33], we will not separate the bremsstrahlung from the laser plasma interaction. To simulate the bremsstrahlung and nonlinear Compton scattering in the laser plasma interaction, MC method has been implemented in our 2D PIC code.…”
Section: B Simulation Methodsmentioning
confidence: 99%
“…Unlike methods used in Refs. [31][32][33], we will not separate the bremsstrahlung from the laser plasma interaction. To simulate the bremsstrahlung and nonlinear Compton scattering in the laser plasma interaction, MC method has been implemented in our 2D PIC code.…”
Section: B Simulation Methodsmentioning
confidence: 99%
“…the particle-in-cell (PIC) method. Such approach is appropriate for bulk targets and it has been applied in several studies [32][33][34][35]. However, for thinner targets and fast electron sources with very high current densities, collective effects during the electron transport may become important and even dominant, the assumption that the target is static and undisturbed may be violated due to its significant expansion, and electron refluxing cannot be neglected.…”
Section: Introductionmentioning
confidence: 99%
“…When an intense laser beam irradiates a solid target, relativistic electrons can be produced in front of the target through the direct-laser-heating/acceleration mechanism. These energetic electrons can propagate through the bulk solid and trigger abundant plasma-atomic processes, which typically include resistive return current, resistive electric and magnetic fields [21], bulk heating and ionization dynamics [22], Bremsstrahlung X-ray generation [23][24][25] and also ion accelerations [16][17][18][19][20].…”
Section: Introductionmentioning
confidence: 99%