Abstract

Fast electron transport has been studied in cold solid density CH, cold CH foam ($200\phantom{\rule{0.28em}{0ex}}\mathrm{mg}/{\mathrm{cm}}^{3}$), and CH plasma (40 eV $30\phantom{\rule{0.28em}{0ex}}\mathrm{mg}/{\mathrm{cm}}^{3}$) targets---the latter created by shocking the CH foam with a 1.2 kJ long pulse laser and allowing it to expand. The fast electrons were produced using the OMEGA EP laser pulse (800 J, 8 ps) incident on a Au flat target. With the CH plasma, the fluence of fast electrons reaching a Cu foil at the far side of the transport was reduced significantly ($25\ifmmode\times\else\texttimes\fi{}$ weaker peak $K\ensuremath{\alpha}$ emission). Particle-in-cell simulations using the osiris code modeled fast electron transport in the unshocked foam and plasma cases assuming fixed ionization and including source generation, transport in Au and CH layers, Coulomb collisions, and refluxing. Simulations indicate two main mechanisms which alter electron energy transport through the target between the foam and plasma cases, both due to the magnetic field: a collimating field in the CH region, caused by the resistivity of the return current and more prevalent in the foam; and an insulating field at the Au-CH interface, present only with the plasma.

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