Abstract:It was shown for the first time that in a laboratory experiment a train of laser plasma clouds makes it possible to increase the length of the whistler waves generated in the power tube of a magnetized medium. The intensity of waves is orders of magnitude higher than the level achieved by known methods.
“…A possible scheme for maintaining the LPP uniformity and density over longer distances is the use of pulse shaping to produce a train of laser pulses separated in time 34,35 . If the pulses are spaced sufficiently close together, their velocity distributions will cause them to merge together to form a quasicontinuous LPP.…”
Section: Modeling Lpp Density Dispersionmentioning
The creation of a repeatable collisionless quasi-parallel shock in the laboratory would provide a valuable platform for experimental studies of space and astrophysical shocks. However, conducting such an experiment presents substantial challenges. Scaling the results of hybrid simulations of quasi-parallel shock formation to the laboratory highlights the experimentally demanding combination of dense, fast, and magnetized background and driver plasmas required. One possible driver for such experiments are high-energy laser-produced plasmas (LPPs). Preliminary experiments at the University of California Los Angeles have explored LPPs as drivers of quasi-parallel shocks by combining the Phoenix Laser Laboratory [Niemann et al. Journal of Instrumentation, 7, 2012] with the Large Plasma Device (LAPD) [Gekelman et al. Review of Scientific Instruments, 87, 2016]. Beam instabilities and waves characteristic of the early stages of shock formation are observed, but spatial dispersion of the laser-produced plasma prematurely terminates the process. This result is illustrated by experimental measurements and Monte-Carlo calculations of LPP density dispersion. The experimentally-validated Monte-Carlo model is then applied to evaluate several possible approaches to mitigating LPP dispersion in future experiments.
“…A possible scheme for maintaining the LPP uniformity and density over longer distances is the use of pulse shaping to produce a train of laser pulses separated in time 34,35 . If the pulses are spaced sufficiently close together, their velocity distributions will cause them to merge together to form a quasicontinuous LPP.…”
Section: Modeling Lpp Density Dispersionmentioning
The creation of a repeatable collisionless quasi-parallel shock in the laboratory would provide a valuable platform for experimental studies of space and astrophysical shocks. However, conducting such an experiment presents substantial challenges. Scaling the results of hybrid simulations of quasi-parallel shock formation to the laboratory highlights the experimentally demanding combination of dense, fast, and magnetized background and driver plasmas required. One possible driver for such experiments are high-energy laser-produced plasmas (LPPs). Preliminary experiments at the University of California Los Angeles have explored LPPs as drivers of quasi-parallel shocks by combining the Phoenix Laser Laboratory [Niemann et al. Journal of Instrumentation, 7, 2012] with the Large Plasma Device (LAPD) [Gekelman et al. Review of Scientific Instruments, 87, 2016]. Beam instabilities and waves characteristic of the early stages of shock formation are observed, but spatial dispersion of the laser-produced plasma prematurely terminates the process. This result is illustrated by experimental measurements and Monte-Carlo calculations of LPP density dispersion. The experimentally-validated Monte-Carlo model is then applied to evaluate several possible approaches to mitigating LPP dispersion in future experiments.
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