Laser Amplification in Strongly-Magnetized Plasma
arXiv:1812.09429 · doi:10.1103/PhysRevLett.123.025001
Abstract
We consider backscattering of laser pulses in strongly-magnetized plasma mediated by kinetic magnetohydrodynamic waves. Magnetized low-frequency scattering, which can occur when the external magnetic field is neither perpendicular nor parallel to the laser propagation direction, provides an instability growth rate higher than Raman scattering and a frequency downshift comparable to Brillouin scattering. In addition to the high growth rate, which allows smaller plasmas, and the 0.1-2\% frequency downshift, which permits a wide range of pump sources, MLF scattering is an ideal candidate for amplification because the process supports an extremely large bandwidth, which particle-in-cell simulations show produces ultrashort durations. Under some conditions, MLF scattering also becomes the dominant spontaneous backscatter instability, with implications for magnetized laser-confinement experiments.
7 pages, 4 figures
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Cited by in corpus (9)
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- Magnetized Laser-Plasma Interactions in High-Energy-Density Systems: Parallel Propagation
- Modulation-Slippage Tradeoff in Resonant Four-Wave Upconversion
- Enhanced strong-coupling stimulated Brillouin amplification assisted by Raman amplification
- Enhanced collisionless laser absorption in strongly magnetized plasmas
- Phase-Matched Harmonic Generation in Strongly Magnetized Plasma
- Pushing the Frontiers of Light: Magnetized Plasma Lenses and Chirp Tailoring for Extreme Intensities