2006
DOI: 10.1016/j.jcp.2006.01.039
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QUICKPIC: A highly efficient particle-in-cell code for modeling wakefield acceleration in plasmas

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Cited by 179 publications
(143 citation statements)
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“…Of particular relevance is the assessment of the role of the beam emittance for typical electron beams now available. Figure 5 3D PIC simulations using the quasistatic PIC code QUICKPIC [32] have been performed to examine in detail the spin precession and polarization dynamics in LWFA scenarios. To this purpose, a random sample of the externally injected electrons was tracked using a particletracking algorithm [36], which stored the trajectories and fields associated with the accelerated electron beam.…”
Section: Numerical Simulationsmentioning
confidence: 99%
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“…Of particular relevance is the assessment of the role of the beam emittance for typical electron beams now available. Figure 5 3D PIC simulations using the quasistatic PIC code QUICKPIC [32] have been performed to examine in detail the spin precession and polarization dynamics in LWFA scenarios. To this purpose, a random sample of the externally injected electrons was tracked using a particletracking algorithm [36], which stored the trajectories and fields associated with the accelerated electron beam.…”
Section: Numerical Simulationsmentioning
confidence: 99%
“…In order to identify the role of the beam emittance in more realistic scenarios, QUICKPIC [32] simulations using nonzero electron beam emittances were performed, using sim N ¼ 62:5 mm mrad (typical SLAC beam emittance) and keeping the rest of the laser, plasma, and beam parameters unchanged. For these values, Eq.…”
Section: Numerical Simulationsmentioning
confidence: 99%
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“…Using a fully self-consistent Particle-In-Cell (PIC) algorithm to simulate such a stage is still impractical with state of the art computing facilities. The use of reduced models [7,8,9] is therefore required to model acceleration of particle beams to these high energies as it can greatly reduce the required number of simulation hours. Here we use the fully self-consistent PIC algorithm, implemented in the code VORPAL [10], to simulate the evolution of an externally injected electron bunch over the accelerating stage by scaling the physical quantities with the plasma density.…”
Section: Scaling Lawsmentioning
confidence: 99%
“…While both plasma wavelength and total length of the plasma need to be increased as we wish to increase the beam energy gain, the laser wavelength stays fixed to 1 µm. Reduced models are used to overcome this issue, such as the Ponderomotive Guiding Center method [3,4,5,6,7] where the laser wavelength is not resolved and only the average ponderomotive force of the laser is modeled, and simulations in a boosted frame [8,9,10], where the simulation is done in a frame that moves at a relativistic velocity along with the laser pulse. Further challenge is to accurately simulate the electron beam properties as numerical noise accumulates in particle-in-cell simulations.…”
Section: Introductionmentioning
confidence: 99%