Fast electron generation using PW-class PEARL facility

Soloviev, A. A.; Burdonov, K.; Гинзбург, В. Н.; Gonoskov, Arkady; Katin, E. V.; Kim, A. V.; Kirsanov, A. V.; Korzhimanov, A. V.; Kostyukov, I. Yu.; Lozhkarev, V. V.; Luchinin, G. A.; Mal’shakov, A.N.; Martyanov, M. A.; Nerush, E. N.; Palashov, O.; Poteomkin, A.; Сергеев, А. М.; Shaykin, A. A.; Starodubtsev, M.; Yakovlev, I. V.; Zelenogorsky, V. V.; Хазанов, Е. А.

doi:10.1016/j.nima.2011.01.180

Cited by 24 publications

(15 citation statements)

References 15 publications

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“…The code ELMIS (Extreme Laser-Matter Interaction Simulator) is a fully parallelized, 3D/2D PIC implementation based on the spectral method for solving Maxwell's equations and an original parallel algorithm for fast Fourier transform [88]. First presented at [85] in 2009, ELMIS code [13] has been successfully applied to a number of studies in the field of laser-plasma interactions, including ion acceleration [89], laser wakefield acceleration [90,91] and higher harmonic generation at solids [17]. The code is based on an original spectral-rotational Maxwell solver (for more details see [13] Sect.…”

Section: B Elmis: a Parallel Pic Code Based On Dispersion-free Spectr...mentioning

confidence: 99%

Extended particle-in-cell schemes for physics in ultrastrong laser fields: Review and developments

Bastrakov²,

et al. 2015

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We review common extensions of particle-in-cell (PIC) schemes which account for strong field phenomena in laser-plasma interactions. After describing the physical processes of interest and their numerical implementation, we provide solutions for several associated methodological and algorithmic problems. We propose a modified event generator that precisely models the entire spectrum of incoherent particle emission without any low-energy cutoff, and which imposes close to the weakest possible demands on the numerical time step. Based on this, we also develop an adaptive event generator that subdivides the time step for locally resolving QED events, allowing for efficient simulation of cascades. Further, we present a new and unified technical interface for including the processes of interest in different PIC implementations. Two PIC codes which support this interface, PICADOR and ELMIS, are also briefly reviewed. CONTENTS

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Section: B Elmis: a Parallel Pic Code Based On Dispersion-free Spectr...mentioning

confidence: 99%

Extended particle-in-cell schemes for physics in ultrastrong laser fields: Review and developments

Bastrakov²,

et al. 2015

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“…The experiments were performed on a laboratory facility for studies of laser-plasma interaction [33,34] based on the PEARL laser complex [35]. The laser plasma was produced inside the magnetic system described in Sec.…”

Section: Setup Of the Experimentsmentioning

confidence: 99%

Experimental Study of the Interaction of a Laser Plasma Flow with a Transverse Magnetic Field

Soloviev

Burdonov

Котов

et al. 2021

Radiophys Quantum El

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We present the results of studying experimentally the expansion of laser plasma in a strong external magnetic field (with a magnetic flux density of 13.5 T) at various sizes of the region of plasma formation on the surface of a solid-state target. It is shown that when the size of the plasma formation region is smaller than the classical plasma braking radius, a nearly identical topology of plasma flows is observed, which is characterized by the formation of a thin plasma sheet directed along the external magnetic field. If the width of the plasma formation region is comparable with the classical plasma braking radius, an additional plasma sheet starts to be formed.

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“…Leading research groups are focused on improving the repetition rate and pulse quality instead of successfully generating PW-class pulses [3][4][5][6][9][10][11]. Applications of ultra-high-power lasers require extraordinarily high quality, and it is necessary to increase the repetition rate to use them practically [8,12].…”

Section: Thermal Birefringencementioning

confidence: 99%

“…Owing to features such as excellent thermal conductivity, high mechanical durability, and wide amplification bandwidth, Ti:sapphire is widely used as a medium for high-power chirped pulse amplification (CPA) technology [1,2]. Some researchers from RAL, SIOM, PEARL, Apollon Project, and APRI, ELI, J-KAREN, and Vulcan have previously generated several petawatt (PW) laser pulses and are targeting 10 PW or more [3][4][5][6][7][8][9][10][11]. A high-power laser can be used in applications such as laser-material interaction, particle acceleration, basic research about materials under extreme environments, and medical applications [12][13][14].…”

Section: Introductionmentioning

confidence: 99%

Modeling and Analysis of High-Power Ti:sapphire Laser Amplifiers–A Review

et al. 2019

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We have introduced several factors that can be useful for the modeling and analysis of high-power Ti:sapphire laser amplifiers. The amplification model includes the phase distortion effect caused by the atomic phase shift (APS) in gain medium and the thermal-induced phase distortion effect caused by the high-average-power amplification. We have provided an accurate amplification model for the development of ultra-high-intensity and high-average-power lasers.

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Fast electron generation using PW-class PEARL facility

Cited by 24 publications

References 15 publications

Extended particle-in-cell schemes for physics in ultrastrong laser fields: Review and developments

Extended particle-in-cell schemes for physics in ultrastrong laser fields: Review and developments

Experimental Study of the Interaction of a Laser Plasma Flow with a Transverse Magnetic Field

Modeling and Analysis of High-Power Ti:sapphire Laser Amplifiers–A Review

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