4.4 Article

Convective Raman amplification of light pulses causing kinetic inflation in inertial fusion plasmas

Journal

PHYSICS OF PLASMAS
Volume 19, Issue 11, Pages -

Publisher

AIP Publishing
DOI: 10.1063/1.4762853

Keywords

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Funding

  1. U.S. Department of Energy by Lawrence Livermore National Laboratory [DE-AC52-07NA27344]
  2. University of California, Los Angeles [FG52-09NA29552, DE-NA0001833]
  3. Laboratory Directed Research and Development Program at LLNL [08-ERD-017]
  4. Lawrence Scholar Program at LLNL

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We perform 1D particle-in-cell (PIC) simulations using OSIRIS, which model a short-duration (similar to 500 omega(-1)(0) FWHM) scattered light seed pulse in the presence of a constant counter-propagating pump laser with an intensity far below the absolute instability threshold. The seed undergoes linear convective Raman amplification and dominates over fluctuations due to particle discreteness. Our simulation results are in good agreement with results from a coupled-mode solver when we take into account special relativity and the use of finite size PIC simulation particles. We present linear gain spectra including both effects. Extending the PIC simulations past when the seed exits the simulation domain reveals bursts of large-amplitude scattering in many cases, which does not occur in simulations without the seed pulse. These bursts can have amplitudes several times greater than the amplified seed pulse, and we demonstrate that this large-amplitude scattering is the result of kinetic inflation by examining trapped particle orbits. This large-amplitude scattering is caused by the seed modifying the distribution function earlier in the simulation. We perform some simulations with longer duration seeds, which lead to parts of the seeds undergoing kinetic inflation and reaching amplitudes several times more than the steady-state linear theory results. Simulations with continuous seeds demonstrate that the onset of inflation depends on seed wavelength and incident intensity, and we observe oscillations in the reflectivity at a frequency equal to the difference between the seed frequency and the frequency at which the inflationary stimulated Raman scattering grows. (C) 2012 American Institute of Physics. [http://dx.doi.org/10.1063/1.4762853]

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