Physical Review Letters · 2012 · 36 citations · 22 references
Natural SciencesPhysicsNuclear PhysicsParticle PhysicsPlasma PhysicsAccelerator PhysicsLaser PhysicsLaser-plasma InteractionsPlasma SimulationPlasma WavesPlasma-surface InteractionsHigh-energy Particle AccelerationLaser-driven Ion AccelerationParticle Acceleration In PlasmasParticle-in-cell SimulationsRelativistic Plasma DynamicsRelativistic PlasmasSurface WavesUnderdense Plasma Interaction
The interaction of a high-energy relativistic laser pulse with an underdense plasma is studied by means of 3-dimensional particle in cell simulations and theoretical analysis. For powers above the threshold for channeling, the laser pulse propagates as a single mode in an electron-free channel during a time of the order of 1 picosecond. The steep laser front gives rise to the excitation of a surface wave along the sharp boundaries of the ion channel. The surface wave first traps electrons at the channel wall and preaccelerates them to relativistic energies. These particles then have enough energy to be further accelerated in a second stage through an interplay between the acceleration due to the betatron resonance and the acceleration caused by the longitudinal part of the surface wave electric field. It is necessary to introduce this two-stage process to explain the large number of high-energy electrons observed in the simulations.
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Ignition and high gain with ultrapowerful lasers*
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A. Pukhov, Z. M. Sheng, J. Meyer‐ter‐Vehn · Physics of Plasmas · 1999 · 695 citations
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